Let $$\overrightarrow{a}=-\widehat{i}+2\widehat{j}+2\widehat{k},\overrightarrow{b}=8\widehat{i}+7\widehat{j}-3\widehat{k} \text { and } \overrightarrow{c}$$ be a vector such that $$\overrightarrow{a}\times\overrightarrow{c}=\overrightarrow{b}$$. If $$\overrightarrow{c}\cdot(\widehat{i}+\widehat{j}+\widehat{k})=4$$, then $$\mid\overrightarrow{a}+\overrightarrow{c}\mid^{2}$$ is equal to :
JEE Vector Algebra Questions
JEE Vector Algebra Questions
Let $$\vec{c} = (x, y, z)$$. Since $$\vec{c} \cdot (1,1,1) = 4$$, it follows that $$x + y + z = 4$$.
$$\vec{a} \times \vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & 2 & 2 \\ x & y & z \end{vmatrix} = (2z - 2y,\; 2x + z,\; -y - 2x)$$ and equating to $$(8,7,-3)$$ gives $$2z - 2y = 8,\quad 2x + z = 7,\quad -y - 2x = -3,$$ or equivalently $$z - y = 4,\quad 2x + z = 7,\quad 2x + y = 3.$$
From $$x + y + z = 4$$, the second equation gives $$z = 7 - 2x$$ and the third gives $$y = 3 - 2x$$.
Substituting into $$x + y + z = 4$$ yields $$x + (3 - 2x) + (7 - 2x) = 4 \;\Longrightarrow\; -3x + 10 = 4 \;\Longrightarrow\; x = 2,$$ hence $$y = 3 - 2(2) = -1$$ and $$z = 7 - 2(2) = 3$$. Thus $$\vec{c} = (2, -1, 3)$$.
$$\vec{a} + \vec{c} = (-1 + 2,\; 2 - 1,\; 2 + 3) = (1,1,5),$$ so $$|\vec{a}+\vec{c}|^2 = 1^2 + 1^2 + 5^2 = 27.$$ The answer is Option 3: 27.
Let $$\overrightarrow{c} \text{ and } \overrightarrow{d}$$ be vectors such that $$\mid\overrightarrow{c}+\overrightarrow{d}\mid=\sqrt{29}$$ and $$\overrightarrow{c}\times( 2\widehat{i}+3\widehat{j}+4\widehat{k})=(2\widehat{i}+3\widehat{j}+4\widehat{k})\times\overrightarrow{d}$$. If $$\lambda_{1}, \lambda_{2}( \lambda_{1}> \lambda_{2})$$ are the possible values of $$(\overrightarrow{c}+\overrightarrow{d})\cdot(-7\widehat{i}+2\widehat{j}+3\overrightarrow{k})$$, then the equation $$K^{2}x^{2}+(K^{2}-5K+\lambda_{1})xy+\left(3K+\frac{\lambda_{2}}{2} \right)y^{2}-8x+12y+\lambda_{2}=0$$ represents a circle, for K equal to :
From the equation $$\vec{c} \times (2\hat{i}+3\hat{j}+4\hat{k}) = (2\hat{i}+3\hat{j}+4\hat{k}) \times \vec{d}$$,
let $$\vec{e} = 2\hat{i}+3\hat{j}+4\hat{k}$$ so that it becomes $$\vec{c} \times \vec{e} = \vec{e} \times \vec{d}$$. Since $$\vec{e} \times \vec{d} = -\vec{d} \times \vec{e}$$, we have $$\vec{c} \times \vec{e} + \vec{d} \times \vec{e} = \vec{0}$$, implying $$(\vec{c} + \vec{d}) \times \vec{e} = \vec{0}$$.
Hence, $$\vec{c} + \vec{d}$$ is parallel to $$\vec{e}$$ and can be written as $$\vec{c} + \vec{d} = \lambda\vec{e}$$ for some scalar $$\lambda$$.
Using the condition $$|\vec{c} + \vec{d}| = \sqrt{29}$$, we get $$|\lambda \vec{e}| = |\lambda|\sqrt{4 + 9 + 16} = |\lambda|\sqrt{29} = \sqrt{29}$$, which gives $$|\lambda| = 1\implies \lambda = \pm1$$.
find $$(\vec{c} + \vec{d}) \cdot (-7\hat{i}+2\hat{j}+3\hat{k})$$, substitute $$\vec{c} + \vec{d} = \lambda\vec{e}$$: $$\lambda\vec{e} \cdot (-7\hat{i}+2\hat{j}+3\hat{k}) = \lambda[2(-7) + 3(2) + 4(3)] = 4\lambda$$.
For $$\lambda = 1$$, the value is 4, and for $$\lambda = -1$$ it is -4. Since $$\lambda_1 > \lambda_2$$, we take $$\lambda_1 = 4$$ and $$\lambda_2 = -4$$.
$$K^2x^2 + (K^2 - 5K + \lambda_1)xy + (3K + \frac{\lambda_2}{2})y^2 - 8x + 12y + \lambda_2 = 0$$ and substitute $$\lambda_1 = 4$$ and $$\lambda_2 = -4$$ to obtain $$K^2x^2 + (K^2 - 5K + 4)xy + (3K - 2)y^2 - 8x + 12y - 4 = 0$$.
For a general second-degree equation $$ax^2 + 2hxy + by^2 + 2gx + 2fy + c = 0$$ to represent a circle, the coefficient of $$x^2$$ must equal that of $$y^2$$ (so $$a=b$$) and the coefficient of $$xy$$ must be zero (so $$h=0$$).
Equating the coefficients gives two conditions: $$K^2 = 3K - 2$$ and $$K^2 - 5K + 4 = 0$$. The first yields $$K^2 - 3K + 2 = 0\implies (K-1)(K-2) = 0$$, so $$K = 1$$ or $$2$$. The second gives $$(K-1)(K-4) = 0$$, so $$K = 1$$ or $$4$$.
The only value of $$K$$ satisfying both conditions is $$K = 1$$. Therefore, the correct answer is Option (3): 1.
For three unit vectors $$\overrightarrow{a},\overrightarrow{b},\overrightarrow{c}$$ satisfying $$|\overrightarrow{a}-\overrightarrow{b}|^{2}+|\overrightarrow{b}-\overrightarrow{c}|^{2}+|\overrightarrow{c}-\overrightarrow{a}|^{2}=9$$ and $$|2\overrightarrow{a}+k\overrightarrow{b}+k\overrightarrow{c}|+3$$. the positive value of k is
Three unit vectors $$\vec{a}, \vec{b}, \vec{c}$$ satisfy $$|\vec{a} - \vec{b}|^2 + |\vec{b} - \vec{c}|^2 + |\vec{c} - \vec{a}|^2 = 9$$. We seek the positive value of $$k$$ such that $$|2\vec{a} + k\vec{b} + k\vec{c}| = 3$$.
Expanding each squared difference gives $$|\vec{a} - \vec{b}|^2 = |\vec{a}|^2 - 2\vec{a} \cdot \vec{b} + |\vec{b}|^2 = 2 - 2\vec{a} \cdot \vec{b}$$, and similarly for the other pairs. Summing these three expressions yields $$6 - 2(\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{c} + \vec{c} \cdot \vec{a}) = 9$$, so $$\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{c} + \vec{c} \cdot \vec{a} = -\frac{3}{2}$$.
Next, observe that $$|\vec{a} + \vec{b} + \vec{c}|^2 = |\vec{a}|^2 + |\vec{b}|^2 + |\vec{c}|^2 + 2(\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{c} + \vec{c} \cdot \vec{a}) = 3 + 2\left(-\frac{3}{2}\right) = 0$$. Hence $$\vec{a} + \vec{b} + \vec{c} = \vec{0}$$, which implies $$\vec{b} + \vec{c} = -\vec{a}$$.
Using this result, one finds $$|2\vec{a} + k\vec{b} + k\vec{c}|^2 = |2\vec{a} + k(\vec{b} + \vec{c})|^2 = |2\vec{a} - k\vec{a}|^2 = (2 - k)^2|\vec{a}|^2 = (2 - k)^2$$. Therefore $$|2\vec{a} + k\vec{b} + k\vec{c}| = |2 - k|$$.
Setting this equal to 3 gives $$|2 - k| = 3$$, so $$2 - k = 3\implies k = -1$$ or $$2 - k = -3\implies k = 5$$. The positive value is $$k = 5$$.
Final answer: The required positive value of $$k$$ is 5.
If $$\vec{a}$$ and $$\vec{b}$$ are two vectors such that $$|\vec{a}| = 2$$ and $$|\vec{b}| = 3$$, then the maximum value of $$3|3\vec{a} + 2\vec{b}| + 4|3\vec{a} - 2\vec{b}|$$ is :
Let the angle between $$\vec{a}$$ and $$\vec{b}$$ be $$\theta$$. We have $$|\vec{a}| = 2$$, $$|\vec{b}| = 3$$, so $$\vec{a} \cdot \vec{b} = 6\cos\theta$$.
Computing the magnitudes:
$$|3\vec{a} + 2\vec{b}|^2 = 9(4) + 12(6\cos\theta) + 4(9) = 72 + 72\cos\theta = 144\cos^2\frac{\theta}{2}$$
So $$|3\vec{a} + 2\vec{b}| = 12\left|\cos\frac{\theta}{2}\right|$$.
$$|3\vec{a} - 2\vec{b}|^2 = 9(4) - 12(6\cos\theta) + 4(9) = 72 - 72\cos\theta = 144\sin^2\frac{\theta}{2}$$
So $$|3\vec{a} - 2\vec{b}| = 12\left|\sin\frac{\theta}{2}\right|$$.
The expression becomes (taking $$\theta \in [0, \pi]$$ so that $$\cos(\theta/2) \geq 0$$ and $$\sin(\theta/2) \geq 0$$):
$$3|3\vec{a} + 2\vec{b}| + 4|3\vec{a} - 2\vec{b}| = 36\cos\frac{\theta}{2} + 48\sin\frac{\theta}{2}$$
This is of the form $$A\cos\phi + B\sin\phi$$, whose maximum value is $$\sqrt{A^2 + B^2}$$:
$$\sqrt{36^2 + 48^2} = \sqrt{1296 + 2304} = \sqrt{3600} = 60$$
Hence, the correct answer is Option 3.
Let the vectors $$\vec{a} = -\hat{i} + \hat{j} + 3\hat{k}$$ and $$\vec{b} = \hat{i} + 3\hat{j} + \hat{k}$$. For some $$\lambda, \mu \in \mathbb{R}$$, let $$\vec{c} = \lambda\vec{a} + \mu\vec{b}$$. If $$\vec{c} \cdot (3\hat{i} - 6\hat{j} + 2\hat{k}) = 10$$ and $$\vec{c} \cdot (\hat{i} + \hat{j} + \hat{k}) = -2$$, then $$|\vec{c}|^2$$ is equal to :
The given vectors are
$$\vec{a}= -\hat{i}+ \hat{j}+ 3\hat{k},\qquad
\vec{b}= \hat{i}+ 3\hat{j}+ \hat{k}.$$
Let $$\vec{c}= \lambda\vec{a}+ \mu\vec{b}$$ where $$\lambda,\mu\in\mathbb{R}.$$
First write $$\vec{c}$$ in component form:
$$\vec{c}= \lambda(-1,1,3)+ \mu(1,3,1)=(-\lambda+\mu,\; \lambda+3\mu,\; 3\lambda+\mu).$$
The two scalar-product conditions are
1. $$\vec{c}\cdot(3\hat{i}-6\hat{j}+2\hat{k})=10,$$
2. $$\vec{c}\cdot(\hat{i}+ \hat{j}+ \hat{k})=-2.$$
Condition 1:
$$(-\lambda+\mu,\; \lambda+3\mu,\; 3\lambda+\mu)\cdot(3,-6,2)=10.$$
Compute the dot product:
$$3(-\lambda+\mu)+(-6)(\lambda+3\mu)+2(3\lambda+\mu)=10.$$
$$(-3\lambda+3\mu)\;+\;(-6\lambda-18\mu)\;+\;(6\lambda+2\mu)=10.$$
Combine like terms:
$$(-3\lambda-6\lambda+6\lambda)+ (3\mu-18\mu+2\mu)=10 \implies -3\lambda-13\mu=10.$$
$$\Rightarrow\quad -(3\lambda+13\mu)=10 \quad -(1)$$
Condition 2:
$$(-\lambda+\mu,\; \lambda+3\mu,\; 3\lambda+\mu)\cdot(1,1,1)=-2.$$
Compute the dot product:
$$(-\lambda+\mu)+(\lambda+3\mu)+(3\lambda+\mu)=-2.$$
Simplify:
$$(-\lambda+\lambda+3\lambda)+( \mu+3\mu+\mu)=-2 \implies 3\lambda+5\mu=-2 \quad -(2)$$
We now have the simultaneous linear equations
$$-3\lambda-13\mu=10 \quad -(1)$$
$$\;\;3\lambda+5\mu=-2 \quad\;\, -(2)$$
Add equations $$(1)+(2):$$
$$(-3\lambda+3\lambda)+(-13\mu+5\mu)=10-2 \implies -8\mu=8 \implies \mu=-1.$$
Substitute $$\mu=-1$$ in $$(2):$$
$$3\lambda+5(-1)=-2 \implies 3\lambda-5=-2 \implies 3\lambda=3 \implies \lambda=1.$$
Hence $$\lambda=1,\quad \mu=-1.$$
Therefore
$$\vec{c}=1\cdot\vec{a}+(-1)\cdot\vec{b}= \vec{a}-\vec{b}.$$
Compute $$\vec{c}$$ explicitly:
$$\vec{c}=(-1,1,3)-(1,3,1)=(-2,-2,2).$$
The square of its magnitude is
$$|\vec{c}|^{2}=(-2)^{2}+(-2)^{2}+2^{2}=4+4+4=12.$$
Hence, $$|\vec{c}|^{2}=12.$$
Option B which is: $$12$$
Let $$\vec{a} = 4\hat{i} - \hat{j} + 3\hat{k}$$, $$\vec{b} = 10\hat{i} + 2\hat{j} - \hat{k}$$ and a vector $$\vec{c}$$ be such that $$2(\vec{a} \times \vec{b}) + 3(\vec{b} \times \vec{c}) = \vec{0}$$. If $$\vec{a} \cdot \vec{c} = 15$$, then $$\vec{c} \cdot (\hat{i} + \hat{j} - 3\hat{k})$$ is equal to :
To solve this efficiently, we use the properties of vector cross products.
Given: $$2(\vec{a} \times \vec{b}) + 3(\vec{b} \times \vec{c}) = \vec{0}$$
Rearrange: $$3(\vec{b} \times \vec{c}) = -2(\vec{a} \times \vec{b})$$
Using the property $$\vec{u} \times \vec{v} = -(\vec{v} \times \vec{u})$$, we get:
$$3(\vec{b} \times \vec{c}) = 2(\vec{b} \times \vec{a})$$
$$\vec{b} \times 3\vec{c} = \vec{b} \times 2\vec{a}$$
This implies that $$3\vec{c} - 2\vec{a}$$ is parallel to $$\vec{b}$$:
$$3\vec{c} = 2\vec{a} + \lambda\vec{b}$$
$$\vec{c} = \frac{2\vec{a} + \lambda\vec{b}}{3}$$
Use the condition $$\vec{a} \cdot \vec{c} = 15$$:
$$\vec{a} \cdot \left( \frac{2\vec{a} + \lambda\vec{b}}{3} \right) = 15$$
$$2|\vec{a}|^2 + \lambda(\vec{a} \cdot \vec{b}) = 45$$
- $$|\vec{a}|^2 = 4^2 + (-1)^2 + 3^2 = 16 + 1 + 9 = 26$$
- $$\vec{a} \cdot \vec{b} = (4)(10) + (-1)(2) + (3)(-1) = 40 - 2 - 3 = 35$$
- $$\vec{a} \cdot \vec{d} = (4)(1) + (-1)(1) + (3)(-3) = 4 - 1 - 9 = -6$$
- $$\vec{b} \cdot \vec{d} = (10)(1) + (2)(1) + (-1)(-3) = 10 + 2 + 3 = 15$$
Substitute:
$$2(26) + \lambda(35) = 45$$
$$52 + 35\lambda = 45$$
$$35\lambda = -7 \implies \lambda = -\frac{1}{5}$$
We need $$\vec{c} \cdot \vec{d}$$ where $$\vec{d} = \hat{i} + \hat{j} - 3\hat{k}$$.
$$\vec{c} \cdot \vec{d} = \frac{2(\vec{a} \cdot \vec{d}) + \lambda(\vec{b} \cdot \vec{d})}{3}$$
$$\vec{c} \cdot \vec{d} = \frac{2(-6) + (-\frac{1}{5})(15)}{3}$$
$$\vec{c} \cdot \vec{d} = \frac{-12 - 3}{3} = \frac{-15}{3} = -5$$
Correct Answer: B (-5)
Let $$\vec{a} = \sqrt{7}\hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = \hat{j} + 2\hat{k}$$. If $$\vec{r}$$ is a vector such that $$\vec{r} \times \vec{a} + \vec{a} \times \vec{b} = \vec{0}$$ and $$\vec{r} \cdot \vec{a} = 0$$, then $$|3\vec{r}|^2$$ is equal to :
Let $$\hat{u}$$ and $$\hat{v}$$ be unit vectors inclined at acute angle such that $$|\hat{u} \times \hat{v}| = \frac{\sqrt{3}}{2}$$. If $$\vec{A} = \lambda\hat{u} + \hat{v} + (\hat{u} \times \hat{v})$$, then $$\lambda$$ is equal to :
Since $$\hat u,\;\hat v$$ are unit vectors, let the angle between them be $$\theta$$.
Given $$\left|\hat u \times \hat v\right| = \sin\theta = \frac{\sqrt3}{2} \; \Longrightarrow \; \theta = 60^{\circ}\;(\text{i.e. } \cos\theta = \tfrac12).$$
The vector in the question is
$$\vec A = \lambda\,\hat u + \hat v + (\hat u \times \hat v).$$
Take the dot product of $$\vec A$$ with $$\hat u$$:
$$\vec A \cdot \hat u = \lambda(\hat u \cdot \hat u) + (\hat v \cdot \hat u) + \bigl(\hat u \times \hat v\bigr)\cdot\hat u.$$
Here $$\hat u \cdot \hat u = 1,$$ $$\hat v \cdot \hat u = \cos\theta = \tfrac12,$$ and $$\bigl(\hat u \times \hat v\bigr)\cdot\hat u = 0$$ because the cross-product is perpendicular to both $$\hat u$$ and $$\hat v$$. Hence
$$\vec A \cdot \hat u = \lambda + \tfrac12 \quad -(1).$$
Next, dot $$\vec A$$ with $$\hat v$$:
$$\vec A \cdot \hat v = \lambda(\hat u \cdot \hat v) + (\hat v \cdot \hat v) + \bigl(\hat u \times \hat v\bigr)\cdot\hat v,$$
giving $$\vec A \cdot \hat v = \lambda\!\left(\tfrac12\right) + 1 + 0 = \tfrac12\lambda + 1 \quad -(2).$$
Denote $$\vec A \cdot \hat u = P$$ and $$\vec A \cdot \hat v = Q.$$
From $$(1):\; P = \lambda + \tfrac12 \;\Longrightarrow\; \lambda = P - \tfrac12 \quad -(3).$$
From $$(2):\; Q = \tfrac12\lambda + 1.$$ Substitute $$\lambda$$ from $$(3):$$
$$Q = \tfrac12(P - \tfrac12) + 1 = \tfrac12P - \tfrac14 + 1 = \tfrac12P + \tfrac34 \quad -(4).$$
We now express $$\lambda$$ as a linear combination of $$P$$ and $$Q$$.
Multiply $$(4)$$ by $$-\tfrac23$$ and add to $$\tfrac43 P$$:
$$\tfrac43 P - \tfrac23 Q = \tfrac43 P - \tfrac23\!\left(\tfrac12P + \tfrac34\right) = \tfrac43 P - \tfrac13 P - \tfrac12 = P - \tfrac12.$$
Using $$(3),$$ $$P - \tfrac12 = \lambda.$$ Therefore
$$\boxed{\lambda = \tfrac43(\vec A \cdot \hat u) - \tfrac23(\vec A \cdot \hat v)}.$$
This matches Option A.
Let $$\vec{a} = 2\hat{i} + 3\hat{j} + 3\hat{k}$$ and $$\vec{b} = 6\hat{i} + 3\hat{j} + 3\hat{k}$$. Then the square of the area of the triangle with adjacent sides determined by the vectors $$(2\vec{a} + 3\vec{b})$$ and $$(\vec{a} - \vec{b})$$ is :
Let $$O$$ be the origin, $$\overrightarrow{OP} = \vec{a}$$ and $$\overrightarrow{OQ} = \vec{b}$$.If $$R$$ is the point on $$\overrightarrow{OP}$$ such that $$\overrightarrow{OP} = 5\overrightarrow{OR}$$,and $$M$$ is the point such that $$\overrightarrow{OQ} = 5\overrightarrow{RM}$$. Then $$\overrightarrow{PM}$$ is equal to :
Let $$\overrightarrow{a},\overrightarrow{b},\overrightarrow{c}$$ be three vectors such that $$\overrightarrow{a}\times\overrightarrow{b}=2(\overrightarrow{a}\times\overrightarrow{c}).$$ If $$ \mid \overrightarrow{a}\mid, \mid\overrightarrow{b}\mid = 4, \mid \overrightarrow{c}\mid = 2,$$ and the angle between $$\overrightarrow{b}$$ and $$\overrightarrow{c}$$ is $$60^{o}$$, then $$\mid\overrightarrow{a}\cdot\overrightarrow{c}$$ is
We are given three vectors $$\overrightarrow{a}, \overrightarrow{b}, \overrightarrow{c}$$ such that $$\overrightarrow{a} \times \overrightarrow{b} = 2(\overrightarrow{a} \times \overrightarrow{c})$$, with $$|\overrightarrow{a}| = |\overrightarrow{b}| = 4$$, $$|\overrightarrow{c}| = 2$$, and the angle between $$\overrightarrow{b}$$ and $$\overrightarrow{c}$$ is $$60°$$.
Since $$\overrightarrow{a} \times \overrightarrow{b} = 2(\overrightarrow{a} \times \overrightarrow{c})$$, it follows that $$\overrightarrow{a} \times \overrightarrow{b} - 2(\overrightarrow{a} \times \overrightarrow{c}) = \overrightarrow{0}$$ and hence $$\overrightarrow{a} \times (\overrightarrow{b} - 2\overrightarrow{c}) = \overrightarrow{0}$$. This implies that $$\overrightarrow{a}$$ is parallel to $$(\overrightarrow{b} - 2\overrightarrow{c})$$, so one can write $$(\overrightarrow{b} - 2\overrightarrow{c}) = \lambda\,\overrightarrow{a}$$ for some scalar $$\lambda$$.
Taking magnitudes squared of both sides gives $$|\overrightarrow{b} - 2\overrightarrow{c}|^2 = \lambda^2 |\overrightarrow{a}|^2$$, which expands to $$|\overrightarrow{b}|^2 - 4\,\overrightarrow{b}\cdot\overrightarrow{c} + 4|\overrightarrow{c}|^2 = 16\lambda^2$$. Now $$\overrightarrow{b}\cdot\overrightarrow{c} = |\overrightarrow{b}|\,|\overrightarrow{c}|\cos 60° = 4 \times 2 \times \tfrac12 = 4$$, so this becomes $$16 - 16 + 16 = 16\lambda^2 \implies \lambda^2 = 1 \implies \lambda = \pm 1$$.
Next, taking the dot product with $$\overrightarrow{c}$$ in $$(\overrightarrow{b} - 2\overrightarrow{c}) = \lambda\,\overrightarrow{a}$$ yields $$\overrightarrow{a}\cdot\overrightarrow{c} = \frac{(\overrightarrow{b} - 2\overrightarrow{c})\cdot\overrightarrow{c}}{\lambda} = \frac{\overrightarrow{b}\cdot\overrightarrow{c} - 2|\overrightarrow{c}|^2}{\lambda} = \frac{4 - 8}{\lambda} = \frac{-4}{\lambda}$$. When $$\lambda = 1$$, $$\overrightarrow{a}\cdot\overrightarrow{c} = -4$$ and thus $$|\overrightarrow{a}\cdot\overrightarrow{c}| = 4$$; similarly, when $$\lambda = -1$$, $$\overrightarrow{a}\cdot\overrightarrow{c} = 4$$ so again $$|\overrightarrow{a}\cdot\overrightarrow{c}| = 4$$.
The correct answer is Option A: 4.
Let $$\overrightarrow{r}=2\widehat{i}+\widehat{j}-2\widehat{k}, \overrightarrow{b}=\widehat{i}+\widehat{j}\text{ and }\overrightarrow{c}=\overrightarrow{a}\times \overrightarrow{b}$$. Let $$\overrightarrow{d}$$ be a vector such that $$|\overrightarrow{d}-\overrightarrow{a}|=\sqrt{11},|\overrightarrow{c}\times \overrightarrow{d}|=3$$ and the angle between $$\overrightarrow{c}\text{ and }\overrightarrow{d}$$ is $$\frac{\pi}{4}$$. Then $$\overrightarrow{a}. \overrightarrow{d}$$ is equal to
Consider the vectors $$\vec{a} = 2\hat{i} + \hat{j} - 2\hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j}$$, with $$\vec{c} = \vec{a} \times \vec{b}$$. It is also given that $$|\vec{d} - \vec{a}| = \sqrt{11}$$, $$|\vec{c} \times \vec{d}| = 3$$, and the angle between $$\vec{c}$$ and $$\vec{d}$$ is $$\frac{\pi}{4}$$.
First, computing the cross product yields $$\vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 1 & -2 \\ 1 & 1 & 0 \end{vmatrix} = \hat{i}(0+2) - \hat{j}(0+2) + \hat{k}(2-1) = 2\hat{i} - 2\hat{j} + \hat{k}$$, and therefore $$|\vec{c}| = \sqrt{4+4+1} = 3$$.
Since $$|\vec{c} \times \vec{d}| = |\vec{c}||\vec{d}|\sin\theta$$ we have $$3\cdot|\vec{d}|\cdot\sin\frac{\pi}{4} = 3$$, implying $$|\vec{d}|\cdot\frac{1}{\sqrt{2}} = 1$$ and hence $$|\vec{d}| = \sqrt{2}$$.
Similarly, the dot product is given by $$\vec{c} \cdot \vec{d} = |\vec{c}||\vec{d}|\cos\frac{\pi}{4} = 3\cdot\sqrt{2}\cdot\frac{1}{\sqrt{2}} = 3$$.
Using $$|\vec{d} - \vec{a}|^2 = |\vec{d}|^2 - 2\vec{a}\cdot\vec{d} + |\vec{a}|^2 = 11$$ and noting $$|\vec{a}| = \sqrt{4+1+4} = 3$$ so that $$|\vec{a}|^2 = 9$$, we substitute to obtain $$2 - 2(\vec{a}\cdot\vec{d}) + 9 = 11$$, which leads to $$\vec{a}\cdot\vec{d} = \frac{11 - 9 - 2}{-2} = 0$$.
Therefore $$\vec{a} \cdot \vec{d} = 0$$, which corresponds to Option 2.
Two adjacent sides of a parallelogram $$PQRS$$ are given by $$\vec{PQ} = \hat{j} + \hat{k}$$ and $$\vec{PS} = \hat{i} - \hat{j}$$. If the side $$PS$$ is rotated about the point $$P$$ by an acute angle $$\alpha$$ in the plane of the parallelogram so that it becomes perpendicular to the side $$PQ$$, then $$\sin^2\left(\frac{5\alpha}{2}\right) - \sin^2\left(\frac{\alpha}{2}\right)$$ is equal to :
The given adjacent sides of parallelogram $$PQRS$$ are
$$\vec{PQ}= \hat{j}+\hat{k}, \qquad \vec{PS}= \hat{i}-\hat{j}.$$
First, find the angle $$\theta$$ between $$\vec{PQ}$$ and $$\vec{PS}$$.
Using the dot-product formula $$\vec{a}\cdot\vec{b}=|\vec{a}|\,|\vec{b}|\cos\theta$$,
$$\vec{PQ}\cdot\vec{PS}= (0,1,1)\cdot(1,-1,0) = 0\cdot1 + 1\cdot(-1) + 1\cdot0 = -1.$$
Magnitudes:
$$|\vec{PQ}| = \sqrt{0^2+1^2+1^2}= \sqrt2, \qquad |\vec{PS}| = \sqrt{1^2+(-1)^2+0^2}= \sqrt2.$$
Therefore,
$$\cos\theta = \frac{-1}{|\vec{PQ}|\,|\vec{PS}|}= \frac{-1}{(\sqrt2)(\sqrt2)}= -\frac12.$$
So $$\theta = 120^{\circ}\;(=\frac{2\pi}{3}).$$
The side $$PS$$ is rotated in the plane of the parallelogram through an acute angle $$\alpha$$ to a new position (call it $$PT$$) such that $$PT \perp PQ$$. Hence the new angle between $$PQ$$ and $$PT$$ must be $$90^{\circ}$$.
Since the original angle is $$120^{\circ}$$ and we need $$90^{\circ}$$, the amount of rotation is
$$\alpha = 120^{\circ}-90^{\circ}=30^{\circ}\;(=\frac{\pi}{6}),$$
which is indeed acute.
Now evaluate $$\sin^2\!\left(\frac{5\alpha}{2}\right) - \sin^2\!\left(\frac{\alpha}{2}\right).$$
Compute half-angles:
$$\frac{\alpha}{2}= \frac{30^{\circ}}{2}=15^{\circ}, \qquad
\frac{5\alpha}{2}= \frac{5\cdot30^{\circ}}{2}=75^{\circ}.$$
Using standard values:
$$\sin15^{\circ}= \sin(45^{\circ}-30^{\circ}) = \frac{\sqrt2}{2}\cdot\frac12 - \frac{\sqrt3}{2}\cdot\frac{\sqrt2}{2}
= \frac{\sqrt2-\sqrt6}{4},$$
$$\sin75^{\circ}= \sin(45^{\circ}+30^{\circ}) = \frac{\sqrt2}{2}\cdot\frac12 + \frac{\sqrt3}{2}\cdot\frac{\sqrt2}{2}
= \frac{\sqrt2+\sqrt6}{4}.$$
Squares:
$$\sin^2 15^{\circ}= \left(\frac{\sqrt2-\sqrt6}{4}\right)^2
= \frac{8-4\sqrt3}{16}= \frac12 - \frac{\sqrt3}{4},$$
$$\sin^2 75^{\circ}= \left(\frac{\sqrt2+\sqrt6}{4}\right)^2
= \frac{8+4\sqrt3}{16}= \frac12 + \frac{\sqrt3}{4}.$$
Desired difference:
$$\sin^2\!\left(\frac{5\alpha}{2}\right) - \sin^2\!\left(\frac{\alpha}{2}\right)
= \left(\frac12 + \frac{\sqrt3}{4}\right) - \left(\frac12 - \frac{\sqrt3}{4}\right)
= \frac{\sqrt3}{2}.$$
Hence the required value is $$\displaystyle \frac{\sqrt3}{2}.$$
Option B which is: $$\frac{\sqrt3}{2}$$.
Let $$(\alpha,\beta,\gamma)$$ be the co-ordinates of the foot of the perpendicular drawn from the point (5, 4, 2) on the line $$\overrightarrow{r}=(-\widehat{i}+3\widehat{j}+\widehat{k})+\lambda(2\widehat{i}+3\widehat{j}-\widehat{k}).$$ Then the length of the projection of the vector $$\alpha\widehat{i}+\beta\widehat{j}+\gamma\widehat{k}$$ on the vector $$6\widehat{i}+2\widehat{j}+3\widehat{k}$$ is:
Foot of perpendicular from (5,4,2) on line $$\vec{r} = (-1,3,1) + \lambda(2,3,-1)$$.
Point on line: $$(-1+2\lambda, 3+3\lambda, 1-\lambda)$$.
Direction from (5,4,2) to point: $$(-6+2\lambda, -1+3\lambda, -1-\lambda)$$.
Perpendicular to direction (2,3,-1):
$$2(-6+2\lambda) + 3(-1+3\lambda) + (-1)(-1-\lambda) = 0$$
$$-12+4\lambda-3+9\lambda+1+\lambda = 0$$
$$14\lambda - 14 = 0 \Rightarrow \lambda = 1$$
Foot = $$(1, 6, 0)$$, so $$(\alpha, \beta, \gamma) = (1, 6, 0)$$.
Projection of $$(1, 6, 0)$$ on $$(6, 2, 3)$$: $$\frac{6+12+0}{\sqrt{36+4+9}} = \frac{18}{7}$$.
The answer is Option 4: $$\frac{18}{7}$$.
Let $$\overrightarrow{AB} = 2\widehat{i}+4\widehat{j}-5\widehat{k}$$ and $$ \overrightarrow{AD} = \widehat{i}+2\widehat{j}+\lambda\widehat{k}, \lambda\text{ }\epsilon \text{ } R$$. Let the projection of the vector $$ \overrightarrow{v}=\widehat{i}+\widehat{j}+\widehat{k}$$ on the disgonal $$\overrightarrow{AC}$$ of the parallelogram ABCD be of length one unit. If $$\alpha> \beta$$, be the roots of the equation $$\lambda^{2}x^{2}-6\lambda x+5=0$$, then $$2\alpha-\beta$$ is equal to
Given vectors $$\overrightarrow{AB} = 2\widehat{i} + 4\widehat{j} - 5\widehat{k}$$ and $$\overrightarrow{AD} = \widehat{i} + 2\widehat{j} + \lambda\widehat{k}$$, the diagonal $$\overrightarrow{AC}$$ of parallelogram ABCD is found using vector addition:
$$\overrightarrow{AC} = \overrightarrow{AB} + \overrightarrow{AD} = (2\widehat{i} + 4\widehat{j} - 5\widehat{k}) + (\widehat{i} + 2\widehat{j} + \lambda\widehat{k}) = 3\widehat{i} + 6\widehat{j} + (\lambda - 5)\widehat{k}$$
The vector $$\overrightarrow{v} = \widehat{i} + \widehat{j} + \widehat{k}$$ is given. The projection of $$\overrightarrow{v}$$ onto $$\overrightarrow{AC}$$ has a length of 1 unit. The scalar projection of a vector $$\overrightarrow{a}$$ onto $$\overrightarrow{b}$$ is given by $$\frac{|\overrightarrow{a} \cdot \overrightarrow{b}|}{|\overrightarrow{b}|}$$, and this equals 1:
$$\left| \frac{\overrightarrow{v} \cdot \overrightarrow{AC}}{|\overrightarrow{AC}|} \right| = 1$$
This implies:
$$|\overrightarrow{v} \cdot \overrightarrow{AC}| = |\overrightarrow{AC}|$$
Compute the dot product:
$$\overrightarrow{v} \cdot \overrightarrow{AC} = (1)(3) + (1)(6) + (1)(\lambda - 5) = 3 + 6 + \lambda - 5 = \lambda + 4$$
Compute the magnitude of $$\overrightarrow{AC}$$:
$$|\overrightarrow{AC}| = \sqrt{3^2 + 6^2 + (\lambda - 5)^2} = \sqrt{9 + 36 + (\lambda - 5)^2} = \sqrt{45 + (\lambda - 5)^2}$$
So the equation is:
$$|\lambda + 4| = \sqrt{45 + (\lambda - 5)^2}$$
Since both sides are non-negative, squaring both sides:
$$(\lambda + 4)^2 = 45 + (\lambda - 5)^2$$
Expand both sides:
$$\lambda^2 + 8\lambda + 16 = 45 + \lambda^2 - 10\lambda + 25$$
Simplify the right side:
$$\lambda^2 + 8\lambda + 16 = \lambda^2 - 10\lambda + 70$$
Subtract $$\lambda^2$$ from both sides:
$$8\lambda + 16 = -10\lambda + 70$$
Bring like terms together:
$$8\lambda + 10\lambda = 70 - 16$$
$$18\lambda = 54$$
$$\lambda = 3$$
Verify by substituting $$\lambda = 3$$:
$$\overrightarrow{AC} = 3\widehat{i} + 6\widehat{j} + (3 - 5)\widehat{k} = 3\widehat{i} + 6\widehat{j} - 2\widehat{k}$$
$$|\overrightarrow{AC}| = \sqrt{3^2 + 6^2 + (-2)^2} = \sqrt{9 + 36 + 4} = \sqrt{49} = 7$$
$$\overrightarrow{v} \cdot \overrightarrow{AC} = 3 + 6 - 2 = 7$$
Projection length = $$\frac{|7|}{7} = 1$$, which satisfies the condition.
Now, $$\alpha > \beta$$ are the roots of the equation $$\lambda^2 x^2 - 6\lambda x + 5 = 0$$ with $$\lambda = 3$$:
$$(3)^2 x^2 - 6(3)x + 5 = 9x^2 - 18x + 5 = 0$$
Solve the quadratic equation using the quadratic formula:
$$x = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}$$
Here, $$a = 9$$, $$b = -18$$, $$c = 5$$:
Discriminant $$D = (-18)^2 - 4(9)(5) = 324 - 180 = 144 = 12^2$$
So:
$$x = \frac{18 \pm 12}{18}$$
Thus:
$$x_1 = \frac{18 + 12}{18} = \frac{30}{18} = \frac{5}{3}$$
$$x_2 = \frac{18 - 12}{18} = \frac{6}{18} = \frac{1}{3}$$
Since $$\alpha > \beta$$, $$\alpha = \frac{5}{3}$$, $$\beta = \frac{1}{3}$$.
Now compute $$2\alpha - \beta$$:
$$2\left(\frac{5}{3}\right) - \frac{1}{3} = \frac{10}{3} - \frac{1}{3} = \frac{9}{3} = 3$$
Therefore, $$2\alpha - \beta = 3$$.
Let $$\overrightarrow{a}=\widehat{i}-2\widehat{j}+3\widehat{k}, \overrightarrow{b}=2\widehat{i}+\widehat{j}-\widehat{k}, \overrightarrow{c}=\lambda \widehat{i}+\widehat{j}+\widehat{k}$$ and $$\overrightarrow{v}= \overrightarrow{a} \times \overrightarrow{b}$$. If $$\overrightarrow{v}\cdot\overrightarrow{c}=11$$ and the length of the projection of $$\overrightarrow{b}$$ on $$\overrightarrow{c}$$ is p, then $$9p^{2}$$ is equal to
Given: $$\vec{a} = \hat{i} - 2\hat{j} + 3\hat{k}$$, $$\vec{b} = 2\hat{i} + \hat{j} - \hat{k}$$, $$\vec{c} = \lambda\hat{i} + \hat{j} + \hat{k}$$, and $$\vec{v} = \vec{a} \times \vec{b}$$.
We need to find $$9p^2$$ where $$\vec{v} \cdot \vec{c} = 11$$ and $$p$$ is the length of projection of $$\vec{b}$$ on $$\vec{c}$$.
Computing the cross product $$\vec{v} = \vec{a} \times \vec{b}$$, we evaluate the determinant $$\vec{v} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -2 & 3 \\ 2 & 1 & -1 \end{vmatrix}$$ which expands as $$= \hat{i}[(-2)(-1) - (3)(1)] - \hat{j}[(1)(-1) - (3)(2)] + \hat{k}[(1)(1) - (-2)(2)]$$ then simplifies to $$= \hat{i}[2 - 3] - \hat{j}[-1 - 6] + \hat{k}[1 + 4]$$ and finally yields $$= -\hat{i} + 7\hat{j} + 5\hat{k}.$$
Using $$\vec{v} \cdot \vec{c} = 11$$ we write $$\vec{v} \cdot \vec{c} = (-1)(\lambda) + (7)(1) + (5)(1) = -\lambda + 7 + 5 = 12 - \lambda$$ so that $$12 - \lambda = 11$$, which implies $$\lambda = 1$$. Thus $$\vec{c} = \hat{i} + \hat{j} + \hat{k}$$.
The length of projection of $$\vec{b}$$ on $$\vec{c}$$ is given by $$p = \frac{|\vec{b} \cdot \vec{c}|}{|\vec{c}|},$$ with $$\vec{b} \cdot \vec{c} = (2)(1) + (1)(1) + (-1)(1) = 2 + 1 - 1 = 2$$ and $$|\vec{c}| = \sqrt{1 + 1 + 1} = \sqrt{3},$$ hence $$p = \frac{|2|}{\sqrt{3}} = \frac{2}{\sqrt{3}}.$$
Since $$p^2 = \frac{4}{3},$$ it follows that $$9p^2 = 9 \times \frac{4}{3} = 12.$$
The correct answer is Option (1): $$\boxed{12}$$.
Let $$\overrightarrow{a}= 2\widehat{i}-\widehat{j}+\widehat{k}$$ and $$\overrightarrow{b}= \lambda \widehat{j}+2\widehat{k}, \lambda\in Z$$ be two vectors. Let $$\overrightarrow{c}= \overrightarrow{a} \times \overrightarrow{b} \text{and } \overrightarrow{d}$$ be a vector of magnitude 2 in yz-plane. If $$|\overrightarrow{c}|=\sqrt{53}$$, then the maximum possible value of $$\left(\overrightarrow{c}\cdot\overrightarrow{d}\right)^{2}$$ is equal to :
We need to find the maximum value of $$(\vec{c} \cdot \vec{d})^2$$ given the constraints.
First, we compute $$\vec{c} = \vec{a} \times \vec{b}$$. We have $$\vec{a} = 2\hat{i} - \hat{j} + \hat{k} = (2, -1, 1)$$ and $$\vec{b} = \lambda\hat{j} + 2\hat{k} = (0, \lambda, 2)$$. The cross product can be evaluated as:
$$\vec{c} = \vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & -1 & 1 \\ 0 & \lambda & 2 \end{vmatrix}$$
$$= \hat{i}[(-1)(2) - (1)(\lambda)] - \hat{j}[(2)(2) - (1)(0)] + \hat{k}[(2)(\lambda) - (-1)(0)]$$
$$= \hat{i}(-2 - \lambda) - \hat{j}(4) + \hat{k}(2\lambda)$$
$$= (-2-\lambda, -4, 2\lambda)$$
Next, using $$|\vec{c}| = \sqrt{53}$$ we determine $$\lambda$$ by setting $$|\vec{c}|^2 = (-2-\lambda)^2 + (-4)^2 + (2\lambda)^2 = 53$$, which gives:
$$ (\lambda+2)^2 + 16 + 4\lambda^2 = 53$$
$$ \lambda^2 + 4\lambda + 4 + 16 + 4\lambda^2 = 53$$
$$ 5\lambda^2 + 4\lambda + 20 = 53$$
$$ 5\lambda^2 + 4\lambda - 33 = 0$$
By the quadratic formula, $$\lambda = \frac{-4 \pm \sqrt{16 + 660}}{10} = \frac{-4 \pm \sqrt{676}}{10} = \frac{-4 \pm 26}{10}$$, so $$\lambda = \frac{22}{10} = 2.2$$ or $$\lambda = \frac{-30}{10} = -3$$. Since $$\lambda \in \mathbb{Z}$$, it follows that $$\lambda = -3$$.
Substituting $$\lambda = -3$$ into the expression for $$\vec{c}$$ yields $$\vec{c} = (-2-(-3), -4, 2(-3)) = (1, -4, -6)$$.
Finally, to maximize $$(\vec{c} \cdot \vec{d})^2$$, note that $$\vec{d}$$ lies in the yz-plane with $$|\vec{d}| = 2$$, so we write $$\vec{d} = (0, d_2, d_3)$$ subject to $$d_2^2 + d_3^2 = 4$$. Then
$$\vec{c} \cdot \vec{d} = (1)(0) + (-4)(d_2) + (-6)(d_3) = -4d_2 - 6d_3$$
and we seek the maximum of $$(-4d_2 - 6d_3)^2$$ under the constraint $$d_2^2 + d_3^2 = 4$$. By the Cauchy-Schwarz inequality:
$$(-4d_2 - 6d_3)^2 \leq ((-4)^2 + (-6)^2)(d_2^2 + d_3^2) = (16 + 36)(4) = 52 \times 4 = 208$$
Equality occurs when $$\frac{d_2}{-4} = \frac{d_3}{-6}$$, i.e.\ when $$\vec{d}$$ is parallel to the projection of $$\vec{c}$$ onto the yz-plane, which is possible since $$\vec{d}$$ lies in that plane. Hence the maximum value of $$(\vec{c} \cdot \vec{d})^2$$ is 208.
The correct answer is Option 1: 208.
Let PQR be a triangle such that $$\overrightarrow{PQ}=-2\widehat{i}-\widehat{j}+2\widehat{k}$$ and $$\overrightarrow{PR}=a\widehat{i}+b\widehat{j}-4\widehat{k},a,b \in Z$$. Let S be the point on QR, which is equidistant from the lines PQ and PR. If $$|\overrightarrow{PR}|=9$$ and $$\overrightarrow{PS}=\widehat{i}-7\widehat{j}+2\widehat{k}$$, then the value of 3a - 4b is_______
If $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{b} = \hat{j} - \hat{k}$$ and $$\vec{c}$$ be three vectors such that $$\vec{a} \times \vec{c} = \vec{b}$$ and $$\vec{a} \cdot \vec{c} = 3$$, then $$\vec{c} \cdot (\vec{a} - 2\vec{b})$$ is equal to _______.
Let $$\vec{a_k} = (\tan\theta_k)\hat{i} + \hat{j}$$ and $$\vec{b_k} = \hat{i} - (\cot\theta_k)\hat{j}$$, where $$\theta_k = \frac{2^{k-1}\pi}{2^n + 1}$$, for some $$n \in \mathbb{N}$$, $$n > 5$$. Then the value of $$\frac{\sum_{k=1}^{n}|\vec{a_k}|^2}{\sum_{k=1}^{n}|\vec{b_k}|^2}$$ is _____.
Let $$\overrightarrow{a}= 2\widehat{i}-\widehat{j}-\widehat{k}, \overrightarrow{b}=\widehat{i}+ 3\widehat{j}-\widehat{k}$$ and $$\overrightarrow{c} = 2\widehat{i}+\widehat{j}+3\widehat{k}.$$ Let $$\overrightarrow{\nu}$$ be the vector in the plane of the vectors $$\overrightarrow{a}$$ and $$\overrightarrow{b}$$, such that the length of its projection on the vector $$\overrightarrow{C}$$ is $$\frac{1}{\sqrt{14}}$$. Then $$\mid \overrightarrow{\nu} \mid$$ is euqal to
A vector lying in the plane of $$\overrightarrow{a}$$ and $$\overrightarrow{b}$$ can be written as a linear combination of the two,
$$\overrightarrow{\nu}= \overrightarrow{a}+ \lambda\,\overrightarrow{b} \qquad (\lambda \in \mathbb{R}).$$
The projection of $$\overrightarrow{\nu}$$ on $$\overrightarrow{c}$$ has length
$$\text{proj}_{\overrightarrow{c}}(\overrightarrow{\nu})=\frac{\left|\overrightarrow{\nu}\cdot\overrightarrow{c}\right|}{\left|\overrightarrow{c}\right|}.$$
First compute $$\left|\overrightarrow{c}\right|$$:
$$\overrightarrow{c}=2\widehat{i}+\widehat{j}+3\widehat{k}\;\;\Longrightarrow\;\;
\left|\overrightarrow{c}\right|=\sqrt{2^{2}+1^{2}+3^{2}}=\sqrt{14}.$$
Next evaluate the dot-products that will appear:
$$\overrightarrow{a}\cdot\overrightarrow{c}
=(2)(2)+(-1)(1)+(-1)(3)=4-1-3=0,$$
$$\overrightarrow{b}\cdot\overrightarrow{c}
=(1)(2)+(3)(1)+(-1)(3)=2+3-3=2.$$
Therefore
$$\overrightarrow{\nu}\cdot\overrightarrow{c} =(\overrightarrow{a}+\lambda\overrightarrow{b})\cdot\overrightarrow{c} =\overrightarrow{a}\cdot\overrightarrow{c} +\lambda\,\overrightarrow{b}\cdot\overrightarrow{c} =0+\lambda(2)=2\lambda.$$
The given condition on the projection is
$$\frac{\left|2\lambda\right|}{\sqrt{14}} =\frac{1}{\sqrt{14}} \;\;\Longrightarrow\;\; \left|2\lambda\right|=1 \;\;\Longrightarrow\;\; \lambda=\pm\frac12.$$
Choosing either sign (the magnitude will be the same), take
$$\overrightarrow{\nu}= \overrightarrow{a}+ \frac12\,\overrightarrow{b}.$$
Compute its magnitude:
$$\overrightarrow{\nu} =\left(2,-1,-1\right)+\frac12\left(1,3,-1\right) =\left(\frac52,\frac12,-\frac32\right).$$
Hence
$$\left|\overrightarrow{\nu}\right|^2
=\left(\frac52\right)^2+\left(\frac12\right)^2+\left(-\frac32\right)^2
=\frac{25}{4}+\frac{1}{4}+\frac{9}{4}
=\frac{35}{4},$$
$$\left|\overrightarrow{\nu}\right|
=\frac{\sqrt{35}}{2}.$$
Thus $$\mid\overrightarrow{\nu}\mid = \dfrac{\sqrt{35}}{2}.$$
Option D is correct.
Let $$\overrightarrow{a}=-\widehat{i}+\widehat{j}+2\widehat{k},\overrightarrow{b}=\widehat{i}-\widehat{j}-3\widehat{k},\overrightarrow{c}=\overrightarrow{a} \times \overrightarrow{b}\text{ and }\overrightarrow{d}=\overrightarrow{c}\times\overrightarrow{a}$$. Then $$\large (\overrightarrow{a}-\overrightarrow{b}).\overrightarrow{d}$$ is equal to:
We are given $$\vec{a} = -\hat{i} + \hat{j} + 2\hat{k}$$, $$\vec{b} = \hat{i} - \hat{j} - 3\hat{k}$$, $$\vec{c} = \vec{a} \times \vec{b}$$, and $$\vec{d} = \vec{c} \times \vec{a}$$. We need to find $$(\vec{a} - \vec{b}) \cdot \vec{d}$$.
First we compute $$\vec{c} = \vec{a} \times \vec{b}$$. Using the determinant form, we have $$\vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & 1 & 2 \\ 1 & -1 & -3 \end{vmatrix}$$ $$= \hat{i}(1 \cdot (-3) - 2 \cdot (-1)) - \hat{j}((-1)(-3) - 2 \cdot 1) + \hat{k}((-1)(-1) - 1 \cdot 1)$$ $$= \hat{i}(-3 + 2) - \hat{j}(3 - 2) + \hat{k}(1 - 1) = -\hat{i} - \hat{j} + 0\hat{k}$$ so $$\vec{c} = (-1, -1, 0)$$.
Next, we compute $$\vec{d} = \vec{c} \times \vec{a}$$. Again using the determinant, $$\vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & -1 & 0 \\ -1 & 1 & 2 \end{vmatrix}$$ $$= \hat{i}((-1)(2) - 0 \cdot 1) - \hat{j}((-1)(2) - 0 \cdot (-1)) + \hat{k}((-1)(1) - (-1)(-1))$$ $$= \hat{i}(-2) - \hat{j}(-2) + \hat{k}(-1 - 1) = -2\hat{i} + 2\hat{j} - 2\hat{k}$$ which gives $$\vec{d} = (-2, 2, -2)$$.
Then $$\vec{a} - \vec{b} = (-1 - 1, 1 - (-1), 2 - (-3)) = (-2, 2, 5)\,, $$ and the dot product is $$(\vec{a} - \vec{b}) \cdot \vec{d} = (-2)(-2) + (2)(2) + (5)(-2) = 4 + 4 - 10 = -2\,.$$
The correct answer is Option A: $$-2$$.
Let $$\overrightarrow{a}= 2\widehat{i}-5\widehat{j}+5\widehat{k}$$ and $$\overrightarrow{b}= \widehat{i}-\widehat{j}+3\widehat{k}$$. If $$\overrightarrow{C}$$ is a vector such that $$2(\overrightarrow{a}\times\overrightarrow{c})+3(\overrightarrow{b}\times\overrightarrow{c})= \overrightarrow{0}$$ and $$(\overrightarrow{a}-\overrightarrow{b})\cdot\overrightarrow{c}=-97,$$ then $$\mid \overrightarrow{c}\times\widehat{k} \mid^{2}$$ is equal to
We need to find $$|\vec{c} \times \hat{k}|^2$$ given the conditions on vectors $$\vec{a}$$, $$\vec{b}$$, and $$\vec{c}$$.
The vectors are given by $$\vec{a} = 2\hat{i} - 5\hat{j} + 5\hat{k}$$ and $$\vec{b} = \hat{i} - \hat{j} + 3\hat{k}$$, and it is known that $$2(\vec{a} \times \vec{c}) + 3(\vec{b} \times \vec{c}) = \vec{0}$$ as well as $$(\vec{a} - \vec{b}) \cdot \vec{c} = -97$$.
The cross product relation can be written as $$(2\vec{a} + 3\vec{b}) \times \vec{c} = \vec{0}$$, which means $$\vec{c}$$ is parallel to $$2\vec{a} + 3\vec{b}$$.
Calculating $$2\vec{a} + 3\vec{b}$$ gives $$2\vec{a} + 3\vec{b} = 2(2\hat{i} - 5\hat{j} + 5\hat{k}) + 3(\hat{i} - \hat{j} + 3\hat{k}) = (4+3)\hat{i} + (-10-3)\hat{j} + (10+9)\hat{k} = 7\hat{i} - 13\hat{j} + 19\hat{k}$$, so we may write $$\vec{c} = t(7\hat{i} - 13\hat{j} + 19\hat{k})$$ for some scalar $$t$$.
Using $$(\vec{a} - \vec{b}) \cdot \vec{c} = -97$$ and noting that $$\vec{a} - \vec{b} = (2-1)\hat{i} + (-5+1)\hat{j} + (5-3)\hat{k} = \hat{i} - 4\hat{j} + 2\hat{k}$$, we get $$(\vec{a} - \vec{b}) \cdot \vec{c} = t(7 + 52 + 38) = 97t = -97$$, hence $$t = -1$$ and $$\vec{c} = -7\hat{i} + 13\hat{j} - 19\hat{k}$$.
To compute $$|\vec{c} \times \hat{k}|^2$$, note that $$\vec{c} \times \hat{k} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -7 & 13 & -19 \\ 0 & 0 & 1 \end{vmatrix} = \hat{i}(13 \cdot 1 - (-19) \cdot 0) - \hat{j}((-7)(1) - (-19)(0)) + \hat{k}(0 - 0) = 13\hat{i} + 7\hat{j}$$, so $$|\vec{c} \times \hat{k}|^2 = 13^2 + 7^2 = 169 + 49 = 218$$.
Therefore, $$|\vec{c} \times \hat{k}|^2 = $$ Option 3: 218.
Let $$\overrightarrow{a}$$ and $$ \overrightarrow{b}$$ be two unit vectors such that the angle between them is $$\frac{\pi}{3}$$. Tf $$\lambda \overrightarrow{a} +2\overrightarrow{b}\text{ and }3\overrightarrow{a}-\lambda \overrightarrow{b}$$ are perpendicular to each other, then the number of values of $$\lambda$$ in [-1,3] is :
Let $$\vec{a}$$ and $$\vec{b}$$ be unit vectors with the angle $$\frac{\pi}{3}$$ between them, and consider the vectors $$\lambda\vec{a} + 2\vec{b}$$ and $$3\vec{a} - \lambda\vec{b}$$ for $$\lambda\in[-1,3]$$; we seek the number of values of $$\lambda$$ for which these vectors are perpendicular.
Since perpendicularity means their dot product vanishes, we write
$$(\lambda\vec{a} + 2\vec{b}) \cdot (3\vec{a} - \lambda\vec{b}) = 0\,. $$
Expanding the dot product gives
$$3\lambda(\vec{a}\cdot\vec{a}) - \lambda^2(\vec{a}\cdot\vec{b}) + 6(\vec{b}\cdot\vec{a}) - 2\lambda(\vec{b}\cdot\vec{b}) = 0\,. $$
Because $$|\vec{a}|=|\vec{b}|=1$$ we have $$\vec{a}\cdot\vec{a}=1$$ and $$\vec{b}\cdot\vec{b}=1$$, while $$\vec{a}\cdot\vec{b}=|\vec{a}||\vec{b}|\cos\frac{\pi}{3}=\frac12\,. $$
Substituting these results into the expanded dot product yields
$$3\lambda - \frac{\lambda^2}{2} + 6\cdot\frac12 - 2\lambda = 0\,, $$
which simplifies to
$$\lambda - \frac{\lambda^2}{2} + 3 = 0\,. $$
Multiplying both sides by $$-2$$ gives the quadratic equation
$$\lambda^2 - 2\lambda - 6 = 0\,. $$
Solving this quadratic leads to
$$\lambda = \frac{2\pm\sqrt{4+24}}{2} = 1\pm\sqrt{7}\,. $$
Since $$\sqrt{7}\approx2.646$$, the two solutions are approximately $$1+\sqrt{7}\approx3.646$$ and $$1-\sqrt{7}\approx-1.646$$, neither of which lies in the interval $$[-1,3]$$.
Therefore there are no values of $$\lambda$$ in $$[-1,3]$$ that make the given vectors perpendicular, and hence the number of such values is 0.
Final Answer: 0.
Let the arc AC of a circle subtend a right angle at the centre O. If the point B on the arc AC, divides the arc AC such that $$\frac{\text{lenght of arc AB}}{\text{lenght of arc BC}}=\frac{1}{5}$$,and $$\overrightarrow{OC}=\alpha\overrightarrow{OA}+\beta\overrightarrow{OB}$$, then $$\alpha +\sqrt{2}(\sqrt{3}-1)\beta$$ is equal to
Arc AC subtends $$90°$$ at center O. B divides arc AC in ratio 1:5, so arc AB subtends $$\frac{1}{6} \times 90° = 15°$$.
With A at angle $$0°$$, B at $$15°$$, C at $$90°$$ (unit radius):
$$\vec{OA} = (1, 0)$$, $$\vec{OB} = (\cos 15°, \sin 15°)$$, $$\vec{OC} = (0, 1)$$.
From $$\vec{OC} = \alpha\vec{OA} + \beta\vec{OB}$$:
$$0 = \alpha + \beta\cos 15°$$ and $$1 = \beta\sin 15°$$.
$$\beta = \frac{1}{\sin 15°} = \frac{4}{\sqrt{6}-\sqrt{2}} = \sqrt{6}+\sqrt{2}$$
$$\alpha = -\cot 15° = -(2+\sqrt{3})$$
Evaluating:
$$(\sqrt{3}-1)(\sqrt{6}+\sqrt{2}) = 3\sqrt{2}-\sqrt{2} = 2\sqrt{2}$$
$$\sqrt{2}(\sqrt{3}-1)\beta = \sqrt{2} \times 2\sqrt{2} = 4$$
$$\alpha + \sqrt{2}(\sqrt{3}-1)\beta = -(2+\sqrt{3}) + 4 = 2 - \sqrt{3}$$
The correct answer is Option 2: $$2 - \sqrt{3}$$.
If $$\vec{a}$$ is nonzero vector such that its projections on the vectors $$2\hat{i} - \hat{j} + 2\hat{k}$$, $$\hat{i} + 2\hat{j} - 2\hat{k}$$ and $$\hat{k}$$ are equal, then a unit vector along $$\vec{a}$$ is:
Let $$\vec{a} = x\hat{i} + y\hat{j} + z\hat{k}$$ be a nonzero vector. The projection of $$\vec{a}$$ on a vector $$\vec{v}$$ is $$\frac{\vec{a} \cdot \vec{v}}{|\vec{v}|}$$.
The three given vectors are $$\vec{v_1} = 2\hat{i} - \hat{j} + 2\hat{k}$$, $$\vec{v_2} = \hat{i} + 2\hat{j} - 2\hat{k}$$, and $$\vec{v_3} = \hat{k}$$.
Their magnitudes are: $$|\vec{v_1}| = \sqrt{4+1+4} = 3$$, $$|\vec{v_2}| = \sqrt{1+4+4} = 3$$, $$|\vec{v_3}| = 1$$.
The projections are:
$$\text{proj}_1 = \frac{2x - y + 2z}{3}, \quad \text{proj}_2 = \frac{x + 2y - 2z}{3}, \quad \text{proj}_3 = z$$
Setting proj$$_1$$ = proj$$_2$$: $$2x - y + 2z = x + 2y - 2z$$, which gives $$x - 3y + 4z = 0$$ ...(1)
Setting proj$$_2$$ = proj$$_3$$: $$\frac{x + 2y - 2z}{3} = z$$, which gives $$x + 2y - 5z = 0$$ ...(2)
From (1) and (2): subtracting (2) from (1): $$-5y + 9z = 0$$, so $$y = \frac{9z}{5}$$.
Substituting into (2): $$x + \frac{18z}{5} - 5z = 0$$, so $$x = 5z - \frac{18z}{5} = \frac{7z}{5}$$.
Taking $$z = 5$$: $$\vec{a} = 7\hat{i} + 9\hat{j} + 5\hat{k}$$.
$$|\vec{a}| = \sqrt{49 + 81 + 25} = \sqrt{155}$$.
The unit vector along $$\vec{a}$$ is $$\frac{1}{\sqrt{155}}(7\hat{i} + 9\hat{j} + 5\hat{k})$$.
Hence, the correct answer is Option C.
Let the position vectors of three vertices of a triangle be $$4\vec p+\vec q-3\vec r,\;-5\vec p+\vec q+2\vec r$$ and $$2\vec p-\vec q+2\vec r.$$ If the position vectors of the orthocenter and the circumcenter of the triangle are $$\frac{\vec p+\vec q+\vec r}{4}$$ and $$\alpha\vec p+\beta\vec q+\gamma\vec r$$ { respectively, then $$\alpha+2\beta+5\gamma$$ is equal to:
Let the vertices of the triangle be $$P = 4\vec{p} + \vec{q} - 3\vec{r}$$, $$Q = -5\vec{p} + \vec{q} + 2\vec{r}$$, $$R = 2\vec{p} - \vec{q} + 2\vec{r}$$.
The orthocenter is $$H = \frac{\vec{p} + \vec{q} + \vec{r}}{4}$$.
We use the property that the centroid $$G$$ divides $$OH$$ in ratio $$1:2$$ (where $$O$$ is circumcenter), i.e., $$G$$ divides segment from circumcenter to orthocenter. More precisely: $$\vec{G} = \frac{\vec{P}+\vec{Q}+\vec{R}}{3}$$.
$$\vec{G} = \frac{(4-5+2)\vec{p} + (1+1-1)\vec{q} + (-3+2+2)\vec{r}}{3} = \frac{\vec{p} + \vec{q} + \vec{r}}{3}$$
Euler line relation: $$\vec{G} = \frac{\vec{H} + 2\vec{O}}{3}$$ where $$O$$ is the circumcenter.
$$\frac{\vec{p}+\vec{q}+\vec{r}}{3} = \frac{1}{3}\left(\frac{\vec{p}+\vec{q}+\vec{r}}{4} + 2\vec{O}\right)$$
$$\vec{p}+\vec{q}+\vec{r} = \frac{\vec{p}+\vec{q}+\vec{r}}{4} + 2\vec{O}$$
$$2\vec{O} = \frac{3(\vec{p}+\vec{q}+\vec{r})}{4}$$
$$\vec{O} = \frac{3}{8}(\vec{p}+\vec{q}+\vec{r}) = \frac{3}{8}\vec{p} + \frac{3}{8}\vec{q} + \frac{3}{8}\vec{r}$$
So $$\alpha = 3/8$$, $$\beta = 3/8$$, $$\gamma = 3/8$$.
$$\alpha + 2\beta + 5\gamma = \frac{3}{8} + \frac{6}{8} + \frac{15}{8} = \frac{24}{8} = 3$$.
The correct answer is Option A: 3.
Consider the vectors
$$\vec{x} = \hat{i} + 2\hat{j} + 3\hat{k}$$, $$\quad \vec{y} = 2\hat{i} + 3\hat{j} + \hat{k}$$, $$\quad$$ and $$\quad \vec{z} = 3\hat{i} + \hat{j} + 2\hat{k}$$.
For two distinct positive real numbers $$\alpha$$ and $$\beta$$, define
$$\vec{X} = \alpha\vec{x} + \beta\vec{y} - \vec{z}$$, $$\quad \vec{Y} = \alpha\vec{y} + \beta\vec{z} - \vec{x}$$, $$\quad$$ and $$\quad \vec{Z} = \alpha\vec{z} + \beta\vec{x} - \vec{y}$$.
If the vectors $$\vec{X}$$, $$\vec{Y}$$, and $$\vec{Z}$$ lie in a plane, then the value of $$\alpha + \beta - 3$$ is ______.
The vectors lie in a plane if and only if their scalar triple product is zero, i.e. $$\vec{X}\cdot(\vec{Y}\times\vec{Z}) = 0$$. In component form this is equivalent to the determinant of the three column vectors being zero.
First write each required vector in $$\hat i,\hat j,\hat k$$ components.
$$\vec{x} = (1,\,2,\,3),\; \vec{y} = (2,\,3,\,1),\; \vec{z} = (3,\,1,\,2)$$
$$\vec{X}= \alpha\vec{x}+\beta\vec{y}-\vec{z} = (\alpha+2\beta-3,\; 2\alpha+3\beta-1,\; 3\alpha+\beta-2)$$
$$\vec{Y}= \alpha\vec{y}+\beta\vec{z}-\vec{x} = (2\alpha+3\beta-1,\; 3\alpha+\beta-2,\; \alpha+2\beta-3)$$
$$\vec{Z}= \alpha\vec{z}+\beta\vec{x}-\vec{y} = (3\alpha+\beta-2,\; \alpha+2\beta-3,\; 2\alpha+3\beta-1)$$
Introduce the shorthand
$$A = \alpha+2\beta-3,\qquad B = 2\alpha+3\beta-1,\qquad C = 3\alpha+\beta-2$$
Then$$ \vec{X} = (A,\;B,\;C),\; \vec{Y} = (B,\;C,\;A),\; \vec{Z} = (C,\;A,\;B). $$
Set up the determinant:
$$ \left| \begin{array}{ccc} A & B & C\\ B & C & A\\ C & A & B \end{array} \right| = 0. $$
Evaluating the determinant,
$$ \begin{aligned} D &= A(CB - A^{2}) - B(B^{2} - AC) + C(AB - C^{2}) \\ &= (ABC - A^{3}) + (ABC - B^{3}) + (ABC - C^{3}) \\ &= 3ABC - (A^{3}+B^{3}+C^{3}). \end{aligned} $$
Hence$$D = 0 \Longrightarrow A^{3}+B^{3}+C^{3}-3ABC = 0.$$ Using the identity$$ A^{3}+B^{3}+C^{3}-3ABC = (A+B+C)\,\bigl(A^{2}+B^{2}+C^{2}-AB-BC-CA\bigr), $$we get two possibilities:
Case 1:$$A+B+C = 0.$$
Case 2:$$A=B=C.$$
Because $$\alpha,\beta$$ are distinct positive numbers, Case 2 is impossible (solving $$A=B$$ forces $$\alpha+\beta=-2$$, which contradicts positivity). Therefore only Case 1 survives.
Compute $$A+B+C$$:
$$ \begin{aligned} A+B+C &= (\alpha+2\beta-3) + (2\alpha+3\beta-1) + (3\alpha+\beta-2)\\ &= 6\alpha + 6\beta - 6\\ &= 6(\alpha+\beta-1). \end{aligned} $$
Setting this to zero gives $$\alpha+\beta-1 = 0 \Longrightarrow \alpha+\beta = 1.$$ Both $$\alpha,\beta$$ can be positive and distinct while satisfying this relation, so the condition is admissible.
Finally, the required expression is
$$\alpha+\beta-3 = 1 - 3 = -2.$$
Hence the answer is -2.
$$\text{Let }\vec a=3\hat i-\hat j+2\hat k,\quad\vec b=\vec a\times(\hat i-2\hat k)\text{ and } \vec c=\vec b\times\hat k.\text{Then the projection of } (\vec c-2\hat j)\text{ on } \vec a \text{ is:}$$
a=3i-j+2k, b=a×(i-2k), c=b×k. Find projection of (c-2j) on a.
b = (3i-j+2k)×(i-2k) = |i j k; 3 -1 2; 1 0 -2| = i(2-0)-j(-6-2)+k(0+1) = 2i+8j+k
c = b×k = (2i+8j+k)×k = |i j k; 2 8 1; 0 0 1| = i(8)-j(2)+k(0) = 8i-2j
c-2j = 8i-4j. Projection on a: (8i-4j)·(3i-j+2k)/|a| = (24+4+0)/√14 = 28/√14 = 2√14.
The correct answer is Option 1: 2√14.
Consider two vectors $$\vec{u} = 3\hat{i} - \hat{j}$$ and $$\vec{v} = 2\hat{i} + \hat{j} - \lambda\hat{k}$$, $$\lambda \gt 0$$. The angle between them is given by $$\cos^{-1}\left(\dfrac{\sqrt{5}}{2\sqrt{7}}\right)$$. Let $$\vec{v} = \vec{v}_1 + \vec{v}_2$$, where $$\vec{v}_1$$ is parallel to $$\vec{u}$$ and $$\vec{v}_2$$ is perpendicular to $$\vec{u}$$. Then the value $$|\vec{v}_1|^2 + |\vec{v}_2|^2$$ is equal to
The given vectors are $$\vec u = 3\hat i - \hat j$$ and $$\vec v = 2\hat i + \hat j - \lambda \hat k$$ with $$\lambda \gt 0$$.
The angle $$\theta$$ between them satisfies
$$\cos\theta = \dfrac{\vec u \cdot \vec v}{\lvert\vec u\rvert\,\lvert\vec v\rvert} = \dfrac{\sqrt5}{2\sqrt7}\,\,\,\,-(1)$$
First compute the numerator:
$$\vec u \cdot \vec v = (3)(2) + (-1)(1) + (0)(-\lambda) = 6 - 1 = 5$$
Next compute the magnitudes:
$$\lvert\vec u\rvert = \sqrt{3^{2} + (-1)^{2}} = \sqrt{9 + 1} = \sqrt{10}$$
$$\lvert\vec v\rvert = \sqrt{2^{2} + 1^{2} + \lambda^{2}} = \sqrt{5 + \lambda^{2}}$$
Insert these results in $$(1)$$:
$$\frac{5}{\sqrt{10}\,\sqrt{5+\lambda^{2}}} = \frac{\sqrt5}{2\sqrt7}$$
Cross-multiply and simplify:
$$10\sqrt7 = \sqrt5\,\sqrt{10}\,\sqrt{5+\lambda^{2}}$$
$$10\sqrt7 = (\sqrt{5\cdot10})\,\sqrt{5+\lambda^{2}} = 5\sqrt2\,\sqrt{5+\lambda^{2}}$$
Divide by $$5$$:
$$2\sqrt7 = \sqrt2\,\sqrt{5+\lambda^{2}}$$
Square both sides:
$$(2\sqrt7)^{2} = (\sqrt2\,\sqrt{5+\lambda^{2}})^{2}$$
$$4\cdot7 = 2\,(5+\lambda^{2})$$
$$28 = 10 + 2\lambda^{2}$$
$$18 = 2\lambda^{2}$$
$$\lambda^{2} = 9 \Longrightarrow \lambda = 3 \quad(\text{since } \lambda \gt 0)$$
Thus $$\vec v = 2\hat i + \hat j - 3\hat k$$ and its magnitude is
$$\lvert\vec v\rvert^{2} = 2^{2} + 1^{2} + (-3)^{2} = 4 + 1 + 9 = 14\,\,\,\,-(2)$$
Now write $$\vec v = \vec v_1 + \vec v_2$$ where $$\vec v_1$$ is parallel to $$\vec u$$ and $$\vec v_2$$ is perpendicular to $$\vec u$$.
Because a parallel component and a perpendicular component are orthogonal, we have the Pythagorean relation
$$\lvert\vec v\rvert^{2} = \lvert\vec v_1\rvert^{2} + \lvert\vec v_2\rvert^{2}\,\,\,\,-(3)$$
Substituting the value from $$(2)$$ into $$(3)$$ gives
$$\lvert\vec v_1\rvert^{2} + \lvert\vec v_2\rvert^{2} = 14$$
Hence the required value is $$14$$.
Option B is correct.
Let $$\vec{w} = \hat{i} + \hat{j} - 2\hat{k}$$, and $$\vec{u}$$ and $$\vec{v}$$ be two vectors, such that $$\vec{u} \times \vec{v} = \vec{w}$$ and $$\vec{v} \times \vec{w} = \vec{u}$$. Let $$\alpha, \beta, \gamma$$, and $$t$$ be real numbers such that
$$\vec{u} = \alpha\hat{i} + \beta\hat{j} + \gamma\hat{k}, \quad -t\alpha + \beta + \gamma = 0, \quad \alpha - t\beta + \gamma = 0, \quad \text{and} \quad \alpha + \beta - t\gamma = 0.$$
Match each entry in List-I to the correct entry in List-II and choose the correct option.
The three vectors are connected by
$$\vec{u}\times\vec{v}= \vec{w},\qquad \vec{v}\times\vec{w}= \vec{u},\qquad \vec{w}= \hat{i}+ \hat{j}-2\hat{k}.$$
The cross-product of two vectors is perpendicular to each of them, so
$$\vec{u}\cdot\vec{v}=0, \qquad \vec{v}\cdot\vec{w}=0, \qquad \vec{w}\cdot\vec{u}=0.$$
Hence the three vectors are pair-wise perpendicular.
Magnitude of $$\vec{w}$$:
$$|\vec{w}|^{2}=1^{2}+1^{2}+(-2)^{2}=6.$$
Using the identity $$|\vec{a}\times\vec{b}|^{2}=|\,\vec{a}\,|^{2}|\,\vec{b}\,|^{2}-(\vec{a}\cdot\vec{b})^{2},$$
$$|\vec{w}|^{2}=|\vec{u}\times\vec{v}|^{2}=|\vec{u}|^{2}|\vec{v}|^{2}\quad(\because\vec{u}\cdot\vec{v}=0)$$
and
$$|\vec{u}|^{2}=|\vec{v}\times\vec{w}|^{2}=|\vec{v}|^{2}|\vec{w}|^{2}\quad(\because\vec{v}\cdot\vec{w}=0).$$
Let $$|\vec{u}|^{2}=a,\; |\vec{v}|^{2}=b.$$
Then $$6=ab \quad\text{and}\quad a=6b.$$
Substituting, $$6=(6b)b\;\Longrightarrow\; b^{2}=1\;\Longrightarrow\; b=1.$$
Therefore
Case P: $$|\vec{v}|^{2}=1\; \Rightarrow\; (P)\to(2).$$
The components of $$\vec{u}=\alpha\hat{i}+\beta\hat{j}+\gamma\hat{k}$$ obey the three equations
$$-t\alpha+\beta+\gamma=0\; -(1)$$
$$\alpha-t\beta+\gamma=0\; -(2)$$
$$\alpha+\beta-t\gamma=0\; -(3).$$
For a non-trivial solution, the determinant of the coefficient matrix must vanish:
$$\begin{vmatrix}-t&1&1\\[2pt]1&-t&1\\[2pt]1&1&-t\end{vmatrix}=0 \;\Longrightarrow\; -t^{3}+3t+2=0 \;\Longrightarrow\; t^{3}-3t-2=0 =(t-2)(t+1)^{2}=0.$$
Thus $$t=2\quad\text{or}\quad t=-1.$$ We must also satisfy $$\vec{w}\cdot\vec{u}=0\;\Rightarrow\; \alpha+\beta-2\gamma=0\; -(4).$$
Taking $$t=-1$$
Equations (1)-(3) all reduce to $$\alpha+\beta+\gamma=0.$$
With $$\alpha=\sqrt{3}$$,
$$\beta+\gamma=-\sqrt{3}\; -(5).$$
Using (4): $$\sqrt{3}+\beta-2\gamma=0
\;\Longrightarrow\;
-3\gamma=0
\;\Longrightarrow\;
\gamma=0,\;\beta=-\sqrt{3}.$$
Hence
Case Q: $$\gamma^{2}=0\;\Rightarrow\; (Q)\to(1).$$
Case R: $$(\beta+\gamma)^{2}=(-\sqrt{3})^{2}=3\;\Rightarrow\; (R)\to(4).$$
Taking $$t=2$$
From (1): $$\beta=2\alpha-\gamma.$$
From (2): $$\alpha-2\beta+\gamma=0
\;\Longrightarrow\;
\gamma=\alpha.$$
Therefore $$\beta=\alpha.$$
With $$\alpha=\sqrt{2}$$ we get $$t=2,$$ hence
Case S: $$t+3=2+3=5\;\Rightarrow\; (S)\to(5).$$
Collecting all matches:
(P)$$\to$$(2), (Q)$$\to$$(1), (R)$$\to$$(4), (S)$$\to$$(5).
Thus the correct option is
Option A which is: (P)$$\to$$(2), (Q)$$\to$$(1), (R)$$\to$$(4), (S)$$\to$$(5).
Let $$\vec{a} = 2\hat{i} - 3\hat{j} + \hat{k}$$, $$\vec{b} = 3\hat{i} + 2\hat{j} + 5\hat{k}$$ and a vector $$\vec{c}$$ be such that $$(\vec{a} - \vec{c}) \times \vec{b} = -18\hat{i} - 3\hat{j} + 12\hat{k}$$ and $$\vec{a} \cdot \vec{c} = 3$$. If $$\vec{b} \times \vec{c} = \vec{d}$$, then $$|\vec{a} \cdot \vec{d}|$$ is equal to :
Let $$\vec{a}=2\hat{i}-3\hat{j}+\hat{k}$$, $$\vec{b}=3\hat{i}+2\hat{j}+5\hat{k}$$ and $$\vec{c}=x\hat{i}+y\hat{j}+z\hat{k}$$.
The condition $$(\vec{a}-\vec{c})\times\vec{b}=-18\hat{i}-3\hat{j}+12\hat{k}$$ gives three scalar equations.
Write $$\vec{a}-\vec{c}=(2-x)\hat{i}+(-3-y)\hat{j}+(1-z)\hat{k}.$$
For two vectors $$\vec{p}=(p_1,p_2,p_3)$$ and $$\vec{q}=(q_1,q_2,q_3)$$, the cross product is
$$\vec{p}\times\vec{q}=\bigl(p_2q_3-p_3q_2\bigr)\hat{i}-\bigl(p_1q_3-p_3q_1\bigr)\hat{j}+\bigl(p_1q_2-p_2q_1\bigr)\hat{k}.$$
Putting $$\vec{p}=(2-x,-3-y,1-z)$$ and $$\vec{q}=(3,2,5)$$:
$$\begin{aligned} (\vec{a}-\vec{c})\times\vec{b} &=\bigl[5(-3-y)-2(1-z)\bigr]\hat{i}\\ &\;\;-\bigl[5(2-x)-3(1-z)\bigr]\hat{j}\\ &\;\;+\bigl[2(2-x)-3(-3-y)\bigr]\hat{k}. \end{aligned}$$
Equating with $$-18\hat{i}-3\hat{j}+12\hat{k}$$ gives
$$5(-3-y)-2(1-z)=-18$$ $$-(1)$$
$$5(2-x)-3(1-z)=3$$ $$-(2)$$
$$2(2-x)-3(-3-y)=12$$ $$-(3)$$
Simplify each:
From $$(1):\; -15-5y-2+2z=-18 \;\Rightarrow\; 5y-2z=1 \;-(4)$$
From $$(2):\; 10-5x-3+3z=3 \;\Rightarrow\; 5x-3z=4 \;-(5)$$
From $$(3):\; 4-2x+9+3y=12 \;\Rightarrow\; 2x-3y=1 \;-(6)$$
The second given condition is $$\vec{a}\cdot\vec{c}=3$$:
$$2x-3y+z=3 \;-(7)$$
Solve equations $$(4)-(7).$$
From $$(6):\; 2x-3y=1 \;\Rightarrow\; y=\frac{2x-1}{3}.$$
Substitute this in $$(7):$$
$$2x-3\!\left(\frac{2x-1}{3}\right)+z=3$$
$$\Rightarrow\;2x-(2x-1)+z=3 \;\Rightarrow\;1+z=3 \;\Rightarrow\; z=2.$$
Insert $$z=2$$ in $$(5):$$
$$5x-3(2)=4 \;\Rightarrow\; 5x-6=4 \;\Rightarrow\; x=2.$$
Put $$x=2$$ in $$(6):$$
$$2(2)-3y=1 \;\Rightarrow\; 4-3y=1 \;\Rightarrow\; y=1.$$
Hence $$\vec{c}=2\hat{i}+\hat{j}+2\hat{k}.$$
Now find $$\vec{d}=\vec{b}\times\vec{c}.$$
Compute the determinant:
$$\vec{d}= \begin{vmatrix}
\hat{i} & \hat{j} & \hat{k}\\
3 & 2 & 5\\
2 & 1 & 2
\end{vmatrix}
= \bigl(2\cdot2-5\cdot1\bigr)\hat{i}-\bigl(3\cdot2-5\cdot2\bigr)\hat{j}+\bigl(3\cdot1-2\cdot2\bigr)\hat{k}.$$
Simplifying:
$$\vec{d}=-1\hat{i}+4\hat{j}-1\hat{k}= -\hat{i}+4\hat{j}-\hat{k}.$$
Finally compute $$\vec{a}\cdot\vec{d}:$$
$$\vec{a}\cdot\vec{d}=(2,-3,1)\cdot(-1,4,-1)=-2-12-1=-15.$$
Therefore
$$\lvert\vec{a}\cdot\vec{d}\rvert=15.$$
Option D is correct.
Let $$\vec{a}$$ and $$\vec{b}$$ be the vectors of the same magnitude such that $$\frac{|\vec{a}+\vec{b}|+|\vec{a}-\vec{b}|}{|\vec{a}+\vec{b}|-|\vec{a}-\vec{b}|} = \sqrt{2}+1$$. Then $$\frac{|\vec{a}+\vec{b}|^2}{|\vec{a}|^2}$$ is :
Let the common magnitude of the two vectors be $$|\vec a| = |\vec b| = m$$ and let the angle between them be $$\theta$$.
Using the cosine rule for vectors:
$$|\vec a + \vec b| = \sqrt{m^2 + m^2 + 2m^2 \cos\theta} = m\sqrt{2(1+\cos\theta)}$$
$$|\vec a - \vec b| = \sqrt{m^2 + m^2 - 2m^2 \cos\theta} = m\sqrt{2(1-\cos\theta)}$$
Rewrite these with the half-angle substitution $$\theta = 2x$$ (so $$x = \theta/2$$):
$$|\vec a + \vec b| = 2m\cos x$$
$$|\vec a - \vec b| = 2m\sin x$$
The given ratio becomes
$$\frac{|\vec a+\vec b| + |\vec a-\vec b|}{|\vec a+\vec b| - |\vec a-\vec b|} =
\frac{2m(\cos x + \sin x)}{2m(\cos x - \sin x)} =
\frac{\cos x + \sin x}{\cos x - \sin x}$$
This ratio equals $$\sqrt{2}+1$$, hence
$$\frac{\cos x + \sin x}{\cos x - \sin x} = \sqrt{2}+1 \; -(1)$$
Cross-multiplying in $$(1)$$:
$$\cos x + \sin x = (\sqrt{2}+1)(\cos x - \sin x)$$
$$\cos x + \sin x - (\sqrt{2}+1)\cos x + (\sqrt{2}+1)\sin x = 0$$
$$\cos x(1-\sqrt{2}-1) + \sin x(1+\sqrt{2}+1) = 0$$
$$\cos x(-\sqrt{2}) + \sin x(\sqrt{2}+2) = 0$$
$$\tan x = \frac{\sqrt{2}}{\sqrt{2}+2} \; -(2)$$
The quantity required is
$$\frac{|\vec a+\vec b|^{2}}{|\vec a|^{2}} = \frac{(2m\cos x)^{2}}{m^{2}} = 4\cos^{2}x \; -(3)$$
From $$(2)$$, set $$\tan x = t = \dfrac{\sqrt{2}}{\sqrt{2}+2}$$. Then
$$\cos^{2}x = \frac{1}{1+t^{2}}$$
Compute $$t^{2}$$:
$$t^{2} = \frac{2}{(\sqrt{2}+2)^{2}} = \frac{2}{6+4\sqrt{2}} = \frac{1}{3+2\sqrt{2}}$$
Hence
$$1+t^{2} = 1 + \frac{1}{3+2\sqrt{2}} = \frac{4+2\sqrt{2}}{3+2\sqrt{2}}$$
Insert this into $$(3)$$:
$$4\cos^{2}x = \frac{4}{1+t^{2}} = 4 \cdot \frac{3+2\sqrt{2}}{4+2\sqrt{2}}$$
$$= \frac{12 + 8\sqrt{2}}{4 + 2\sqrt{2}}
= \frac{6 + 4\sqrt{2}}{2 + \sqrt{2}}
= 2 + \sqrt{2}$$
Therefore,
$$\frac{|\vec a + \vec b|^{2}}{|\vec a|^{2}} = 2 + \sqrt{2}$$
The correct choice is Option C.
Let $$\widehat{a}$$ be a unit vector perpendicular to the vectors $$\overrightarrow{b}=\widehat{i}-2\widehat{j}+3\widehat{k}$$ and $$\overrightarrow{c}=2\widehat{i}+3\widehat{j}-\widehat{k}$$, and makes an angle of $$\cos^{-1}(-\frac{1}{3})$$ with the vector $$\widehat{i}+\widehat{j}+\widehat{k}$$ . If $$\widehat{a}$$ makes an angle of $$\frac{\pi}{3}$$ with the vector $$\widehat{i}+\alpha\widehat{j}+\widehat{k}$$ , then the value of $$\alpha$$ is :
First, find a vector perpendicular to both $$\vec{b} = \hat{i} - 2\hat{j} + 3\hat{k}$$ and $$\vec{c} = 2\hat{i} + 3\hat{j} - \hat{k}$$. $$\vec{b} \times \vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -2 & 3 \\ 2 & 3 & -1 \end{vmatrix}$$ which simplifies to $$= \hat{i}(2-9) - \hat{j}(-1-6) + \hat{k}(3+4) = -7\hat{i} + 7\hat{j} + 7\hat{k}$$.
Therefore, $$\vec{b} \times \vec{c} = 7(-\hat{i} + \hat{j} + \hat{k})$$. The unit vector in this direction is given by $$\hat{a} = \pm\frac{1}{\sqrt{3}}(-\hat{i} + \hat{j} + \hat{k})$$.
Next, $$\hat{a}$$ makes an angle $$\cos^{-1}\bigl(-\tfrac{1}{3}\bigr)$$ with $$\hat{i} + \hat{j} + \hat{k}$$, so
$$\hat{a} \cdot (\hat{i} + \hat{j} + \hat{k}) = |\hat{a}|\;|\hat{i}+\hat{j}+\hat{k}|\;\cos\theta.$$
For $$\hat{a} = \frac{1}{\sqrt{3}}(-1+1+1) = \frac{1}{\sqrt{3}},$$
$$\cos\theta = \frac{1/\sqrt{3}}{\sqrt{3}} = \frac{1}{3}.$$
For $$\hat{a} = \frac{-1}{\sqrt{3}}(-1+1+1) = \frac{-1}{\sqrt{3}},$$
$$\cos\theta = \frac{-1/\sqrt{3}}{\sqrt{3}} = -\frac{1}{3}$$ ✓.
Hence, $$\hat{a} = \frac{-1}{\sqrt{3}}(-\hat{i} + \hat{j} + \hat{k}) = \frac{1}{\sqrt{3}}(\hat{i} - \hat{j} - \hat{k}).$$
Now, $$\hat{a}$$ makes an angle $$\frac{\pi}{3}$$ with $$\hat{i} + \alpha\hat{j} + \hat{k}$$, so
$$\cos\frac{\pi}{3} = \frac{\hat{a} \cdot (\hat{i} + \alpha\hat{j} + \hat{k})}{|\hat{i} + \alpha\hat{j} + \hat{k}|}$$
gives
$$\frac{1}{2} = \frac{\frac{1}{\sqrt{3}}(1 - \alpha - 1)}{\sqrt{2 + \alpha^2}} = \frac{-\alpha}{\sqrt{3}\sqrt{2+\alpha^2}}$$
and therefore
$$\frac{1}{2} = \frac{-\alpha}{\sqrt{3(2+\alpha^2)}}.$$
Since the left side is positive, $$\alpha$$ must be negative. Squaring both sides yields
$$\frac{1}{4} = \frac{\alpha^2}{3(2+\alpha^2)},$$
so
$$3(2+\alpha^2) = 4\alpha^2,\quad 6 + 3\alpha^2 = 4\alpha^2,\quad \alpha^2 = 6,\quad \alpha = -\sqrt{6}.$$
The correct answer is Option 2: $$-\sqrt{6}$$.
Let $$\vec a=\hat{i}+2\hat{j}+3\hat{k}, b=3\hat{i}+\hat{j}-\hat{k} $$ and be three vectors such that $$c$$ is coplanar with $$ \vec a$$ and $$\vec b$$. If $$\vec c $$ is perpendicular to $$\vec b$$ and $$\vec a\cdot \vec c=5,$$ then $$|\vec c|$$ is equal to:
$$\vec{a} = \hat{i}+2\hat{j}+3\hat{k}$$, $$\vec{b} = 3\hat{i}+\hat{j}-\hat{k}$$. $$\vec{c}$$ is coplanar with $$\vec{a}$$ and $$\vec{b}$$, perpendicular to $$\vec{b}$$, and $$\vec{a}\cdot\vec{c} = 5$$.
Since $$\vec{c}$$ is coplanar with $$\vec{a}$$ and $$\vec{b}$$: $$\vec{c} = \lambda\vec{a} + \mu\vec{b}$$
$$\vec{c} \perp \vec{b}$$: $$\vec{c}\cdot\vec{b} = 0$$
$$\lambda(\vec{a}\cdot\vec{b}) + \mu(\vec{b}\cdot\vec{b}) = 0$$
$$\vec{a}\cdot\vec{b} = 3+2-3 = 2$$, $$|\vec{b}|^2 = 9+1+1 = 11$$
$$2\lambda + 11\mu = 0 \Rightarrow \lambda = -\frac{11\mu}{2}$$
$$\vec{a}\cdot\vec{c} = 5$$
$$\lambda|\vec{a}|^2 + \mu(\vec{a}\cdot\vec{b}) = 5$$
$$|\vec{a}|^2 = 1+4+9 = 14$$
$$14\lambda + 2\mu = 5$$
$$14(-11\mu/2) + 2\mu = 5$$
$$-77\mu + 2\mu = 5$$
$$-75\mu = 5 \Rightarrow \mu = -1/15$$
$$\lambda = -11(-1/15)/2 = 11/30$$
$$\vec{c} = \frac{11}{30}(1,2,3) - \frac{1}{15}(3,1,-1)$$
$$= (\frac{11}{30}-\frac{2}{10}, \frac{22}{30}-\frac{1}{15}, \frac{33}{30}+\frac{1}{15})$$
$$= (\frac{11-6}{30}, \frac{22-2}{30}, \frac{33+2}{30}) = (\frac{5}{30}, \frac{20}{30}, \frac{35}{30}) = (\frac{1}{6}, \frac{2}{3}, \frac{7}{6})$$
$$|\vec{c}|^2 = \frac{1}{36} + \frac{4}{9} + \frac{49}{36} = \frac{1+16+49}{36} = \frac{66}{36} = \frac{11}{6}$$
$$|\vec{c}| = \sqrt{\frac{11}{6}}$$
The correct answer is Option 1: $$\sqrt{\frac{11}{6}}$$.
Let $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{b} = 3\hat{i} + 2\hat{j} - \hat{k}$$, $$\vec{c} = \lambda\hat{j} + \mu\hat{k}$$ and $$\hat{d}$$ be a unit vector such that $$\vec{a} \times \hat{d} = \vec{b} \times \hat{d}$$ and $$\vec{c} \cdot \hat{d} = 1$$. If $$\vec{c}$$ is perpendicular to $$\vec{a}$$, then $$|3\lambda\hat{d} + \mu\vec{c}|^2$$ is equal to __________.
Given
$$\vec{a}= \hat{i}+ \hat{j}+ \hat{k},\; \vec{b}=3\hat{i}+2\hat{j}-\hat{k},\; \vec{c}= \lambda\hat{j}+ \mu\hat{k},\; \hat{d}\; \text{(unit)}$$
with the conditions
$$\vec{a}\times\hat{d}=\vec{b}\times\hat{d},\qquad \vec{c}\cdot\hat{d}=1,\qquad \vec{c}\perp\vec{a}.$$
Step 1: Relating $$\vec{a}$$ and $$\vec{b}$$ to $$\hat{d}$$
The identity $$\vec{u}\times\hat{d}=\vec{v}\times\hat{d}\;\Longrightarrow\;(\vec{u}-\vec{v})\times\hat{d}= \vec{0}$$ means $$\vec{u}-\vec{v}$$ is parallel to $$\hat{d}$$.
Thus $$\bigl(\vec{a}-\vec{b}\bigr)\times\hat{d}= \vec{0}\;\Longrightarrow\;\vec{a}-\vec{b}=t\hat{d}\;$$ for some scalar $$t$$.
Compute $$\vec{a}-\vec{b}$$:
$$\vec{a}-\vec{b}=(1-3)\hat{i}+(1-2)\hat{j}+(1-(-1))\hat{k}=-2\hat{i}-\hat{j}+2\hat{k}.$$
The magnitude of this vector is
$$\lvert\vec{a}-\vec{b}\rvert=\sqrt{(-2)^2+(-1)^2+2^2}=3.$$
Therefore the required unit vector is
$$\hat{d}=s\,\frac{-2\hat{i}-\hat{j}+2\hat{k}}{3},\qquad s=\pm1.$$
Explicitly
$$\hat{d}=s\Bigl(-\tfrac23\,\hat{i}-\tfrac13\,\hat{j}+\tfrac23\,\hat{k}\Bigr).$$
Step 2: Using $$\vec{c}\cdot\hat{d}=1$$
With $$\vec{c}=(0,\lambda,\mu)$$, dot product gives
$$\vec{c}\cdot\hat{d}=s\Bigl(-\tfrac{\lambda}{3}+\tfrac{2\mu}{3}\Bigr)=1$$
$$\Longrightarrow\;s(-\lambda+2\mu)=3\;.$$ $$-(1)$$
Step 3: Using $$\vec{c}\perp\vec{a}$$
Orthogonality with $$\vec{a}=(1,1,1)$$ yields
$$\vec{a}\cdot\vec{c}=0\;\Longrightarrow\;\lambda+\mu=0\;\Longrightarrow\;\mu=-\lambda.$$ $$-(2)$$
Step 4: Determining $$\lambda,\mu$$
Substituting $$\mu=-\lambda$$ from $$(2)$$ into $$(1)$$:
$$s(-\lambda+2(-\lambda))=s(-3\lambda)=3\;\Longrightarrow\;\lambda=-\frac{1}{s},\qquad \mu=-\lambda=\frac{1}{s}.$$
Hence
For $$s=1:\; \lambda=-1,\;\mu=1,\;\hat{d}=(-\tfrac23,-\tfrac13,\tfrac23).$$
For $$s=-1:\;\lambda=1,\;\mu=-1,\;\hat{d}=(\tfrac23,\tfrac13,-\tfrac23).$$
Step 5: Evaluating $$\bigl|\,3\lambda\hat{d}+\mu\vec{c}\bigr|^2$$
Take the case $$s=1$$ (the other choice will give the same result).
Here $$\lambda=-1,\;\mu=1$$ and
$$3\lambda\hat{d}=3(-1)\Bigl(-\tfrac23,-\tfrac13,\tfrac23\Bigr)=(2,1,-2),$$
$$\mu\vec{c}=1\,(0,-1,1)=(0,-1,1).$$
Therefore
$$3\lambda\hat{d}+\mu\vec{c}=(2,1,-2)+(0,-1,1)=(2,0,-1).$$
The square of its magnitude is
$$\lvert(2,0,-1)\rvert^{2}=2^{2}+0^{2}+(-1)^{2}=4+1=5.$$
Repeating with $$s=-1$$ also produces the vector $$(2,0,-1)$$, confirming the result is independent of the sign choice.
Final Answer:
$$\bigl|\,3\lambda\hat{d}+\mu\vec{c}\bigr|^{2}=5.$$
Let $$\overrightarrow{c}$$ be the projection vector of $$\overrightarrow{b}=\lambda\widehat{i}+4\widehat{k}$$, $$\lambda > 0$$, on the vector $$\overrightarrow{a}=\widehat{i}+2\widehat{j}+2\widehat{k}$$. If $$|\overrightarrow{a}+ \overrightarrow{c}|= 7$$, then the area of the parallelogram formed by the vectors $$\overrightarrow{b}$$ and $$\overrightarrow{c}$$ is ______
$$\vec{a} = \hat{i} + 2\hat{j} + 2\hat{k}$$, $$\vec{b} = \lambda\hat{i} + 4\hat{k}$$ ($$\lambda > 0$$). $$\vec{c}$$ is the projection vector of $$\vec{b}$$ on $$\vec{a}$$. $$|\vec{a} + \vec{c}| = 7$$.
The projection of $$\vec{b}$$ onto $$\vec{a}$$ is:
$$\vec{c} = \frac{\vec{b} \cdot \vec{a}}{|\vec{a}|^2} \vec{a}$$
$$\vec{b} \cdot \vec{a} = \lambda(1) + 0(2) + 4(2) = \lambda + 8$$
$$|\vec{a}|^2 = 1 + 4 + 4 = 9$$
$$\vec{c} = \frac{\lambda + 8}{9} \vec{a} = \frac{\lambda + 8}{9}(\hat{i} + 2\hat{j} + 2\hat{k})$$
$$\vec{a} + \vec{c} = \left(1 + \frac{\lambda+8}{9}\right)\vec{a} = \frac{9 + \lambda + 8}{9}\vec{a} = \frac{\lambda + 17}{9}\vec{a}$$
$$|\vec{a} + \vec{c}| = \frac{|\lambda + 17|}{9} |\vec{a}| = \frac{\lambda + 17}{9} \times 3 = \frac{\lambda + 17}{3}$$
(Since $$\lambda > 0$$, $$\lambda + 17 > 0$$)
$$\frac{\lambda + 17}{3} = 7 \implies \lambda = 4$$
$$\vec{b} = 4\hat{i} + 4\hat{k}$$
$$\vec{c} = \frac{4+8}{9}(\hat{i} + 2\hat{j} + 2\hat{k}) = \frac{12}{9}(\hat{i} + 2\hat{j} + 2\hat{k}) = \frac{4}{3}(\hat{i} + 2\hat{j} + 2\hat{k})$$
$$\vec{c} = \frac{4}{3}\hat{i} + \frac{8}{3}\hat{j} + \frac{8}{3}\hat{k}$$
Area = $$|\vec{b} \times \vec{c}|$$
$$\vec{b} \times \vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 4 & 0 & 4 \\ 4/3 & 8/3 & 8/3 \end{vmatrix}$$
$$= \hat{i}(0 \cdot \frac{8}{3} - 4 \cdot \frac{8}{3}) - \hat{j}(4 \cdot \frac{8}{3} - 4 \cdot \frac{4}{3}) + \hat{k}(4 \cdot \frac{8}{3} - 0)$$
$$= \hat{i}(-\frac{32}{3}) - \hat{j}(\frac{16}{3}) + \hat{k}(\frac{32}{3})$$
$$|\vec{b} \times \vec{c}| = \frac{1}{3}\sqrt{32^2 + 16^2 + 32^2} = \frac{1}{3}\sqrt{1024 + 256 + 1024} = \frac{1}{3}\sqrt{2304} = \frac{48}{3} = 16$$
The area is 16.
Let $$\vec{a} = \hat{i} + 2\hat{j} + \hat{k}$$, $$\vec{b} = 3\hat{i} - 3\hat{j} + 3\hat{k}$$, $$\vec{c} = 2\hat{i} - \hat{j} + 2\hat{k}$$ and $$\vec{d}$$ be a vector such that $$\vec{b} \times \vec{d} = \vec{c} \times \vec{d}$$ and $$\vec{a} \cdot \vec{d} = 4$$. Then $$|\vec{a} \times \vec{d}|^2$$ is equal to ________.
Given $$\vec{a} = \hat{i} + 2\hat{j} + \hat{k}$$, $$\vec{b} = 3\hat{i} - 3\hat{j} + 3\hat{k}$$, $$\vec{c} = 2\hat{i} - \hat{j} + 2\hat{k}$$.
We need $$\vec{b} \times \vec{d} = \vec{c} \times \vec{d}$$, which gives $$(\vec{b} - \vec{c}) \times \vec{d} = \vec{0}$$.
$$\vec{b} - \vec{c} = (3-2)\hat{i} + (-3+1)\hat{j} + (3-2)\hat{k} = \hat{i} - 2\hat{j} + \hat{k}$$
Since $$(\vec{b} - \vec{c}) \times \vec{d} = \vec{0}$$, $$\vec{d}$$ is parallel to $$\vec{b} - \vec{c} = \hat{i} - 2\hat{j} + \hat{k}$$.
So $$\vec{d} = t(\hat{i} - 2\hat{j} + \hat{k})$$ for some scalar $$t$$.
Using $$\vec{a} \cdot \vec{d} = 4$$: $$t(1 - 4 + 1) = 4$$, so $$t(-2) = 4$$, giving $$t = -2$$.
Therefore, $$\vec{d} = -2\hat{i} + 4\hat{j} - 2\hat{k}$$.
Now, $$\vec{a} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 2 & 1 \\ -2 & 4 & -2 \end{vmatrix}$$
$$= \hat{i}(-4 - 4) - \hat{j}(-2 + 2) + \hat{k}(4 + 4) = -8\hat{i} + 0\hat{j} + 8\hat{k}$$
$$|\vec{a} \times \vec{d}|^2 = 64 + 0 + 64 = 128$$
Hence, the correct answer is 128.
Let $$\overrightarrow{a}=\hat{i}+\hat{j}+\hat{k},\overrightarrow{b}=2\hat{i}+2\hat{j}+\hat{k}$$ and $$\overrightarrow{d}=\overrightarrow{a}\times \overrightarrow{b}$$. If$$\overrightarrow{c}$$ is a vector such that $$\overrightarrow{a}. \overrightarrow{c}=|\overrightarrow{c}|,|\overrightarrow{c}-2\overrightarrow{a}|^{2}=8$$ and the angle between $$\overrightarrow{d}$$ and $$\overrightarrow{c}$$ is $$\frac{\pi}{4}$$, then $$|10-3\overrightarrow{b}.\overrightarrow{c}|+|\overrightarrow{d}\times \overrightarrow{c}|^{2}$$ is equal to
Given vectors:
$$\overrightarrow{a} = \hat{i} + \hat{j} + \hat{k}$$
$$\overrightarrow{b} = 2\hat{i} + 2\hat{j} + \hat{k}$$
First, compute $$\overrightarrow{d} = \overrightarrow{a} \times \overrightarrow{b}$$.
The cross product is:
$$\overrightarrow{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 1 & 1 \\ 2 & 2 & 1 \end{vmatrix} = \hat{i}(1 \cdot 1 - 1 \cdot 2) - \hat{j}(1 \cdot 1 - 1 \cdot 2) + \hat{k}(1 \cdot 2 - 1 \cdot 2) = \hat{i}(-1) - \hat{j}(-1) + \hat{k}(0) = -\hat{i} + \hat{j}$$
So, $$\overrightarrow{d} = -\hat{i} + \hat{j}$$.
Let $$\overrightarrow{c} = x\hat{i} + y\hat{j} + z\hat{k}$$. The given conditions are:
1. $$\overrightarrow{a} \cdot \overrightarrow{c} = |\overrightarrow{c}|$$
$$\overrightarrow{a} \cdot \overrightarrow{c} = x + y + z$$
$$|\overrightarrow{c}| = \sqrt{x^2 + y^2 + z^2}$$
So,
$$x + y + z = \sqrt{x^2 + y^2 + z^2} \quad \text{(1)}$$
2. $$|\overrightarrow{c} - 2\overrightarrow{a}|^2 = 8$$
$$2\overrightarrow{a} = 2\hat{i} + 2\hat{j} + 2\hat{k}$$
$$\overrightarrow{c} - 2\overrightarrow{a} = (x - 2)\hat{i} + (y - 2)\hat{j} + (z - 2)\hat{k}$$
So,
$$(x - 2)^2 + (y - 2)^2 + (z - 2)^2 = 8 \quad \text{(2)}$$
3. Angle between $$\overrightarrow{d}$$ and $$\overrightarrow{c}$$ is $$\frac{\pi}{4}$$.
$$\overrightarrow{d} \cdot \overrightarrow{c} = (-1)(x) + (1)(y) + (0)(z) = -x + y$$
$$|\overrightarrow{d}| = \sqrt{(-1)^2 + 1^2} = \sqrt{2}$$
$$\cos \frac{\pi}{4} = \frac{\sqrt{2}}{2}$$
So,
$$\overrightarrow{d} \cdot \overrightarrow{c} = |\overrightarrow{d}| |\overrightarrow{c}| \cos \frac{\pi}{4} \implies -x + y = \sqrt{2} \cdot |\overrightarrow{c}| \cdot \frac{\sqrt{2}}{2} = |\overrightarrow{c}|$$
Thus,
$$-x + y = |\overrightarrow{c}| \quad \text{(3)}$$
From equations (1) and (3), let $$|\overrightarrow{c}| = k$$:
$$x + y + z = k \quad \text{(1)}$$
$$-x + y = k \quad \text{(3)}$$
Subtract equation (3) from equation (1):
$$(x + y + z) - (-x + y) = k - k \implies 2x + z = 0 \quad \text{(4)}$$
So, $$z = -2x$$.
From equation (3):
$$y = k + x \quad \text{(5)}$$
Substitute $$z = -2x$$ and $$y = k + x$$ into equation (1):
$$x + (k + x) + (-2x) = k \implies k = k$$ (always true).
Now, $$k = |\overrightarrow{c}| = \sqrt{x^2 + y^2 + z^2} = \sqrt{x^2 + (k + x)^2 + (-2x)^2}$$:
$$k^2 = x^2 + (k + x)^2 + (-2x)^2 = x^2 + k^2 + 2kx + x^2 + 4x^2 = k^2 + 6x^2 + 2kx$$
$$0 = 6x^2 + 2kx \implies 2x(3x + k) = 0$$
So, $$x = 0$$ or $$k = -3x$$.
**Case 1: $$x = 0$$**
From equation (4): $$z = -2(0) = 0$$.
From equation (5): $$y = k + 0 = k$$.
From equation (1): $$0 + k + 0 = k \implies k = k$$ (true).
Equation (2):
$$(0 - 2)^2 + (k - 2)^2 + (0 - 2)^2 = 4 + (k - 2)^2 + 4 = (k - 2)^2 + 8 = 8$$
$$(k - 2)^2 = 0 \implies k = 2$$
Then $$y = 2$$, so $$\overrightarrow{c} = 2\hat{j}$$.
**Case 2: $$k = -3x$$**
Since $$k \geq 0$$, $$-3x \geq 0 \implies x \leq 0$$.
From equation (5): $$y = -3x + x = -2x$$.
From equation (4): $$z = -2x$$.
Equation (2):
$$(x - 2)^2 + (-2x - 2)^2 + (-2x - 2)^2 = (x - 2)^2 + 2(-2(x + 1))^2 = (x - 2)^2 + 8(x + 1)^2 = 8$$
$$(x - 2)^2 + 8(x + 1)^2 = 8$$
$$x^2 - 4x + 4 + 8(x^2 + 2x + 1) = 8 \implies x^2 - 4x + 4 + 8x^2 + 16x + 8 = 8 \implies 9x^2 + 12x + 12 = 8$$
$$9x^2 + 12x + 4 = 0$$
Discriminant: $$12^2 - 4 \cdot 9 \cdot 4 = 144 - 144 = 0$$
$$x = \frac{-12}{18} = -\frac{2}{3}$$
Then $$k = -3 \left(-\frac{2}{3}\right) = 2$$, $$y = -2 \left(-\frac{2}{3}\right) = \frac{4}{3}$$, $$z = -2 \left(-\frac{2}{3}\right) = \frac{4}{3}$$, so $$\overrightarrow{c} = -\frac{2}{3}\hat{i} + \frac{4}{3}\hat{j} + \frac{4}{3}\hat{k}$$.
Now compute $$|10 - 3\overrightarrow{b} \cdot \overrightarrow{c}| + |\overrightarrow{d} \times \overrightarrow{c}|^2$$ for both cases.
**For $$\overrightarrow{c} = 2\hat{j}$$:**
$$\overrightarrow{b} \cdot \overrightarrow{c} = (2)(0) + (2)(2) + (1)(0) = 4$$
$$3\overrightarrow{b} \cdot \overrightarrow{c} = 12$$
$$10 - 12 = -2 \implies | -2 | = 2$$
$$\overrightarrow{d} \times \overrightarrow{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & 1 & 0 \\ 0 & 2 & 0 \end{vmatrix} = \hat{i}(0) - \hat{j}(0) + \hat{k}(-2) = -2\hat{k}$$
$$|\overrightarrow{d} \times \overrightarrow{c}|^2 = (-2)^2 = 4$$
Sum: $$2 + 4 = 6$$.
**For $$\overrightarrow{c} = -\frac{2}{3}\hat{i} + \frac{4}{3}\hat{j} + \frac{4}{3}\hat{k}$$:**
$$\overrightarrow{b} \cdot \overrightarrow{c} = (2)\left(-\frac{2}{3}\right) + (2)\left(\frac{4}{3}\right) + (1)\left(\frac{4}{3}\right) = -\frac{4}{3} + \frac{8}{3} + \frac{4}{3} = \frac{8}{3}$$
$$3\overrightarrow{b} \cdot \overrightarrow{c} = 8$$
$$10 - 8 = 2 \implies |2| = 2$$
$$\overrightarrow{d} \times \overrightarrow{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & 1 & 0 \\ -\frac{2}{3} & \frac{4}{3} & \frac{4}{3} \end{vmatrix} = \hat{i}\left(1 \cdot \frac{4}{3} - 0 \cdot \frac{4}{3}\right) - \hat{j}\left(-1 \cdot \frac{4}{3} - 0 \cdot \left(-\frac{2}{3}\right)\right) + \hat{k}\left(-1 \cdot \frac{4}{3} - 1 \cdot \left(-\frac{2}{3}\right)\right) = \frac{4}{3}\hat{i} + \frac{4}{3}\hat{j} - \frac{2}{3}\hat{k}$$
$$|\overrightarrow{d} \times \overrightarrow{c}|^2 = \left(\frac{4}{3}\right)^2 + \left(\frac{4}{3}\right)^2 + \left(-\frac{2}{3}\right)^2 = \frac{16}{9} + \frac{16}{9} + \frac{4}{9} = \frac{36}{9} = 4$$
Sum: $$2 + 4 = 6$$.
In both cases, the expression evaluates to 6.
Thus, $$|10 - 3\overrightarrow{b} \cdot \overrightarrow{c}| + |\overrightarrow{d} \times \overrightarrow{c}|^2 = 6$$.
**Final Answer:** $$6$$
Let the three sides of a triangle ABC be given by the vectors $$2\hat{i} - \hat{j} + \hat{k}$$, $$\hat{i} - 3\hat{j} - 5\hat{k}$$ and $$3\hat{i} - 4\hat{j} - 4\hat{k}$$. Let G be the centroid of the triangle ABC. Then $$6\left(|\vec{AG}|^2 + |\vec{BG}|^2 + |\vec{CG}|^2\right)$$ is equal to ______.
Let A, B, C be three points in $$xy-plane$$, whose position vector are given by $$\sqrt{3}\hat{i}+\hat{j}, \hat{i}+\sqrt{3}\hat{j}$$ and $$a\hat{i}+ (1-a)\hat{j}$$ respectively with respect to the origin O . If the distance of the point C from the line bisecting the angle between the vectors $$\overrightarrow{OA}$$ and $$\overrightarrow{OB}$$ is $$\frac{9}{\sqrt{2}}$$, then the sum of all the possible values of $$a$$ is :
Let the position vectors of points A, B and C be given by $$\overrightarrow{OA}=\sqrt{3}\,\hat{i}+\hat{j}$$, $$\overrightarrow{OB}=\hat{i}+\sqrt{3}\,\hat{j}$$ and $$\overrightarrow{OC}=a\,\hat{i}+(1-a)\,\hat{j}$$ respectively.
We first find the equation of the internal angle bisector of the angle between $$\overrightarrow{OA}$$ and $$\overrightarrow{OB}$$.
Formula for internal bisector direction: if $$\mathbf{v}_1$$ and $$\mathbf{v}_2$$ are two vectors, then a direction vector along the internal bisector is $$\mathbf{u}=\frac{\mathbf{v}_1}{\|\mathbf{v}_1\|}+\frac{\mathbf{v}_2}{\|\mathbf{v}_2\|}$$.
Here, $$\|\overrightarrow{OA}\|=\sqrt{(\sqrt{3})^2+1^2}=\sqrt{3+1}=2$$ and $$\|\overrightarrow{OB}\|=\sqrt{1^2+(\sqrt{3})^2}=2$$.
Thus $$\mathbf{u} =\frac{1}{2}(\sqrt{3},1)+\frac{1}{2}(1,\sqrt{3}) =\Bigl(\frac{\sqrt{3}+1}{2},\frac{1+\sqrt{3}}{2}\Bigr) \;\Longrightarrow\; \text{direction }(d_x,d_y)=(\sqrt{3}+1,\;1+\sqrt{3}).$$
Since $$\sqrt{3}+1=1+\sqrt{3}$$, the slope of this line is $$m=\frac{1+\sqrt{3}}{\sqrt{3}+1}=1.$$ Hence the internal bisector is the line $$y-x=0\quad\text{or}\quad x-y=0.$$
Point C has coordinates $$(a,\;1-a)$$. The distance of $$(a,1-a)$$ from the line $$x-y=0$$ is given by the formula $$\text{Distance}=\frac{\bigl|a-(1-a)\bigr|}{\sqrt{1^2+(-1)^2}} =\frac{|2a-1|}{\sqrt{2}}\quad-(1)$$.
We are given that this distance equals $$\dfrac{9}{\sqrt{2}}$$. Equating with $$(1)$$ we get: $$\frac{|2a-1|}{\sqrt{2}}=\frac{9}{\sqrt{2}} \;\Longrightarrow\;|2a-1|=9.$$ This gives two cases:
Case 1: $$2a-1=9\quad\Longrightarrow\quad2a=10\quad\Longrightarrow\quad a=5.$$
Case 2: $$2a-1=-9\quad\Longrightarrow\quad2a=-8\quad\Longrightarrow\quad a=-4.$$
Thus the possible values of $$a$$ are $$5$$ and $$-4$$. Their sum is $$5+(-4)=1.$$
Final Answer: The sum of all possible values of $$a$$ is $$1$$ (Option C).
Let the position vectors of the vertices A, B and C of a tetrahedron ABCD be $$\widehat{i}+2\widehat{j}+\widehat{k},\widehat{i}+3\widehat{j}-2\widehat{k}$$ and $$2\widehat{i}+\widehat{j}-\widehat{k}$$ respectively. The altitude from the vertex D to the opposite face ABC meets the median line segment through of the triangle ABC at the point . If the length of AD is $$\frac{\sqrt{110}}{3}$$ and the volume of the tetrahedron is $$\frac{\sqrt{805}}{6\sqrt{2}}$$, then the position vector of is
The position vectors of vertices A, B, and C are given as: $$\overrightarrow{A} = \widehat{i} + 2\widehat{j} + \widehat{k},\quad \overrightarrow{B} = \widehat{i} + 3\widehat{j} - 2\widehat{k},\quad \overrightarrow{C} = 2\widehat{i} + \widehat{j} - \widehat{k}.$$
The median from vertex A to side BC is found by determining the midpoint M of BC: $$\overrightarrow{M} = \frac{\overrightarrow{B} + \overrightarrow{C}}{2} = \frac{(\widehat{i} + 3\widehat{j} - 2\widehat{k}) + (2\widehat{i} + \widehat{j} - \widehat{k})}{2} = \frac{3\widehat{i} + 4\widehat{j} - 3\widehat{k}}{2} = \frac{3}{2}\widehat{i} + 2\widehat{j} - \frac{3}{2}\widehat{k}.$$ The vector $$\overrightarrow{AM}$$ is $$\overrightarrow{AM} = \overrightarrow{M} - \overrightarrow{A} = \Bigl(\tfrac{3}{2}\widehat{i} + 2\widehat{j} - \tfrac{3}{2}\widehat{k}\Bigr) - (\widehat{i} + 2\widehat{j} + \widehat{k}) = \tfrac{1}{2}\widehat{i} - \tfrac{5}{2}\widehat{k}.$$
The parametric equation of the median AM is $$\overrightarrow{P}(t) = \overrightarrow{A} + t\,\overrightarrow{AM} = (\widehat{i} + 2\widehat{j} + \widehat{k}) + t\Bigl(\tfrac{1}{2}\widehat{i} - \tfrac{5}{2}\widehat{k}\Bigr) = \Bigl(1 + \tfrac{t}{2}\Bigr)\widehat{i} + 2\widehat{j} + \Bigl(1 - \tfrac{5t}{2}\Bigr)\widehat{k}.$$
The altitude from D to the plane ABC is perpendicular to the plane. The normal vector to plane ABC is $$\overrightarrow{AB}\times\overrightarrow{AC}$$, where $$\overrightarrow{AB} = \overrightarrow{B} - \overrightarrow{A} = (\widehat{i} + 3\widehat{j} - 2\widehat{k}) - (\widehat{i} + 2\widehat{j} + \widehat{k}) = \widehat{j} - 3\widehat{k},$$ $$\overrightarrow{AC} = \overrightarrow{C} - \overrightarrow{A} = (2\widehat{i} + \widehat{j} - \widehat{k}) - (\widehat{i} + 2\widehat{j} + \widehat{k}) = \widehat{i} - \widehat{j} - 2\widehat{k}.$$ Their cross product is $$\overrightarrow{AB}\times\overrightarrow{AC} = \begin{vmatrix} \widehat{i} & \widehat{j} & \widehat{k} \\ 0 & 1 & -3 \\ 1 & -1 & -2 \end{vmatrix} = \widehat{i}(-2 - 3) - \widehat{j}(0 + 3) + \widehat{k}(0 - 1) = -5\widehat{i} - 3\widehat{j} - \widehat{k}.$$ Thus the direction of the altitude is parallel to $$\overrightarrow{N} = -5\widehat{i} - 3\widehat{j} - \widehat{k}$$, and its parametric equation from D is $$\overrightarrow{Q}(s) = \overrightarrow{D} + s\,\overrightarrow{N} = (x\widehat{i} + y\widehat{j} + z\widehat{k}) + s(-5\widehat{i} - 3\widehat{j} - \widehat{k}) = (x - 5s)\widehat{i} + (y - 3s)\widehat{j} + (z - s)\widehat{k}.$$
The intersection point of the altitude and the median satisfies $$(x - 5s)\widehat{i} + (y - 3s)\widehat{j} + (z - s)\widehat{k} = \Bigl(1 + \tfrac{t}{2}\Bigr)\widehat{i} + 2\widehat{j} + \Bigl(1 - \tfrac{5t}{2}\Bigr)\widehat{k},$$ so equating components gives $$x - 5s = 1 + \tfrac{t}{2},\quad y - 3s = 2,\quad z - s = 1 - \tfrac{5t}{2}.$$ From $$y - 3s = 2$$ we get $$y = 2 + 3s$$. Defining $$u = x - 1,\ v = y - 2,\ w = z - 1$$, then $$v = 3s$$. From $$x - 5s = 1 + t/2$$ we have $$u - 5s = t/2\implies t = 2(u - 5s)$$, and from $$z - s = 1 - 5t/2$$ we obtain $$w - s = -5t/2$$. Substituting $$t = 2(u - 5s)$$ yields $$w - s = -5(u - 5s)\implies w = -5u + 26s.$$
The volume of the tetrahedron is $$\tfrac{\sqrt{805}}{6\sqrt{2}}$$, so the scalar triple product satisfies $$\bigl|\overrightarrow{AD}\cdot(\overrightarrow{AB}\times\overrightarrow{AC})\bigr| = \bigl|-5u - 3v - w\bigr| = \frac{\sqrt{805}}{\sqrt{2}} = \sqrt{\tfrac{805}{2}}.$$ Substituting $$v = 3s$$ and $$w = -5u + 26s$$ gives $$S = -5u - 9s + 5u - 26s = -35s,\quad |S| = 35|s| = \sqrt{\tfrac{805}{2}},$$ so $$1225s^2 = \frac{805}{2}\implies s^2 = \frac{23}{70}.$$
The distance $$AD$$ is $$\tfrac{\sqrt{110}}{3}$$, hence $$|\overrightarrow{AD}|^2 = u^2 + v^2 + w^2 = u^2 + 9s^2 + (-5u + 26s)^2 = \frac{110}{9}.$$ Expanding yields $$26u^2 - 260us + 685s^2 = \frac{110}{9},$$ and substituting $$s^2 = \frac{23}{70}$$ gives the quadratic $$252u^2 - 2520su + 2063 = 0.$$
Solving for $$u$$: $$u = \frac{2520s \pm \sqrt{(2520s)^2 - 4\cdot252\cdot2063}}{504} = \frac{2520s \pm 84}{504} = 5s \pm \tfrac{1}{6}.$$ Thus $$u = 5s + \tfrac{1}{6}$$ or $$u = 5s - \tfrac{1}{6}$$, giving $$t = \tfrac{1}{3}$$ or $$t = -\tfrac{1}{3}$$ respectively.
The intersection point $$P$$ on the median is then: for $$t = \tfrac{1}{3}$$, $$\overrightarrow{P} = \tfrac{1}{6}(7\widehat{i} + 12\widehat{j} + \widehat{k});$$ for $$t = -\tfrac{1}{3}$$, $$\overrightarrow{P} = \tfrac{1}{6}(5\widehat{i} + 12\widehat{j} + 11\widehat{k}).$$ Comparing with the options shows that Option D, $$\tfrac{1}{6}(7\widehat{i} + 12\widehat{j} + \widehat{k})$$, matches the case $$t = \tfrac{1}{3}$$. Verification with $$AD$$ length and volume confirms consistency.
Final Answer: D. $$\frac{1}{6}\left(7\widehat{i}+12\widehat{j}+\widehat{k}\right)$$
Let P be the foot of the perpendicular from the point (1,2,2) on the line L: $$\frac{x-1}{1}=\frac{y+1}{-1}=\frac{z-2}{2}.$$ Let the line $$\vec{r}=(-\hat{i}+\hat{j}-2\hat{k})+\lambda(\hat{i}-\hat{j}+\hat{k}), \quad \lambda \in \mathbb{R},$$ intersect the line L at Q. Then $$2(PQ)^{2}$$ is equal to:
Line L: $$\frac{x-1}{1} = \frac{y+1}{-1} = \frac{z-2}{2} = t$$
Parametric form: $$(1+t, -1-t, 2+2t)$$
Finding P (foot of perpendicular from (1,2,2) to L):
Direction of L: $$\vec{d} = (1,-1,2)$$
Vector from point on L to (1,2,2): $$(1-(1+t), 2-(-1-t), 2-(2+2t)) = (-t, 3+t, -2t)$$
For perpendicularity: $$(-t)(1) + (3+t)(-1) + (-2t)(2) = 0$$
$$-t - 3 - t - 4t = 0$$
$$-6t - 3 = 0$$
$$t = -\frac{1}{2}$$
So $$P = \left(\frac{1}{2}, -\frac{1}{2}, 1\right)$$.
Finding Q (intersection of given line with L):
The second line: $$\vec{r} = (-1,1,-2) + \lambda(1,-1,1)$$, i.e., $$(-1+\lambda, 1-\lambda, -2+\lambda)$$
Setting equal to L's parametric form:
$$-1+\lambda = 1+t \Rightarrow \lambda = 2+t \quad ...(1)$$
$$1-\lambda = -1-t \Rightarrow \lambda = 2+t \quad ...(2)$$ ✓
$$-2+\lambda = 2+2t \quad ...(3)$$
From (1): $$\lambda = 2+t$$. Substituting in (3):
$$-2+2+t = 2+2t$$
$$t = -2$$
$$\lambda = 0$$
So $$Q = (-1, 1, -2)$$.
Verification on L: $$(1+(-2), -1-(-2), 2+2(-2)) = (-1, 1, -2)$$ ✓
Computing $$2(PQ)^2$$:
$$PQ = Q - P = \left(-1-\frac{1}{2}, 1+\frac{1}{2}, -2-1\right) = \left(-\frac{3}{2}, \frac{3}{2}, -3\right)$$
$$(PQ)^2 = \frac{9}{4} + \frac{9}{4} + 9 = \frac{9}{4} + \frac{9}{4} + \frac{36}{4} = \frac{54}{4} = \frac{27}{2}$$
$$2(PQ)^2 = 2 \times \frac{27}{2} = 27$$
The correct answer is Option 4: 27.
Let $$\overrightarrow{a}=\hat{i}+2\hat{j}+\hat{k}$$ and $$\overrightarrow{b}=2\hat{i}+7hat{j}+3\hat{k}$$. Let $$L_{1}:\overrightarrow{r}=(-\hat{i}+2\hat{j}+\hat{k})+\lambda \overrightarrow{a},\lambda \in R$$. and $$L_{2}: \overrightarrow{r}=(\hat{j}+\hat{k})+\mu \overrightarrow{b}, \mu \in R$$ be two lines. If the line $$L_{3}$$ passes through the point of intersection of $$L_{1}$$ and $$L_{2}$$, and is parallel to $$\overrightarrow{a}+\overrightarrow{b}$$, then $$L_{3}$$ passes through the point :
We are given $$\vec{a} = \hat{i} + 2\hat{j} + \hat{k}$$ and $$\vec{b} = 2\hat{i} + 7\hat{j} + 3\hat{k}$$, and the lines:
$$L_1: \vec{r} = (-\hat{i} + 2\hat{j} + \hat{k}) + \lambda\vec{a}$$
$$L_2: \vec{r} = (\hat{j} + \hat{k}) + \mu\vec{b}$$
Line $$L_3$$ passes through the intersection of $$L_1$$ and $$L_2$$ and is parallel to $$\vec{a} + \vec{b}$$.
Points on $$L_1$$ are given by $$(-1+\lambda,\;2+2\lambda,\;1+\lambda)$$ and points on $$L_2$$ by $$(2\mu,\;1+7\mu,\;1+3\mu)$$. Setting these equal gives:
$$-1+\lambda = 2\mu\,,\quad 2+2\lambda = 1+7\mu\,,\quad 1+\lambda = 1+3\mu$$
From the third equation $$\lambda = 3\mu$$, and substituting into the first yields $$-1+3\mu = 2\mu\implies \mu = 1$$ and hence $$\lambda = 3$$. Verification in the second equation shows $$2+6=8$$ and $$1+7=8$$. The intersection point is therefore $$(-1+3,\;2+6,\;1+3) = (2,8,4)\,.$$
The direction of $$L_3$$ is the vector sum:
$$\vec{a} + \vec{b} = (1+2)\hat{i} + (2+7)\hat{j} + (1+3)\hat{k} = 3\hat{i} + 9\hat{j} + 4\hat{k}$$
The equation of $$L_3$$ can then be written in vector form as:
$$\vec{r} = (2\hat{i} + 8\hat{j} + 4\hat{k}) + t\,(3\hat{i} + 9\hat{j} + 4\hat{k})$$
with parametric form $$(2+3t,\;8+9t,\;4+4t)\,.$$
Checking which point lies on $$L_3$$, for $$(8,26,12)$$ we have $$2+3t=8\implies t=2$$, and then $$8+18=26$$ and $$4+8=12$$, so the choice is consistent. Thus the correct answer is Option 3: $$(8,26,12)\,.$$
Let $$\overrightarrow{r}=2\hat{i}-\hat{j}+3\hat{k}, \overrightarrow{c}=3\hat{i}-5\hat{j}+\hat{k}$$ and $$\overrightarrow{c}$$ be a vector such that $$\overrightarrow{c} \times \overrightarrow{c} = \overrightarrow{c} \times \overrightarrow{b}$$ and $$(\overrightarrow{a}+\overrightarrow{c}).(\overrightarrow{b}.\overrightarrow{c})=168$$. Then the maximum value of $$|\overrightarrow{c}|^{2}$$ is :
Given vectors are $$\overrightarrow{a} = 2\hat{i} - \hat{j} + 3\hat{k}$$ and $$\overrightarrow{b} = 3\hat{i} - 5\hat{j} + \hat{k}$$. The conditions are:
1. $$\overrightarrow{a} \times \overrightarrow{c} = \overrightarrow{c} \times \overrightarrow{b}$$
2. $$(\overrightarrow{a} + \overrightarrow{c}) \cdot (\overrightarrow{b} \cdot \overrightarrow{c}) = 168$$, but this appears to have a typo. Given the context and solution, it is interpreted as $$(\overrightarrow{a} + \overrightarrow{c}) \cdot (\overrightarrow{b} + \overrightarrow{c}) = 168$$.
From the first condition:
$$\overrightarrow{a} \times \overrightarrow{c} = \overrightarrow{c} \times \overrightarrow{b}$$
Since $$\overrightarrow{c} \times \overrightarrow{b} = - \overrightarrow{b} \times \overrightarrow{c}$$, we have:
$$\overrightarrow{a} \times \overrightarrow{c} = - \overrightarrow{b} \times \overrightarrow{c}$$
$$\overrightarrow{a} \times \overrightarrow{c} + \overrightarrow{b} \times \overrightarrow{c} = \overrightarrow{0}$$
$$(\overrightarrow{a} + \overrightarrow{b}) \times \overrightarrow{c} = \overrightarrow{0}$$
Thus, $$\overrightarrow{c}$$ is parallel to $$\overrightarrow{a} + \overrightarrow{b}$$.
Compute $$\overrightarrow{a} + \overrightarrow{b}$$:
$$\overrightarrow{a} + \overrightarrow{b} = (2 + 3)\hat{i} + (-1 - 5)\hat{j} + (3 + 1)\hat{k} = 5\hat{i} - 6\hat{j} + 4\hat{k}$$
Let $$\overrightarrow{d} = 5\hat{i} - 6\hat{j} + 4\hat{k}$$, so $$\overrightarrow{c} = k \overrightarrow{d} = k(5\hat{i} - 6\hat{j} + 4\hat{k})$$ for some scalar $$k$$.
Now, the second condition is $$(\overrightarrow{a} + \overrightarrow{c}) \cdot (\overrightarrow{b} + \overrightarrow{c}) = 168$$.
Substitute $$\overrightarrow{c} = k(5\hat{i} - 6\hat{j} + 4\hat{k})$$:
$$\overrightarrow{a} + \overrightarrow{c} = (2 + 5k)\hat{i} + (-1 - 6k)\hat{j} + (3 + 4k)\hat{k}$$
$$\overrightarrow{b} + \overrightarrow{c} = (3 + 5k)\hat{i} + (-5 - 6k)\hat{j} + (1 + 4k)\hat{k}$$
Dot product:
$$(\overrightarrow{a} + \overrightarrow{c}) \cdot (\overrightarrow{b} + \overrightarrow{c}) = (2 + 5k)(3 + 5k) + (-1 - 6k)(-5 - 6k) + (3 + 4k)(1 + 4k)$$
Expand each term:
$$(2 + 5k)(3 + 5k) = 2 \cdot 3 + 2 \cdot 5k + 5k \cdot 3 + 5k \cdot 5k = 6 + 10k + 15k + 25k^2 = 6 + 25k + 25k^2$$
$$(-1 - 6k)(-5 - 6k) = (-1)(-5) + (-1)(-6k) + (-6k)(-5) + (-6k)(-6k) = 5 + 6k + 30k + 36k^2 = 5 + 36k + 36k^2$$
$$(3 + 4k)(1 + 4k) = 3 \cdot 1 + 3 \cdot 4k + 4k \cdot 1 + 4k \cdot 4k = 3 + 12k + 4k + 16k^2 = 3 + 16k + 16k^2$$
Sum the expressions:
$$(6 + 5 + 3) + (25k + 36k + 16k) + (25k^2 + 36k^2 + 16k^2) = 14 + 77k + 77k^2$$
Set equal to 168:
$$77k^2 + 77k + 14 = 168$$
$$77k^2 + 77k - 154 = 0$$
Divide by 77:
$$k^2 + k - 2 = 0$$
Solve the quadratic equation:
Discriminant $$D = 1^2 - 4 \cdot 1 \cdot (-2) = 1 + 8 = 9$$
$$k = \frac{-1 \pm \sqrt{9}}{2} = \frac{-1 \pm 3}{2}$$
So, $$k = \frac{-1 + 3}{2} = 1$$ or $$k = \frac{-1 - 3}{2} = -2$$
Now, $$|\overrightarrow{c}|^2 = k^2 |\overrightarrow{d}|^2$$
$$|\overrightarrow{d}|^2 = 5^2 + (-6)^2 + 4^2 = 25 + 36 + 16 = 77$$
For $$k = 1$$, $$|\overrightarrow{c}|^2 = (1)^2 \cdot 77 = 77$$
For $$k = -2$$, $$|\overrightarrow{c}|^2 = (-2)^2 \cdot 77 = 4 \cdot 77 = 308$$
The maximum value is 308.
Verify the second condition for both values:
For $$k = 1$$, $$\overrightarrow{c} = 5\hat{i} - 6\hat{j} + 4\hat{k}$$
$$\overrightarrow{a} + \overrightarrow{c} = (2 + 5)\hat{i} + (-1 - 6)\hat{j} + (3 + 4)\hat{k} = 7\hat{i} - 7\hat{j} + 7\hat{k}$$
$$\overrightarrow{b} + \overrightarrow{c} = (3 + 5)\hat{i} + (-5 - 6)\hat{j} + (1 + 4)\hat{k} = 8\hat{i} - 11\hat{j} + 5\hat{k}$$
Dot product: $$7 \cdot 8 + (-7) \cdot (-11) + 7 \cdot 5 = 56 + 77 + 35 = 168$$
For $$k = -2$$, $$\overrightarrow{c} = -10\hat{i} + 12\hat{j} - 8\hat{k}$$
$$\overrightarrow{a} + \overrightarrow{c} = (2 - 10)\hat{i} + (-1 + 12)\hat{j} + (3 - 8)\hat{k} = -8\hat{i} + 11\hat{j} - 5\hat{k}$$
$$\overrightarrow{b} + \overrightarrow{c} = (3 - 10)\hat{i} + (-5 + 12)\hat{j} + (1 - 8)\hat{k} = -7\hat{i} + 7\hat{j} - 7\hat{k}$$
Dot product: $$(-8) \cdot (-7) + 11 \cdot 7 + (-5) \cdot (-7) = 56 + 77 + 35 = 168$$
Both satisfy the second condition, and the first condition is satisfied since $$\overrightarrow{c}$$ is parallel to $$\overrightarrow{a} + \overrightarrow{b}$$ for both $$k$$. The maximum value of $$|\overrightarrow{c}|^2$$ is 308.
Final Answer: 308
Let $$\vec{a} = \hat{i} + 2\hat{j} + \hat{k}$$ and $$\vec{b} = 2\hat{i} + \hat{j} - \hat{k}$$. Let $$\hat{c}$$ be a unit vector in the plane of the vectors $$\vec{a}$$ and $$\vec{b}$$ and be perpendicular to $$\vec{a}$$. Then such a vector $$\hat{c}$$ is :
We want a unit vector $$\hat{c}$$ which
• lies in the plane of $$\vec{a}$$ and $$\vec{b}$$ (so it is a linear combination of them), and
• is perpendicular to $$\vec{a}$$.
Write $$\vec{a} = \hat{i} + 2\hat{j} + \hat{k}$$ and $$\vec{b} = 2\hat{i} + \hat{j} - \hat{k}$$.
A convenient way to obtain a vector lying in the required plane and orthogonal to $$\vec{a}$$ is to remove from $$\vec{b}$$ its component along $$\vec{a}$$. The result is automatically in the span of $$\vec{a},\vec{b}$$ and perpendicular to $$\vec{a}$$.
First compute the projection of $$\vec{b}$$ on $$\vec{a}$$.
Formula: projection of $$\vec{b}$$ on $$\vec{a}$$ is $$\displaystyle\frac{\vec{a}\cdot\vec{b}}{\vec{a}\cdot\vec{a}}\;\vec{a}$$.
Dot products:
$$\vec{a}\cdot\vec{b} = 1\cdot2 + 2\cdot1 + 1\cdot(-1) = 2 + 2 - 1 = 3$$
$$\vec{a}\cdot\vec{a} = 1^2 + 2^2 + 1^2 = 1 + 4 + 1 = 6$$
Hence the projection is
$$\frac{3}{6}\,\vec{a} = \frac{1}{2}\,( \hat{i} + 2\hat{j} + \hat{k}) = 0.5\,\hat{i} + 1\,\hat{j} + 0.5\,\hat{k}$$.
Subtract this from $$\vec{b}$$ to get the component of $$\vec{b}$$ perpendicular to $$\vec{a}$$:
$$\vec{d} = \vec{b} - \text{proj}_{\vec{a}}\vec{b}$$
$$= (2,\,1,\,-1) - (0.5,\,1,\,0.5)$$
$$= (1.5,\,0,\,-1.5)$$.
Multiply by $$2$$ to clear the decimal:
$$\vec{d} = (3,\,0,\,-3) = 3(1,\,0,\,-1).$$
Any non-zero scalar multiple of $$\vec{d}$$ is still in the same direction, so we choose the simple vector
$$\vec{m} = (1,\,0,\,-1) = \hat{i} - \hat{k}$$.
Check orthogonality with $$\vec{a}$$:
$$(\hat{i} - \hat{k})\cdot(\hat{i} + 2\hat{j} + \hat{k}) = 1 - 1 = 0,$$
so it is indeed perpendicular to $$\vec{a}$$.
Now normalise to get a unit vector:
Magnitude of $$\vec{m}$$:
$$|\vec{m}| = \sqrt{1^2 + 0^2 + (-1)^2} = \sqrt{2}$$.
Hence
$$\hat{c} = \frac{\vec{m}}{|\vec{m}|} = \frac{1}{\sqrt{2}}(\hat{i} - \hat{k}).$$
The negative of a unit vector is also a valid unit vector, so $$-\hat{c} = \dfrac{1}{\sqrt{2}}(-\hat{i} + \hat{k})$$ is equally acceptable.
Comparing with the options, Option D gives $$\dfrac{1}{\sqrt{2}}(-\hat{i} + \hat{k})$$, which matches (up to sign).
Therefore the required vector is given by Option D.
Let $$\vec{p} = 2\hat{i} + \hat{j} + 3\hat{k}$$ and $$\vec{q} = \hat{i} - \hat{j} + \hat{k}$$. If for some real numbers $$\alpha$$, $$\beta$$ and $$\gamma$$, we have $$15\hat{i} + 10\hat{j} + 6\hat{k} = \alpha(2\vec{p} + \vec{q}) + \beta(\vec{p} - 2\vec{q}) + \gamma(\vec{p} \times \vec{q})$$, then the value of $$\gamma$$ is ______.
Write the given vectors in component form:
$$\vec{p}=2\hat i+\hat j+3\hat k \; \rightarrow \; (2,1,3), \qquad
\vec{q}=\hat i-\hat j+\hat k \; \rightarrow \; (1,-1,1).$$
First compute the three auxiliary vectors that appear on the right-hand side.
1. Vector $$2\vec p+\vec q$$
$$2\vec p=(4,2,6) \quad\Longrightarrow\quad
2\vec p+\vec q=(4+1,\,2+(-1),\,6+1)=(5,1,7).$$
2. Vector $$\vec p-2\vec q$$
$$2\vec q=(2,-2,2) \quad\Longrightarrow\quad
\vec p-2\vec q=(2-2,\,1-(-2),\,3-2)=(0,3,1).$$
3. Vector $$\vec p\times\vec q$$
Using the determinant rule:
$$
\vec p\times\vec q=
\begin{vmatrix}
\hat i & \hat j & \hat k\\
2 & 1 & 3\\
1 & -1 & 1
\end{vmatrix}
= \hat i(1\cdot1-3\cdot(-1))-\hat j(2\cdot1-3\cdot1)+\hat k(2\cdot(-1)-1\cdot1)
=4\hat i+\hat j-3\hat k.
$$
Thus $$\vec p\times\vec q=(4,1,-3).$$
Denote
$$\vec a_1=(5,1,7),\qquad \vec a_2=(0,3,1),\qquad \vec a_3=(4,1,-3).$$
The equation in component form becomes
$$\alpha\vec a_1+\beta\vec a_2+\gamma\vec a_3=(15,10,6).$$
Equate the $$\hat i, \hat j, \hat k$$ components:
$$5\alpha+4\gamma=15 \quad-(1)$$
$$\alpha+3\beta+\gamma=10 \quad-(2)$$
$$7\alpha+\beta-3\gamma=6 \quad-(3)$$
Solve sequentially. From $$(1):$$
$$\alpha=\frac{15-4\gamma}{5}=3-0.8\gamma.$$
Substitute this $$\alpha$$ into $$(2):$$
$$(3-0.8\gamma)+3\beta+\gamma=10 \;\Longrightarrow\; 3\beta=7-0.2\gamma,$$
so $$\beta=\dfrac{7-0.2\gamma}{3}.$$
Now use $$(3):$$
$$7\alpha+\beta-3\gamma=6.$$
Insert $$\alpha=3-0.8\gamma$$ and the above $$\beta$$:
$$7(3-0.8\gamma)+\beta-3\gamma=6$$ $$\Longrightarrow 21-5.6\gamma+\beta-3\gamma=6$$ $$\Longrightarrow \beta+21-8.6\gamma=6$$ $$\Longrightarrow \beta=-15+8.6\gamma.$$
Equate the two expressions for $$\beta$$:
$$\frac{7-0.2\gamma}{3}=-15+8.6\gamma.$$ Multiply by 3: $$7-0.2\gamma=-45+25.8\gamma$$ $$\Longrightarrow 52=26\gamma$$ $$\Longrightarrow \gamma=2.$$
Hence, the required value is $$\boxed{2}$$.
Let $$\overrightarrow{OP} = \frac{\alpha - 1}{\alpha}\hat{i} + \hat{j} + \hat{k}$$, $$\overrightarrow{OQ} = \hat{i} + \frac{\beta - 1}{\beta}\hat{j} + \hat{k}$$ and $$\overrightarrow{OR} = \hat{i} + \hat{j} + \frac{1}{2}\hat{k}$$ be three vectors, where $$\alpha, \beta \in \mathbb{R} - \{0\}$$ and $$O$$ denotes the origin. If $$(\overrightarrow{OP} \times \overrightarrow{OQ}) \cdot \overrightarrow{OR} = 0$$ and the point $$(\alpha, \beta, 2)$$ lies on the plane $$3x + 3y - z + l = 0$$, then the value of $$l$$ is ________.
The components of the three position vectors are
$$\overrightarrow{OP} = \left( \frac{\alpha-1}{\alpha},\, 1,\, 1 \right),\;
\overrightarrow{OQ} = \left( 1,\, \frac{\beta-1}{\beta},\, 1 \right),\;
\overrightarrow{OR} = \left( 1,\, 1,\, \frac12 \right).$$
For any three vectors $$\mathbf{a},\mathbf{b},\mathbf{c}$$ originating from one point, the scalar triple product is the determinant of the matrix formed by their components:
$$(\mathbf{a}\times\mathbf{b})\cdot\mathbf{c}=
\begin{vmatrix}
a_x & a_y & a_z \\
b_x & b_y & b_z \\
c_x & c_y & c_z
\end{vmatrix}.$$
Using $$\mathbf{a}=\overrightarrow{OP},\;\mathbf{b}=\overrightarrow{OQ},\;\mathbf{c}=\overrightarrow{OR}$$ we get
$$ \begin{vmatrix} \dfrac{\alpha-1}{\alpha} & 1 & 1 \\[4pt] 1 & \dfrac{\beta-1}{\beta} & 1 \\[4pt] 1 & 1 & \dfrac12 \end{vmatrix}=0.$$ Denote $$A = 1-\frac1{\alpha},\qquad B = 1-\frac1{\beta};$$ then the determinant becomes
$$ \begin{vmatrix} A & 1 & 1 \\ 1 & B & 1 \\ 1 & 1 & \dfrac12 \end{vmatrix}=0.$$ Expanding along the first row:
$$ A\!\left(B\cdot\frac12-1\cdot1\right) -\;1\!\left(1\cdot\frac12-1\cdot1\right) +\;1\!\left(1\cdot1-B\cdot1\right)=0. $$
Simplifying each term:
$$A\!\left(\frac{B}{2}-1\right)+\frac12+(1-B)=0,$$
so
$$A\!\left(\frac{B}{2}-1\right)+\frac32-B=0.$$
Substitute $$A=1-\dfrac1\alpha,\;B=1-\dfrac1\beta$$:
$$ \left(1-\frac1\alpha\right)\!\left(\frac12-\frac1{2\beta}-1\right)+\frac32-\left(1-\frac1\beta\right)=0. $$ First bracket: $$\frac12-\frac1{2\beta}-1=-\frac12-\frac1{2\beta}.$$
Hence
$$-\left(1-\frac1\alpha\right)\!\left(\frac12+\frac1{2\beta}\right)+\frac12+\frac1\beta=0.$$
Multiply throughout by $$2\beta$$ to clear denominators:
$$-\left(1-\frac1\alpha\right)(\beta+1)+\beta+2=0.$$
Expand:
$$-(\beta+1)+\frac{\beta+1}{\alpha}+\beta+2=0.$$
Combining like terms:
$$1+\frac{\beta+1}{\alpha}=0\;\;\Longrightarrow\;\;\frac{\beta+1}{\alpha}=-1
\;\;\Longrightarrow\;\;\beta=-\alpha-1.$$
The point $$(\alpha,\beta,2)$$ lies on the plane $$3x+3y-z+l=0$$, so
$$3\alpha+3\beta-2+l=0.$$
Using $$\beta=-\alpha-1$$:
$$3\alpha+3(-\alpha-1)-2+l=0
\;\Longrightarrow\;-5+l=0
\;\Longrightarrow\;l=5.$$
Therefore, the required value is 5.
If $$A(1, -1, 2), B(5, 7, -6), C(3, 4, -10)$$ and $$D(-1, -4, -2)$$ are the vertices of a quadrilateral $$ABCD$$, then its area is :
We are given $$A(1, -1, 2)$$, $$B(5, 7, -6)$$, $$C(3, 4, -10)$$, $$D(-1, -4, -2)$$.
First, let us check whether $$ABCD$$ is a parallelogram by computing the midpoints of the diagonals.
Midpoint of $$AC = \left(\frac{1+3}{2}, \frac{-1+4}{2}, \frac{2+(-10)}{2}\right) = (2, 1.5, -4)$$
Midpoint of $$BD = \left(\frac{5+(-1)}{2}, \frac{7+(-4)}{2}, \frac{-6+(-2)}{2}\right) = (2, 1.5, -4)$$
Since both diagonals have the same midpoint, $$ABCD$$ is a parallelogram.
For a parallelogram, the area can be computed using the diagonal vectors with the formula:
$$\text{Area} = \frac{1}{2}|\overrightarrow{AC} \times \overrightarrow{BD}|$$
Computing the diagonal vectors:
$$\overrightarrow{AC} = C - A = (3-1, 4-(-1), -10-2) = (2, 5, -12)$$
$$\overrightarrow{BD} = D - B = (-1-5, -4-7, -2-(-6)) = (-6, -11, 4)$$
Now compute the cross product $$\overrightarrow{AC} \times \overrightarrow{BD}$$:
$$\overrightarrow{AC} \times \overrightarrow{BD} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 5 & -12 \\ -6 & -11 & 4 \end{vmatrix}$$
$$\hat{i}$$-component: $$5 \times 4 - (-12) \times (-11) = 20 - 132 = -112$$
$$\hat{j}$$-component: $$-(2 \times 4 - (-12) \times (-6)) = -(8 - 72) = 64$$
$$\hat{k}$$-component: $$2 \times (-11) - 5 \times (-6) = -22 + 30 = 8$$
So $$\overrightarrow{AC} \times \overrightarrow{BD} = (-112, 64, 8)$$.
$$|\overrightarrow{AC} \times \overrightarrow{BD}| = \sqrt{(-112)^2 + 64^2 + 8^2}$$
$$= \sqrt{12544 + 4096 + 64}$$
$$= \sqrt{16704}$$
Let us simplify $$\sqrt{16704}$$. We find: $$16704 = 576 \times 29$$, since $$576 = 24^2$$ and $$576 \times 29 = 16704$$.
$$\sqrt{16704} = 24\sqrt{29}$$
Therefore, the area of the parallelogram $$ABCD$$ is:
$$\text{Area} = \frac{1}{2} \times 24\sqrt{29} = 12\sqrt{29}$$
The answer is Option B: $$12\sqrt{29}$$.
If $$A(3, 1, -1)$$, $$B\left(\frac{5}{3}, \frac{7}{3}, \frac{1}{3}\right)$$, $$C(2, 2, 1)$$ and $$D\left(\frac{10}{3}, \frac{2}{3}, \frac{-1}{3}\right)$$ are the vertices of a quadrilateral $$ABCD$$, then its area is
We are given $$A(3, 1, -1)$$, $$B\left(\frac{5}{3}, \frac{7}{3}, \frac{1}{3}\right)$$, $$C(2, 2, 1)$$, $$D\left(\frac{10}{3}, \frac{2}{3}, -\frac{1}{3}\right)$$.
First, let us check whether $$ABCD$$ is a parallelogram by computing the side vectors:
$$\overrightarrow{AB} = B - A = \left(\frac{5}{3} - 3, \frac{7}{3} - 1, \frac{1}{3} + 1\right) = \left(-\frac{4}{3}, \frac{4}{3}, \frac{4}{3}\right)$$
$$\overrightarrow{DC} = C - D = \left(2 - \frac{10}{3}, 2 - \frac{2}{3}, 1 + \frac{1}{3}\right) = \left(-\frac{4}{3}, \frac{4}{3}, \frac{4}{3}\right)$$
Since $$\overrightarrow{AB} = \overrightarrow{DC}$$, the quadrilateral $$ABCD$$ is a parallelogram.
For a parallelogram with adjacent sides $$\overrightarrow{AB}$$ and $$\overrightarrow{AD}$$, the area is $$|\overrightarrow{AB} \times \overrightarrow{AD}|$$.
Computing $$\overrightarrow{AD}$$:
$$\overrightarrow{AD} = D - A = \left(\frac{10}{3} - 3, \frac{2}{3} - 1, -\frac{1}{3} + 1\right) = \left(\frac{1}{3}, -\frac{1}{3}, \frac{2}{3}\right)$$
Computing the cross product $$\overrightarrow{AB} \times \overrightarrow{AD}$$:
$$\overrightarrow{AB} \times \overrightarrow{AD} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -\frac{4}{3} & \frac{4}{3} & \frac{4}{3} \\ \frac{1}{3} & -\frac{1}{3} & \frac{2}{3} \end{vmatrix}$$
$$\hat{i}$$: $$\frac{4}{3} \cdot \frac{2}{3} - \frac{4}{3} \cdot \left(-\frac{1}{3}\right) = \frac{8}{9} + \frac{4}{9} = \frac{12}{9} = \frac{4}{3}$$
$$\hat{j}$$: $$-\left[\left(-\frac{4}{3}\right)\left(\frac{2}{3}\right) - \frac{4}{3} \cdot \frac{1}{3}\right] = -\left[-\frac{8}{9} - \frac{4}{9}\right] = -\left(-\frac{12}{9}\right) = \frac{4}{3}$$
$$\hat{k}$$: $$\left(-\frac{4}{3}\right)\left(-\frac{1}{3}\right) - \frac{4}{3} \cdot \frac{1}{3} = \frac{4}{9} - \frac{4}{9} = 0$$
So $$\overrightarrow{AB} \times \overrightarrow{AD} = \left(\frac{4}{3}, \frac{4}{3}, 0\right)$$.
$$|\overrightarrow{AB} \times \overrightarrow{AD}| = \sqrt{\left(\frac{4}{3}\right)^2 + \left(\frac{4}{3}\right)^2 + 0} = \frac{4}{3}\sqrt{2}$$
Therefore, the area of the parallelogram $$ABCD$$ is:
$$\text{Area} = \frac{4\sqrt{2}}{3}$$
The answer is Option D: $$\frac{4\sqrt{2}}{3}$$.
Between the following two statements: Statement I : Let $$\vec{a} = \hat{i} + 2\hat{j} - 3\hat{k}$$ and $$\vec{b} = 2\hat{i} + \hat{j} - \hat{k}$$. Then the vector $$\vec{r}$$ satisfying $$\vec{a} \times \vec{r} = \vec{a} \times \vec{b}$$ and $$\vec{a} \cdot \vec{r} = 0$$ is of magnitude $$\sqrt{10}$$. Statement II : In a triangle $$ABC$$, $$\cos 2A + \cos 2B + \cos 2C \ge -\frac{3}{2}$$.
Statement I: $$\vec{a}=\hat{i}+2\hat{j}-3\hat{k}$$, $$\vec{b}=2\hat{i}+\hat{j}-\hat{k}$$. $$\vec{a}\times\vec{r}=\vec{a}\times\vec{b}$$ means $$\vec{a}\times(\vec{r}-\vec{b})=\vec{0}$$, so $$\vec{r}-\vec{b}=\lambda\vec{a}$$.
$$\vec{r}=\vec{b}+\lambda\vec{a}=(2+\lambda)\hat{i}+(1+2\lambda)\hat{j}+(-1-3\lambda)\hat{k}$$.
$$\vec{a}\cdot\vec{r}=0$$: $$(2+\lambda)+2(1+2\lambda)-3(-1-3\lambda)=0$$. $$2+\lambda+2+4\lambda+3+9\lambda=0$$. $$14\lambda+7=0$$, $$\lambda=-1/2$$.
$$\vec{r}=3/2\hat{i}+0\hat{j}+1/2\hat{k}$$. $$|\vec{r}|=\sqrt{9/4+1/4}=\sqrt{10/4}=\sqrt{10}/2$$.
$$|\vec{r}| = \sqrt{10}/2 \neq \sqrt{10}$$. Statement I is incorrect.
Statement II: $$\cos 2A+\cos 2B+\cos 2C \geq -3/2$$.
$$\cos 2A+\cos 2B+\cos 2C = -1-4\cos A\cos B\cos C$$. Min of $$-1-4\cos A\cos B\cos C$$: max of $$\cos A\cos B\cos C = 1/8$$ (at equilateral). Min = $$-1-4(1/8) = -3/2$$.
So $$\geq -3/2$$. Statement II is correct.
The correct answer is Option 1.
Consider three vectors $$\vec{a}, \vec{b}, \vec{c}$$. Let $$|\vec{a}| = 2, |\vec{b}| = 3$$ and $$\vec{a} = \vec{b} \times \vec{c}$$. If $$\alpha \in \left[0, \frac{\pi}{3}\right]$$ is the angle between the vectors $$\vec{b}$$ and $$\vec{c}$$, then the minimum value of $$27|\vec{c} - \vec{a}|^2$$ is equal to:
Given $$|\vec{a}| = 2$$, $$|\vec{b}| = 3$$, $$\vec{a} = \vec{b} \times \vec{c}$$, and $$\alpha \in [0, \pi/3]$$ is the angle between $$\vec{b}$$ and $$\vec{c}$$.
Since $$\vec{a} = \vec{b} \times \vec{c}$$, we have $$|\vec{a}| = |\vec{b}||\vec{c}|\sin\alpha$$.
$$ 2 = 3|\vec{c}|\sin\alpha \Rightarrow |\vec{c}| = \frac{2}{3\sin\alpha} $$Also, $$\vec{a} \perp \vec{b}$$ and $$\vec{a} \perp \vec{c}$$.
Compute $$|\vec{c} - \vec{a}|^2$$.
$$ |\vec{c} - \vec{a}|^2 = |\vec{c}|^2 - 2\vec{a} \cdot \vec{c} + |\vec{a}|^2 $$Since $$\vec{a} \perp \vec{c}$$: $$\vec{a} \cdot \vec{c} = 0$$.
$$ |\vec{c} - \vec{a}|^2 = |\vec{c}|^2 + 4 = \frac{4}{9\sin^2\alpha} + 4 $$ $$ 27|\vec{c} - \vec{a}|^2 = 27\left(\frac{4}{9\sin^2\alpha} + 4\right) = \frac{12}{\sin^2\alpha} + 108 $$Minimize over $$\alpha \in [0, \pi/3]$$.
$$\frac{12}{\sin^2\alpha}$$ is minimized when $$\sin^2\alpha$$ is maximized. On $$[0, \pi/3]$$, $$\sin\alpha$$ is increasing, so maximum at $$\alpha = \pi/3$$: $$\sin(\pi/3) = \frac{\sqrt{3}}{2}$$, $$\sin^2(\pi/3) = \frac{3}{4}$$.
$$ 27|\vec{c} - \vec{a}|^2_{\min} = \frac{12}{3/4} + 108 = 16 + 108 = 124 $$The correct answer is Option (2): 124.
Let $$A(2, 3, 5)$$ and $$C(-3, 4, -2)$$ be opposite vertices of a parallelogram $$ABCD$$ if the diagonal $$\vec{BD} = \hat{i} + 2\hat{j} + 3\hat{k}$$ then the area of the parallelogram is equal to
Finding Diagonal $$\vec{AC}$$
$$\vec{AC} = (-3-2)\hat{i} + (4-3)\hat{j} + (-2-5)\hat{k} = -5\hat{i} + \hat{j} - 7\hat{k}$$
Area $$= \frac{1}{2} |\vec{AC} \times \vec{BD}|$$
$$\vec{AC} \times \vec{BD} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -5 & 1 & -7 \\ 1 & 2 & 3 \end{vmatrix} = \hat{i}(3+14) - \hat{j}(-15+7) + \hat{k}(-10-1) = 17\hat{i} + 8\hat{j} - 11\hat{k}$$
• Magnitude $$= \sqrt{17^2 + 8^2 + (-11)^2} = \sqrt{289 + 64 + 121} = \sqrt{474}$$
• Area $$= \mathbf{\frac{1}{2}\sqrt{474}}$$ (Option B)
Let three vectors $$\vec{a} = \alpha\hat{i} + 4\hat{j} + 2\hat{k}$$, $$\vec{b} = 5\hat{i} + 3\hat{j} + 4\hat{k}$$, $$\vec{c} = x\hat{i} + y\hat{j} + z\hat{k}$$ form a triangle such that $$\vec{c} = \vec{a} - \vec{b}$$ and the area of the triangle is $$5\sqrt{6}$$. If $$\alpha$$ is a positive real number, then $$|\vec{c}|^2$$ is equal to:
$$\vec{c} = \vec{a} - \vec{b} = (\alpha-5)\hat{i} + \hat{j} - 2\hat{k}$$.
Area of triangle = $$\frac{1}{2}|\vec{a} \times \vec{b}| = 5\sqrt{6}$$, so $$|\vec{a} \times \vec{b}| = 10\sqrt{6}$$.
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \alpha & 4 & 2 \\ 5 & 3 & 4 \end{vmatrix} = (16-6)\hat{i} - (4\alpha-10)\hat{j} + (3\alpha-20)\hat{k}$$
$$= 10\hat{i} - (4\alpha-10)\hat{j} + (3\alpha-20)\hat{k}$$
$$|\vec{a} \times \vec{b}|^2 = 100 + (4\alpha-10)^2 + (3\alpha-20)^2 = 600$$
$$(4\alpha-10)^2 + (3\alpha-20)^2 = 500$$
$$16\alpha^2 - 80\alpha + 100 + 9\alpha^2 - 120\alpha + 400 = 500$$
$$25\alpha^2 - 200\alpha + 500 = 500$$
$$25\alpha^2 - 200\alpha = 0 \implies 25\alpha(\alpha - 8) = 0$$
Since $$\alpha > 0$$: $$\alpha = 8$$.
$$\vec{c} = (8-5)\hat{i} + \hat{j} - 2\hat{k} = 3\hat{i} + \hat{j} - 2\hat{k}$$.
$$|\vec{c}|^2 = 9 + 1 + 4 = 14$$.
The correct answer is Option 2: 14.
Let $$\vec{a} = 2\hat{i} + \hat{j} - \hat{k}$$, $$\vec{b} = ((\vec{a} \times (\hat{i} + \hat{j})) \times \hat{i}) \times \hat{i}$$. Then the square of the projection of $$\vec{a}$$ on $$\vec{b}$$ is :
Given $$\vec{a}=2\,\hat{i}+\,\hat{j}-\,\hat{k}$$ and $$\vec{b}=((\vec{a}\times(\hat{i}+\hat{j}))\times\hat{i})\times\hat{i}$$. We first evaluate the cross products one by one.
Step 1: Compute $$\vec{c}=\vec{a}\times(\hat{i}+\hat{j})$$.
Write $$\hat{i}+\hat{j}=(1,1,0)$$ and $$\vec{a}=(2,1,-1)$$.
Using the determinant formula for $$\vec{u}\times\vec{v}$$ :
$$\vec{c}=\begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\\ 2 & 1 & -1\\ 1 & 1 & 0 \end{vmatrix} =\hat{i}(1\cdot0-(-1)\cdot1)-\hat{j}(2\cdot0-(-1)\cdot1)+\hat{k}(2\cdot1-1\cdot1)$$
$$\Rightarrow\;\vec{c}=1\,\hat{i}-1\,\hat{j}+1\,\hat{k}=(1,-1,1)$$.
Step 2: Compute $$\vec{d}=\vec{c}\times\hat{i}$$.
Take $$\hat{i}=(1,0,0)$$:
$$\vec{d}=\begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\\ 1 & -1 & 1\\ 1 & 0 & 0 \end{vmatrix} =\hat{i}((-1)\cdot0-1\cdot0)-\hat{j}(1\cdot0-1\cdot1)+\hat{k}(1\cdot0-(-1)\cdot1)$$
$$\Rightarrow\;\vec{d}=0\,\hat{i}+1\,\hat{j}+1\,\hat{k}=(0,1,1)$$.
Step 3: Compute $$\vec{b}=\vec{d}\times\hat{i}$$.
Again cross with $$\hat{i}=(1,0,0)$$ :
$$\vec{b}=\begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\\ 0 & 1 & 1\\ 1 & 0 & 0 \end{vmatrix} =\hat{i}(1\cdot0-1\cdot0)-\hat{j}(0\cdot0-1\cdot1)+\hat{k}(0\cdot0-1\cdot1)$$
$$\Rightarrow\;\vec{b}=0\,\hat{i}+1\,\hat{j}-1\,\hat{k}=(0,1,-1)$$.
Step 4: Square of the projection of $$\vec{a}$$ on $$\vec{b}$$.
Projection length formula: the component of $$\vec{a}$$ along $$\vec{b}$$ is $$\dfrac{\vec{a}\cdot\vec{b}}{\lvert\vec{b}\rvert}$$. Hence
$$\text{(projection)}^{2}=\dfrac{(\vec{a}\cdot\vec{b})^{2}}{\lvert\vec{b}\rvert^{2}}$$.
Dot product: $$\vec{a}\cdot\vec{b}=(2,1,-1)\cdot(0,1,-1)=0+1+1=2$$.
Magnitude squared of $$\vec{b}$$: $$\lvert\vec{b}\rvert^{2}=0^{2}+1^{2}+(-1)^{2}=2$$.
Therefore $$\text{(projection)}^{2}=\dfrac{2^{2}}{2}=2$$.
Hence the square of the projection of $$\vec{a}$$ on $$\vec{b}$$ is $$2$$, which matches Option C.
Let $$\vec{a} = 3\hat{i} + \hat{j} - 2\hat{k}$$, $$\vec{b} = 4\hat{i} + \hat{j} + 7\hat{k}$$ and $$\vec{c} = \hat{i} - 3\hat{j} + 4\hat{k}$$ be three vectors. If a vector $$\vec{p}$$ satisfies $$\vec{p} \times \vec{b} = \vec{c} \times \vec{b}$$ and $$\vec{p} \cdot \vec{a} = 0$$, then $$\vec{p} \cdot (\hat{i} - \hat{j} - \hat{k})$$ is equal to
$$\vec{p}\times\vec{b}=\vec{c}\times\vec{b}$$, so $$(\vec{p}-\vec{c})\times\vec{b}=0$$, meaning $$\vec{p}-\vec{c}=\lambda\vec{b}$$.
$$\vec{p}=\vec{c}+\lambda\vec{b}=(1+4\lambda)\hat{i}+(-3+\lambda)\hat{j}+(4+7\lambda)\hat{k}$$.
$$\vec{p}\cdot\vec{a}=0$$: $$3(1+4\lambda)+1(-3+\lambda)-2(4+7\lambda)=0$$.
$$3+12\lambda-3+\lambda-8-14\lambda=0 \Rightarrow -\lambda-8=0 \Rightarrow \lambda=-8$$.
$$\vec{p}=(-31)\hat{i}+(-11)\hat{j}+(-52)\hat{k}$$.
$$\vec{p}\cdot(\hat{i}-\hat{j}-\hat{k})=-31+11+52=32$$.
The answer is Option (4): $$\boxed{32}$$.
Let $$\vec{a} = 4\hat{i} - \hat{j} + \hat{k}$$, $$\vec{b} = 11\hat{i} - \hat{j} + \hat{k}$$ and $$\vec{c}$$ be a vector such that $$(\vec{a} + \vec{b}) \times \vec{c} = \vec{c} \times (-2\vec{a} + 3\vec{b})$$. If $$(2\vec{a} + 3\vec{b}) \cdot \vec{c} = 1670$$, then $$|\vec{c}|^2$$ is equal to :
Given $$\vec{a} = 4\hat{i} - \hat{j} + \hat{k}$$, $$\vec{b} = 11\hat{i} - \hat{j} + \hat{k}$$, and $$(\vec{a}+\vec{b}) \times \vec{c} = \vec{c} \times(-2\vec{a}+3\vec{b})$$.
We use the fact that
$$\vec{c} \times(-2\vec{a}+3\vec{b}) = -(-2\vec{a}+3\vec{b}) \times \vec{c}$$.
Hence
$$ (\vec{a}+\vec{b}) \times \vec{c} + (-2\vec{a}+3\vec{b}) \times \vec{c} = \vec{0} $$
Applying the distributive property of the cross product leads to
$$ ((\vec{a}+\vec{b}) + (-2\vec{a}+3\vec{b})) \times \vec{c} = \vec{0} $$
which simplifies to
$$ (-\vec{a}+4\vec{b}) \times \vec{c} = \vec{0}. $$
Therefore, $$\vec{c}$$ must be parallel to $$(-\vec{a}+4\vec{b})$$.
Substituting the component forms gives
$$ -\vec{a} + 4\vec{b} = -(4\hat{i}-\hat{j}+\hat{k}) + 4(11\hat{i}-\hat{j}+\hat{k}) = -4\hat{i}+\hat{j}-\hat{k}+44\hat{i}-4\hat{j}+4\hat{k} = 40\hat{i}-3\hat{j}+3\hat{k}. $$
Thus we can write $$\vec{c} = t(40\hat{i}-3\hat{j}+3\hat{k})$$ for some scalar $$t$$.
Using the condition $$(2\vec{a}+3\vec{b}) \cdot \vec{c} = 1670$$ we compute
$$ 2\vec{a} + 3\vec{b} = 2(4\hat{i}-\hat{j}+\hat{k}) + 3(11\hat{i}-\hat{j}+\hat{k}) = 8\hat{i}-2\hat{j}+2\hat{k}+33\hat{i}-3\hat{j}+3\hat{k} = 41\hat{i}-5\hat{j}+5\hat{k}. $$
Substitution into the dot product yields
$$ (41\hat{i}-5\hat{j}+5\hat{k}) \cdot t(40\hat{i}-3\hat{j}+3\hat{k}) = 1670. $$
This simplifies to
$$ t(41 \times 40 + (-5)(-3) + 5 \times 3) = 1670, $$
so
$$ t(1640 + 15 + 15) = 1670, $$
giving
$$ t \times 1670 = 1670 \implies t = 1. $$
Therefore $$\vec{c} = 40\hat{i}-3\hat{j}+3\hat{k}$$ and its squared magnitude is
$$ |\vec{c}|^2 = 40^2 + 3^2 + 3^2 = 1600 + 9 + 9 = 1618. $$
The correct answer is Option 2: 1618.
Let $$\vec{a} = \hat{i} + \alpha\hat{j} + \beta\hat{k}$$, $$\alpha, \beta \in R$$. Let a vector $$\vec{b}$$ be such that the angle between $$\vec{a}$$ and $$\vec{b}$$ is $$\frac{\pi}{4}$$ and $$|\vec{b}|^2 = 6$$. If $$\vec{a} \cdot \vec{b} = 3\sqrt{2}$$, then the value of $$(\alpha^2 + \beta^2)|\vec{a} \times \vec{b}|^2$$ is equal to
$$|\vec{a}|^2 = 1 + \alpha^2 + \beta^2$$. $$|\vec{b}|^2 = 6$$. $$\vec{a} \cdot \vec{b} = 3\sqrt{2}$$.
Angle $$\pi/4$$ between $$\vec{a}$$ and $$\vec{b}$$: $$\cos(\pi/4) = \frac{\vec{a}\cdot\vec{b}}{|\vec{a}||\vec{b}|} = \frac{3\sqrt{2}}{|\vec{a}|\sqrt{6}}$$.
$$\frac{1}{\sqrt{2}} = \frac{3\sqrt{2}}{|\vec{a}|\sqrt{6}} \Rightarrow |\vec{a}|\sqrt{6} = 3\sqrt{2} \cdot \sqrt{2} = 6 \Rightarrow |\vec{a}| = \sqrt{6}$$.
So $$1 + \alpha^2 + \beta^2 = 6 \Rightarrow \alpha^2 + \beta^2 = 5$$.
$$|\vec{a} \times \vec{b}|^2 = |\vec{a}|^2|\vec{b}|^2 - (\vec{a}\cdot\vec{b})^2 = 36 - 18 = 18$$.
$$(\alpha^2 + \beta^2)|\vec{a} \times \vec{b}|^2 = 5 \times 18 = 90$$.
The answer is Option (1): $$\boxed{90}$$.
Let $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be three non-zero vectors such that $$\vec{b}$$ and $$\vec{c}$$ are non-collinear. If $$\vec{a} + 5\vec{b}$$ is collinear with $$\vec{c}$$, $$\vec{b} + 6\vec{c}$$ is collinear with $$\vec{a}$$ and $$\vec{a} + \alpha\vec{b} + \beta\vec{c} = \vec{0}$$, then $$\alpha + \beta$$ is equal to
$$\vec{a} + 5\vec{b}$$ is collinear with $$\vec{c}$$, and $$\vec{b} + 6\vec{c}$$ is collinear with $$\vec{a}$$. Also $$\vec{a} + \alpha\vec{b} + \beta\vec{c} = \vec{0}$$.
Express the collinearity conditions.
Since $$\vec{a} + 5\vec{b}$$ is collinear with $$\vec{c}$$:
$$\vec{a} + 5\vec{b} = \lambda\vec{c}$$ for some scalar $$\lambda$$ ... (i)
Since $$\vec{b} + 6\vec{c}$$ is collinear with $$\vec{a}$$:
$$\vec{b} + 6\vec{c} = \mu\vec{a}$$ for some scalar $$\mu$$ ... (ii)
Express $$\vec{a}$$ from equation (ii).
$$\vec{a} = \frac{1}{\mu}\vec{b} + \frac{6}{\mu}\vec{c}$$
Substitute into equation (i).
$$\frac{1}{\mu}\vec{b} + \frac{6}{\mu}\vec{c} + 5\vec{b} = \lambda\vec{c}$$
$$\left(\frac{1}{\mu} + 5\right)\vec{b} + \left(\frac{6}{\mu} - \lambda\right)\vec{c} = \vec{0}$$
Since $$\vec{b}$$ and $$\vec{c}$$ are non-collinear, both coefficients must be zero:
$$\frac{1}{\mu} + 5 = 0 \implies \mu = -\frac{1}{5}$$
$$\frac{6}{\mu} = \lambda \implies \lambda = 6 \times (-5) = -30$$
Find $$\alpha$$ and $$\beta$$.
From (i): $$\vec{a} = -5\vec{b} + \lambda\vec{c} = -5\vec{b} - 30\vec{c}$$
So $$\vec{a} + 5\vec{b} + 30\vec{c} = \vec{0}$$
Therefore $$\alpha = 5$$ and $$\beta = 30$$.
$$\alpha + \beta = 5 + 30 = 35$$
The answer is Option 1: 35.
Let $$\vec{OA} = \vec{a}, \vec{OB} = 12\vec{a} + 4\vec{b}$$ and $$\vec{OC} = \vec{b}$$, where $$O$$ is the origin. If $$S$$ is the parallelogram with adjacent sides $$OA$$ and $$OC$$, then $$\frac{\text{area of the quadrilateral } OABC}{\text{area of } S}$$ is equal to _____
We need to find the ratio of the area of quadrilateral $$OABC$$ to the area of parallelogram $$S$$ with adjacent sides $$OA$$ and $$OC$$.
$$\vec{OA} = \vec{a}$$, $$\vec{OB} = 12\vec{a} + 4\vec{b}$$, $$\vec{OC} = \vec{b}$$, where $$O$$ is the origin.
$$S$$ has adjacent sides $$\vec{OA} = \vec{a}$$ and $$\vec{OC} = \vec{b}$$:
$$\text{Area of } S = |\vec{a} \times \vec{b}|$$
The area of quadrilateral $$OABC$$ with vertices in order $$O, A, B, C$$ can be computed by splitting into triangles $$OAB$$ and $$OBC$$:
$$\text{Area}(OABC) = \text{Area}(OAB) + \text{Area}(OBC)$$
$$\text{Area}(OAB) = \frac{1}{2}|\vec{OA} \times \vec{OB}| = \frac{1}{2}|\vec{a} \times (12\vec{a} + 4\vec{b})| = \frac{1}{2}|12(\vec{a} \times \vec{a}) + 4(\vec{a} \times \vec{b})| = \frac{1}{2} \cdot 4|\vec{a} \times \vec{b}| = 2|\vec{a} \times \vec{b}|$$
$$\text{Area}(OBC) = \frac{1}{2}|\vec{OB} \times \vec{OC}| = \frac{1}{2}|(12\vec{a} + 4\vec{b}) \times \vec{b}| = \frac{1}{2}|12(\vec{a} \times \vec{b}) + 4(\vec{b} \times \vec{b})| = \frac{1}{2} \cdot 12|\vec{a} \times \vec{b}| = 6|\vec{a} \times \vec{b}|$$
$$\text{Area}(OABC) = 2|\vec{a} \times \vec{b}| + 6|\vec{a} \times \vec{b}| = 8|\vec{a} \times \vec{b}|$$
$$\frac{\text{Area}(OABC)}{\text{Area}(S)} = \frac{8|\vec{a} \times \vec{b}|}{|\vec{a} \times \vec{b}|} = 8$$
The correct answer is Option (4): 8.
If $$\vec{a} = \hat{i} + 2\hat{j} + \hat{k}$$, $$\vec{b} = 3(\hat{i} - \hat{j} + \hat{k})$$ and $$\vec{c}$$ be the vector such that $$\vec{a} \times \vec{c} = \vec{b}$$ and $$\vec{a} \cdot \vec{c} = 3$$, then $$\vec{a} \cdot ((\vec{c} \times \vec{b}) - \vec{b} - \vec{c})$$ is equal to
We are given
$$\vec{a}=1\,\hat{i}+2\,\hat{j}+1\,\hat{k},\qquad
\vec{b}=3(\hat{i}-\hat{j}+\hat{k})=3\,\hat{i}-3\,\hat{j}+3\,\hat{k}.$$
Let $$\vec{c}=x\,\hat{i}+y\,\hat{j}+z\,\hat{k}.$$
The two conditions on $$\vec{c}$$ are
1. $$\vec{a}\times\vec{c}=\vec{b}$$
2. $$\vec{a}\cdot\vec{c}=3$$
Case 1: Solve $$\vec{a}\times\vec{c}=\vec{b}.$$ Using the determinant rule for a cross product,
$$\vec{a}\times\vec{c}= \begin{vmatrix} \hat{i}&\hat{j}&\hat{k}\\ 1&2&1\\ x&y&z \end{vmatrix} =\hat{i}(2z-y)-\hat{j}(z-x)+\hat{k}(y-2x).$$
Equating components with $$\vec{b}=(3,\,-3,\,3),$$ we obtain
$$2z-y=3\quad -(1)$$
$$-(z-x)=-3\;\Longrightarrow\; z-x=3\quad -(2)$$
$$y-2x=3\quad -(3)$$
Case 2: Solve $$\vec{a}\cdot\vec{c}=3.$$ The dot product gives
$$1\cdot x+2\cdot y+1\cdot z=3\quad -(4)$$
From $$(2)$$ we get $$x=z-3.$$
From $$(1)$$ we get $$y=2z-3.$$
Substitute these in $$(4):$$
$$(z-3)+2(2z-3)+z=3$$
$$z-3+4z-6+z=3$$
$$6z-9=3$$
$$6z=12\;\Longrightarrow\; z=2.$$
Hence
$$x=z-3=2-3=-1,\qquad y=2z-3=4-3=1.$$
Therefore $$\vec{c}=-1\,\hat{i}+1\,\hat{j}+2\,\hat{k}.$$
Case 3: Evaluate the required expression $$\vec{a}\cdot\bigl((\vec{c}\times\vec{b})-\vec{b}-\vec{c}\bigr).$$
First compute $$\vec{c}\times\vec{b}:$$
$$\vec{c}\times\vec{b}= \begin{vmatrix} \hat{i}&\hat{j}&\hat{k}\\ -1&1&2\\ 3&-3&3 \end{vmatrix} =\hat{i}(1\cdot3-2\cdot(-3)) -\hat{j}((-1)\cdot3-2\cdot3) +\hat{k}((-1)(-3)-1\cdot3)$$
$$=\hat{i}(3+6)-\hat{j}(-3-6)+\hat{k}(3-3) =9\,\hat{i}+9\,\hat{j}+0\,\hat{k}.$$
Now form the vector inside the parentheses:
$$(\vec{c}\times\vec{b})-\vec{b}-\vec{c} =(9,9,0)-(3,-3,3)-(-1,1,2)$$
$$=(9-3+1,\;9+3-1,\;0-3-2) =(7,\;11,\;-5).$$
Finally take the dot product with $$\vec{a}=(1,2,1)\!:\!$$
$$\vec{a}\cdot(7,11,-5)=1\cdot7+2\cdot11+1\cdot(-5)=7+22-5=24.$$
Hence the value of $$\vec{a}\cdot\bigl((\vec{c}\times\vec{b})-\vec{b}-\vec{c}\bigr)=24.$$
Therefore, the correct option is Option B (24).
Let a unit vector $$\hat{u} = x\hat{i} + y\hat{j} + z\hat{k}$$ make angles $$\frac{\pi}{2}, \frac{\pi}{3}$$ and $$\frac{2\pi}{3}$$ with the vectors $$\frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{k}, \frac{1}{\sqrt{2}}\hat{j} + \frac{1}{\sqrt{2}}\hat{k}$$ and $$\frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{j}$$ respectively. If $$\vec{v} = \frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{j} + \frac{1}{\sqrt{2}}\hat{k}$$, then $$|\hat{u} - \vec{v}|^2$$ is equal to
Let $$\hat{u} = x\hat{i} + y\hat{j} + z\hat{k}$$ be a unit vector making the given angles with the three vectors. The three given vectors are already unit vectors (each has magnitude 1), so using the dot product to express each angle gives the following equations.
For the angle $$\frac{\pi}{2}$$ with $$\frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{k}$$, we have $$ \frac{x + z}{\sqrt{2}} = \cos\frac{\pi}{2} = 0 \implies x + z = 0 \quad \cdots(1) $$. For the angle $$\frac{\pi}{3}$$ with $$\frac{1}{\sqrt{2}}\hat{j} + \frac{1}{\sqrt{2}}\hat{k}$$, $$ \frac{y + z}{\sqrt{2}} = \cos\frac{\pi}{3} = \frac{1}{2} \implies y + z = \frac{1}{\sqrt{2}} \quad \cdots(2)$$. For the angle $$\frac{2\pi}{3}$$ with $$\frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{j}$$, $$ \frac{x + y}{\sqrt{2}} = \cos\frac{2\pi}{3} = -\frac{1}{2} \implies x + y = -\frac{1}{\sqrt{2}} \quad \cdots(3)$$.
From (1), $$z = -x$$. Substituting into (2) gives $$y - x = \frac{1}{\sqrt{2}} \quad \cdots(4)$$, and (3) states $$x + y = -\frac{1}{\sqrt{2}} \quad \cdots(5)$$. Adding (4) and (5) yields $$2y = 0 \implies y = 0$$. Then (5) implies $$x = -\frac{1}{\sqrt{2}}$$ and (1) gives $$z = \frac{1}{\sqrt{2}}$$, so $$\hat{u} = -\frac{1}{\sqrt{2}}\hat{i} + 0\hat{j} + \frac{1}{\sqrt{2}}\hat{k}$$.
To compute $$|\hat{u} - \vec{v}|^2$$ where $$\vec{v} = \frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{j} + \frac{1}{\sqrt{2}}\hat{k}$$, note that
$$\hat{u} - \vec{v} = \left(-\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}\right)\hat{i} + \left(0 - \frac{1}{\sqrt{2}}\right)\hat{j} + \left(\frac{1}{\sqrt{2}} - \frac{1}{\sqrt{2}}\right)\hat{k}$$
$$= -\sqrt{2}\,\hat{i} - \frac{1}{\sqrt{2}}\hat{j} + 0\hat{k}$$
$$ |\hat{u} - \vec{v}|^2 = 2 + \frac{1}{2} + 0 = \frac{5}{2} $$. Thus the correct answer is Option (2): $$\frac{5}{2}$$.
Let a unit vector which makes an angle of 60° with $$2\hat{i} + 2\hat{j} - \hat{k}$$ and angle 45° with $$\hat{i} - \hat{k}$$ be $$\overrightarrow{C}$$. Then $$\overrightarrow{C} + \left(-\frac{1}{2}\hat{i} + \frac{1}{3\sqrt{2}}\hat{j} - \frac{\sqrt{2}}{3}\hat{k}\right)$$ is:
We need to find a unit vector $$\overrightarrow{C} = x\hat{i} + y\hat{j} + z\hat{k}$$ such that it makes an angle of 60° with $$\overrightarrow{a} = 2\hat{i} + 2\hat{j} - \hat{k}$$ and an angle of 45° with $$\overrightarrow{b} = \hat{i} - \hat{k}$$.
Since $$\overrightarrow{C}$$ is a unit vector, we have:
$$ x^2 + y^2 + z^2 = 1 \quad \cdots(1) $$
Condition 1: Angle with $$\overrightarrow{a}$$ is 60°.
$$|\overrightarrow{a}| = \sqrt{4 + 4 + 1} = 3$$
$$ \cos 60° = \frac{\overrightarrow{C} \cdot \overrightarrow{a}}{|\overrightarrow{C}||\overrightarrow{a}|} = \frac{2x + 2y - z}{3} $$
$$ \frac{1}{2} = \frac{2x + 2y - z}{3} \implies 2x + 2y - z = \frac{3}{2} \quad \cdots(2) $$
Condition 2: Angle with $$\overrightarrow{b}$$ is 45°.
$$|\overrightarrow{b}| = \sqrt{1 + 1} = \sqrt{2}$$
$$ \cos 45° = \frac{\overrightarrow{C} \cdot \overrightarrow{b}}{|\overrightarrow{C}||\overrightarrow{b}|} = \frac{x - z}{\sqrt{2}} $$
$$ \frac{1}{\sqrt{2}} = \frac{x - z}{\sqrt{2}} \implies x - z = 1 \quad \cdots(3) $$
From (3): $$z = x - 1$$. Substituting into (2):
$$ 2x + 2y - (x - 1) = \frac{3}{2} \implies x + 2y + 1 = \frac{3}{2} \implies x = \frac{1}{2} - 2y \quad \cdots(4) $$
Also, $$z = x - 1 = -\frac{1}{2} - 2y$$. Substituting into (1):
$$ \left(\frac{1}{2} - 2y\right)^2 + y^2 + \left(-\frac{1}{2} - 2y\right)^2 = 1 $$
$$ \frac{1}{4} - 2y + 4y^2 + y^2 + \frac{1}{4} + 2y + 4y^2 = 1 $$
$$ 9y^2 + \frac{1}{2} = 1 \implies y^2 = \frac{1}{18} \implies y = \pm \frac{1}{3\sqrt{2}} $$
Case 1: $$y = \frac{1}{3\sqrt{2}}$$, then $$x = \frac{1}{2} - \frac{\sqrt{2}}{3}$$, $$z = -\frac{1}{2} - \frac{\sqrt{2}}{3}$$.
Case 2: $$y = -\frac{1}{3\sqrt{2}}$$, then $$x = \frac{1}{2} + \frac{\sqrt{2}}{3}$$, $$z = -\frac{1}{2} + \frac{\sqrt{2}}{3}$$.
Now compute $$\overrightarrow{C} + \left(-\frac{1}{2}\hat{i} + \frac{1}{3\sqrt{2}}\hat{j} - \frac{\sqrt{2}}{3}\hat{k}\right)$$ for each case.
Case 2 check:
$$i$$-component: $$\frac{1}{2} + \frac{\sqrt{2}}{3} - \frac{1}{2} = \frac{\sqrt{2}}{3}$$
$$j$$-component: $$-\frac{1}{3\sqrt{2}} + \frac{1}{3\sqrt{2}} = 0$$
$$k$$-component: $$-\frac{1}{2} + \frac{\sqrt{2}}{3} - \frac{\sqrt{2}}{3} = -\frac{1}{2}$$
This gives $$\frac{\sqrt{2}}{3}\hat{i} - \frac{1}{2}\hat{k}$$, which matches Option 1.
Hence the correct answer is Option 1.
Let $$O$$ be the origin and the position vector of $$A$$ and $$B$$ be $$2\hat{i} + 2\hat{j} + \hat{k}$$ and $$2\hat{i} + 4\hat{j} + 4\hat{k}$$ respectively. If the internal bisector of $$\angle AOB$$ meets the line $$AB$$ at $$C$$, then the length of $$OC$$ is
We need to find the length of $$OC$$, where $$C$$ is the point where the internal bisector of $$\angle AOB$$ meets line $$AB$$.
Find the position vectors and distances.
$$\vec{OA} = 2\hat{i} + 2\hat{j} + \hat{k}$$, so $$|\vec{OA}| = \sqrt{4+4+1} = 3$$
$$\vec{OB} = 2\hat{i} + 4\hat{j} + 4\hat{k}$$, so $$|\vec{OB}| = \sqrt{4+16+16} = 6$$
Apply the angle bisector theorem.
By the angle bisector theorem, the internal bisector of $$\angle AOB$$ divides $$AB$$ in the ratio $$OA:OB = 3:6 = 1:2$$.
Find the position vector of $$C$$.
Using the section formula (internal division in ratio $$1:2$$):
$$\vec{OC} = \frac{1 \cdot \vec{OB} + 2 \cdot \vec{OA}}{1 + 2} = \frac{(2\hat{i}+4\hat{j}+4\hat{k}) + 2(2\hat{i}+2\hat{j}+\hat{k})}{3}$$
$$= \frac{(2+4)\hat{i} + (4+4)\hat{j} + (4+2)\hat{k}}{3} = \frac{6\hat{i} + 8\hat{j} + 6\hat{k}}{3} = 2\hat{i} + \frac{8}{3}\hat{j} + 2\hat{k}$$
Calculate $$|OC|$$.
$$|OC| = \sqrt{4 + \frac{64}{9} + 4} = \sqrt{8 + \frac{64}{9}} = \sqrt{\frac{72 + 64}{9}} = \sqrt{\frac{136}{9}} = \frac{\sqrt{136}}{3} = \frac{2\sqrt{34}}{3}$$
The correct answer is Option (2): $$\frac{2}{3}\sqrt{34}$$.
Let the position vectors of the vertices A, B and C of a triangle be $$2\hat{i} + 2\hat{j} + \hat{k}$$, $$\hat{i} + 2\hat{j} + 2\hat{k}$$ and $$2\hat{i} + \hat{j} + 2\hat{k}$$ respectively. Let $$l_1, l_2$$ and $$l_3$$ be the lengths of perpendiculars drawn from the ortho centre of the triangle on the sides AB, BC and CA respectively, then $$l_1^2 + l_2^2 + l_3^2$$ equals :
$$A(2,2,1)$$, $$B(1,2,2)$$, $$C(2,1,2)$$.
$$AB = \sqrt{1+0+1} = \sqrt{2}$$, $$BC = \sqrt{1+1+0} = \sqrt{2}$$, $$CA = \sqrt{0+1+1} = \sqrt{2}$$.
The triangle is equilateral. For an equilateral triangle, the orthocenter coincides with the centroid.
Centroid/orthocenter: $$H = \left(\frac{5}{3}, \frac{5}{3}, \frac{5}{3}\right)$$.
For an equilateral triangle with side $$a = \sqrt{2}$$, the distance from the center to any side is $$h/3$$ where $$h = \frac{\sqrt{3}}{2}a$$ is the height. So distance = $$\frac{a}{2\sqrt{3}} = \frac{\sqrt{2}}{2\sqrt{3}} = \frac{1}{\sqrt{6}}$$.
All three perpendicular distances are equal: $$l_1 = l_2 = l_3 = \frac{1}{\sqrt{6}}$$.
$$l_1^2 + l_2^2 + l_3^2 = 3 \times \frac{1}{6} = \frac{1}{2}$$.
The answer corresponds to Option (2).
Let $$\vec{a} = 2\hat{i} + 5\hat{j} - \hat{k}$$, $$\vec{b} = 2\hat{i} - 2\hat{j} + 2\hat{k}$$ and $$\vec{c}$$ be three vectors such that $$(\vec{c} + \hat{i}) \times (\vec{a} + \vec{b} + \hat{i}) = \vec{a} \times (\vec{c} + \hat{i})$$. If $$\vec{a} \cdot \vec{c} = -29$$, then $$\vec{c} \cdot (-2\hat{i} + \hat{j} + \hat{k})$$ is equal to:
Given $$\vec{a} = 2\hat{i} + 5\hat{j} - \hat{k}$$, $$\vec{b} = 2\hat{i} - 2\hat{j} + 2\hat{k}$$, and:
$$ (\vec{c} + \hat{i}) \times (\vec{a} + \vec{b} + \hat{i}) = \vec{a} \times (\vec{c} + \hat{i}) $$Let $$\vec{d} = \vec{c} + \hat{i}$$. Using $$\vec{a} \times \vec{d} = -\vec{d} \times \vec{a}$$:
$$ \vec{d} \times (\vec{a} + \vec{b} + \hat{i}) = -\vec{d} \times \vec{a} $$ $$ \vec{d} \times (2\vec{a} + \vec{b} + \hat{i}) = \vec{0} $$So $$\vec{d}$$ is parallel to $$2\vec{a} + \vec{b} + \hat{i}$$.
$$2\vec{a} + \vec{b} + \hat{i} = 7\hat{i} + 8\hat{j}$$.
So $$\vec{d} = \lambda(7\hat{i} + 8\hat{j})$$ and $$\vec{c} = (7\lambda - 1)\hat{i} + 8\lambda\hat{j}$$.
Using $$\vec{a} \cdot \vec{c} = -29$$:
$$ 2(7\lambda - 1) + 5(8\lambda) = -29 \implies 54\lambda - 2 = -29 \implies \lambda = -\frac{1}{2} $$$$\vec{c} = -\frac{9}{2}\hat{i} - 4\hat{j}$$.
$$\vec{c} \cdot (-2\hat{i} + \hat{j} + \hat{k}) = 9 - 4 + 0 = 5$$.
The correct answer is Option 4: 5.
Let $$\vec{a} = 2\hat{i} + \alpha\hat{j} + \hat{k}, \vec{b} = -\hat{i} + \hat{k}, \vec{c} = \beta\hat{j} - \hat{k}$$, where $$\alpha$$ and $$\beta$$ are integers and $$\alpha\beta = -6$$. Let the values of the ordered pair $$(\alpha, \beta)$$, for which the area of the parallelogram of diagonals $$\vec{a} + \vec{b}$$ and $$\vec{b} + \vec{c}$$ is $$\frac{\sqrt{21}}{2}$$, be $$(\alpha_1, \beta_1)$$ and $$(\alpha_2, \beta_2)$$. Then $$\alpha_1^2 + \beta_1^2 - \alpha_2\beta_2$$ is equal to
Given: $$\vec{a} = 2\hat{i} + \alpha\hat{j} + \hat{k}$$, $$\vec{b} = -\hat{i} + \hat{k}$$, $$\vec{c} = \beta\hat{j} - \hat{k}$$, with $$\alpha\beta = -6$$.
Diagonals: $$\vec{a} + \vec{b} = (1, \alpha, 2)$$ and $$\vec{b} + \vec{c} = (-1, \beta, 0)$$.
Area of parallelogram with diagonals $$\vec{d_1}$$ and $$\vec{d_2}$$ = $$\frac{1}{2}|\vec{d_1} \times \vec{d_2}|$$.
$$\vec{d_1} \times \vec{d_2} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & \alpha & 2 \\ -1 & \beta & 0 \end{vmatrix} = \hat{i}(0-2\beta) - \hat{j}(0+2) + \hat{k}(\beta+\alpha)$$
$$= (-2\beta, -2, \alpha+\beta)$$
$$|\vec{d_1} \times \vec{d_2}|^2 = 4\beta^2 + 4 + (\alpha+\beta)^2$$
Area = $$\frac{\sqrt{21}}{2}$$, so $$\frac{1}{4}[4\beta^2 + 4 + (\alpha+\beta)^2] = \frac{21}{4}$$.
$$4\beta^2 + 4 + \alpha^2 + 2\alpha\beta + \beta^2 = 21$$
$$\alpha^2 + 5\beta^2 + 2(-6) + 4 = 21$$ (using $$\alpha\beta = -6$$)
$$\alpha^2 + 5\beta^2 = 29$$
With $$\alpha\beta = -6$$ (integer solutions): possible $$(\alpha, \beta)$$ pairs: $$(1$$, $$-6)$$, $$(-1$$, $$6)$$, $$(2$$, $$-3)$$, $$(-2$$, $$3)$$, $$(3$$, $$-2)$$, $$(-3$$, $$2)$$, $$(6$$, $$-1)$$, $$(-6$$, $$1)$$.
Check $$\alpha^2 + 5\beta^2 = 29$$:
$$(\alpha_1, \beta_1) = (3, -2)$$ and $$(\alpha_2, \beta_2) = (-3, 2)$$.
$$\alpha_1^2 + \beta_1^2 - \alpha_2\beta_2 = 9 + 4 - (-3)(2) = 13 + 6 = 19$$.
The correct answer is Option A: 19
Let $$\vec{a} = -5\hat{i} + \hat{j} - 3\hat{k}$$, $$\vec{b} = \hat{i} + 2\hat{j} - 4\hat{k}$$ and $$\vec{c} = ((\vec{a} \times \vec{b}) \times \hat{i}) \times \hat{i}) \times \hat{i}$$. Then $$\vec{c} \cdot (-\hat{i} + \hat{j} + \hat{k})$$ is equal to:
Given vectors are:
$$\vec{a} = -5\hat{i} + \hat{j} - 3\hat{k}$$
$$\vec{b} = \hat{i} + 2\hat{j} - 4\hat{k}$$
We need to find $$\vec{c} = ((\vec{a} \times \vec{b}) \times \hat{i}) \times \hat{i}) \times \hat{i}$$ and then compute $$\vec{c} \cdot (-\hat{i} + \hat{j} + \hat{k})$$.
First, compute $$\vec{d} = \vec{a} \times \vec{b}$$ using the cross product formula:
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -5 & 1 & -3 \\ 1 & 2 & -4 \\ \end{vmatrix}$$
Expanding the determinant:
$$\hat{i} \left( (1)(-4) - (-3)(2) \right) - \hat{j} \left( (-5)(-4) - (-3)(1) \right) + \hat{k} \left( (-5)(2) - (1)(1) \right)$$
Calculate each component:
- $$\hat{i}$$ component: $$(1)(-4) - (-3)(2) = -4 + 6 = 2$$
- $$\hat{j}$$ component: $$- \left[ (-5)(-4) - (-3)(1) \right] = - \left[ 20 + 3 \right] = -23$$
- $$\hat{k}$$ component: $$(-5)(2) - (1)(1) = -10 - 1 = -11$$
So, $$\vec{d} = 2\hat{i} - 23\hat{j} - 11\hat{k}$$
Next, compute $$\vec{e} = \vec{d} \times \hat{i}$$. The cross product of any vector $$\vec{u} = u_x \hat{i} + u_y \hat{j} + u_z \hat{k}$$ with $$\hat{i}$$ is given by:
$$\vec{u} \times \hat{i} = (u_z) \hat{j} + (-u_y) \hat{k}$$
Here, $$\vec{d} = 2\hat{i} - 23\hat{j} - 11\hat{k}$$, so $$u_x = 2$$, $$u_y = -23$$, $$u_z = -11$$.
Thus, $$\vec{e} = (-11) \hat{j} + (-(-23)) \hat{k} = -11\hat{j} + 23\hat{k}$$
Now, compute $$\vec{f} = \vec{e} \times \hat{i}$$ using the same formula:
$$\vec{e} = 0\hat{i} -11\hat{j} + 23\hat{k}$$, so $$u_x = 0$$, $$u_y = -11$$, $$u_z = 23$$.
Thus, $$\vec{f} = (23) \hat{j} + (-(-11)) \hat{k} = 23\hat{j} + 11\hat{k}$$
Finally, compute $$\vec{c} = \vec{f} \times \hat{i}$$:
$$\vec{f} = 0\hat{i} + 23\hat{j} + 11\hat{k}$$, so $$u_x = 0$$, $$u_y = 23$$, $$u_z = 11$$.
Thus, $$\vec{c} = (11) \hat{j} + (-23) \hat{k} = 11\hat{j} - 23\hat{k}$$
Now, compute the dot product $$\vec{c} \cdot (-\hat{i} + \hat{j} + \hat{k})$$:
$$\vec{c} = 0\hat{i} + 11\hat{j} - 23\hat{k}$$
Dot product: $$(0)(-1) + (11)(1) + (-23)(1) = 0 + 11 - 23 = -12$$
Therefore, the value is $$-12$$, which corresponds to option A.
Let $$\vec{a} = 6\hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j}$$. If $$\vec{c}$$ is a vector such that $$|\vec{c}| \geq 6$$, $$\vec{a} \cdot \vec{c} = 6|\vec{c}|$$, $$|\vec{c} - \vec{a}| = 2\sqrt{2}$$ and the angle between $$\vec{a} \times \vec{b}$$ and $$\vec{c}$$ is $$60°$$, then $$|(\vec{a} \times \vec{b}) \times \vec{c}|$$ is equal to:
|a| = √(36+1+1) = √38. a·c = 6|c|: cos θ_ac = 6/√38.
|c-a|² = |c|²-2a·c+|a|² = |c|²-12|c|+38 = 8. So |c|²-12|c|+30 = 0. |c| = (12±√(144-120))/2 = (12±√24)/2 = 6±√6. Since |c|≥6: |c| = 6+√6.
a×b = |i j k; 6 1 -1; 1 1 0| = (0+1)i-(-1+0... = i-(-1)j+(6-1)k... Let me compute: = (0+1)i-(0+1)j+(6-1)k = i-j+5k. |a×b| = √(1+1+25) = √27 = 3√3.
|(a×b)×c| = |a×b|·|c|·sin60° = 3√3·(6+√6)·(√3/2) = (9/2)(6+√6).
The correct answer is Option (3): 9(6+√6)/2.
Let $$\vec{a} = a_1\hat{i} + a_2\hat{j} + a_3\hat{k}$$ and $$\vec{b} = b_1\hat{i} + b_2\hat{j} + b_3\hat{k}$$ be two vectors such that $$|\vec{a}| = 1$$; $$\vec{a} \cdot \vec{b} = 2$$ and $$|\vec{b}| = 4$$. If $$\vec{c} = 2(\vec{a} \times \vec{b}) - 3\vec{b}$$, then the angle between $$\vec{b}$$ and $$\vec{c}$$ is equal to :
Given $$|\vec{a}| = 1$$, $$\vec{a} \cdot \vec{b} = 2$$, $$|\vec{b}| = 4$$, and $$\vec{c} = 2(\vec{a} \times \vec{b}) - 3\vec{b}$$.
First, find $$\vec{b} \cdot \vec{c}$$:
$$\vec{b} \cdot \vec{c} = 2\vec{b} \cdot (\vec{a} \times \vec{b}) - 3|\vec{b}|^2 = 0 - 3(16) = -48$$
(since $$\vec{b} \cdot (\vec{a} \times \vec{b}) = 0$$)
Now find $$|\vec{c}|^2$$:
$$|\vec{c}|^2 = 4|\vec{a} \times \vec{b}|^2 - 12(\vec{a} \times \vec{b}) \cdot \vec{b} + 9|\vec{b}|^2$$
$$= 4|\vec{a} \times \vec{b}|^2 + 144$$
We need $$|\vec{a} \times \vec{b}|^2 = |\vec{a}|^2|\vec{b}|^2 - (\vec{a} \cdot \vec{b})^2 = 16 - 4 = 12$$.
$$|\vec{c}|^2 = 48 + 144 = 192$$
$$\cos\theta = \frac{\vec{b} \cdot \vec{c}}{|\vec{b}||\vec{c}|} = \frac{-48}{4\sqrt{192}} = \frac{-48}{4 \cdot 8\sqrt{3}} = \frac{-48}{32\sqrt{3}} = \frac{-3}{2\sqrt{3}} = \frac{-\sqrt{3}}{2}$$
$$\theta = \cos^{-1}\left(-\frac{\sqrt{3}}{2}\right) = 150°$$
The answer is Option (3): $$\boxed{\cos^{-1}\left(-\frac{\sqrt{3}}{2}\right)}$$.
Let $$\vec{a}$$ and $$\vec{b}$$ be two vectors such that $$|\vec{b}| = 1$$ and $$|\vec{b} \times \vec{a}| = 2$$. Then $$|(\vec{b} \times \vec{a}) - \vec{b}|^2$$ is equal to
$$|\vec{b}| = 1$$, $$|\vec{b} \times \vec{a}| = 2$$.
$$|(\vec{b} \times \vec{a}) - \vec{b}|^2 = |\vec{b} \times \vec{a}|^2 - 2(\vec{b} \times \vec{a}) \cdot \vec{b} + |\vec{b}|^2$$
Since $$(\vec{b} \times \vec{a}) \perp \vec{b}$$: $$(\vec{b} \times \vec{a}) \cdot \vec{b} = 0$$.
$$= 4 + 0 + 1 = 5$$.
The answer is Option (2): $$\boxed{5}$$.
Let $$\vec{a} = \hat{i} + 2\hat{j} + 3\hat{k}$$, $$\vec{b} = 2\hat{i} + 3\hat{j} - 5\hat{k}$$ and $$\vec{c} = 3\hat{i} - \hat{j} + \lambda\hat{k}$$ be three vectors. Let $$\vec{r}$$ be a unit vector along $$\vec{b} + \vec{c}$$. If $$\vec{r} \cdot \vec{a} = 3$$, then $$3\lambda$$ is equal to :
We are given $$\vec{a} = \hat{i} + 2\hat{j} + 3\hat{k}, \quad \vec{b} = 2\hat{i} + 3\hat{j} - 5\hat{k}, \quad \vec{c} = 3\hat{i} - \hat{j} + \lambda\hat{k}$$.
We denote $$\vec{r}$$ as the unit vector along $$\vec{b} + \vec{c}$$ and use the condition $$\vec{r} \cdot \vec{a} = 3$$.
First, we compute $$\vec{b} + \vec{c}$$:
$$\vec{b}+\vec{c} = (2+3)\hat{i} + (3-1)\hat{j} + (-5+\lambda)\hat{k} = 5\hat{i} + 2\hat{j} + (\lambda-5)\hat{k}$$
Next, its magnitude is
$$|\vec{b} + \vec{c}| = \sqrt{25 + 4 + (\lambda - 5)^2} = \sqrt{29 + (\lambda - 5)^2}$$
Therefore the unit vector is
$$\vec{r} = \frac{5\hat{i} + 2\hat{j} + (\lambda - 5)\hat{k}}{\sqrt{29 + (\lambda - 5)^2}}$$.
Using the dot product condition gives
$$\vec{r} \cdot \vec{a} = \frac{5(1) + 2(2) + (\lambda - 5)(3)}{\sqrt{29 + (\lambda - 5)^2}} = \frac{5 + 4 + 3\lambda - 15}{\sqrt{29 + (\lambda - 5)^2}} = \frac{3\lambda - 6}{\sqrt{29 + (\lambda - 5)^2}} = 3$$
This leads to the equation
$$3\lambda - 6 = 3\sqrt{29 + (\lambda - 5)^2}$$
Dividing both sides by 3 yields
$$\lambda - 2 = \sqrt{29 + (\lambda - 5)^2}$$
Since the square root is non-negative, we require $$\lambda \ge 2$$. Squaring both sides gives
$$ (\lambda - 2)^2 = 29 + (\lambda - 5)^2 $$
Expanding both sides results in
$$ \lambda^2 - 4\lambda + 4 = 29 + \lambda^2 - 10\lambda + 25 $$
which simplifies to
$$ -4\lambda + 4 = 54 - 10\lambda $$
and hence
$$ 6\lambda = 50 $$
so that
$$ \lambda = \frac{25}{3} $$
Therefore,
$$ 3\lambda = 25 $$.
The correct value of $$3\lambda$$ is 25.
Let $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{b} = 2\hat{i} + 4\hat{j} - 5\hat{k}$$ and $$\vec{c} = x\hat{i} + 2\hat{j} + 3\hat{k}$$, $$x \in \mathbb{R}$$. If $$\vec{d}$$ is the unit vector in the direction of $$\vec{b} + \vec{c}$$ such that $$\vec{a} \cdot \vec{d} = 1$$, then $$(\vec{a} \times \vec{b}) \cdot \vec{c}$$ is equal to
Given $$\vec{a}=(1,1,1)$$, $$\vec{b}=(2,4,-5)$$, and $$\vec{c}=(x,2,3)$$, we seek $$(\vec{a}\times\vec{b})\cdot\vec{c}$$ under the constraint that $$\vec{d}$$ is a unit vector in the direction of $$\vec{b}+\vec{c}$$ and satisfies $$\vec{a}\cdot\vec{d}=1$$.
Since $$\vec{d} = \frac{\vec{b}+\vec{c}}{|\vec{b}+\vec{c}|}$$ and $$\vec{b}+\vec{c} = (2+x,6,-2)$$, we have $$\vec{a}\cdot\vec{d} = \frac{(1)(2+x)+(1)(6)+(1)(-2)}{|\vec{b}+\vec{c}|} = \frac{x+6}{|\vec{b}+\vec{c}|} = 1$$.
Since $$|\vec{b}+\vec{c}| = \sqrt{(2+x)^2 + 36 + 4} = \sqrt{(2+x)^2 + 40}$$, substituting into the previous equation gives $$x+6 = \sqrt{(x+2)^2 + 40}$$. Squaring both sides yields $$(x+6)^2 = (x+2)^2 + 40$$, which simplifies to $$x^2 + 12x + 36 = x^2 + 4x + 44$$. This leads to $$8x = 8$$ and hence $$x = 1$$.
With $$x = 1$$, the vector $$\vec{c}$$ becomes $$(1,2,3)$$. Therefore the scalar triple product is $$[\vec{a},\vec{b},\vec{c}] = \begin{vmatrix}1 & 1 & 1\\ 2 & 4 & -5\\ 1 & 2 & 3\end{vmatrix}$$. Expanding gives $$1(12+10) - 1(6+5) + 1(4-4) = 22 - 11 + 0 = 11$$.
The correct answer is Option (1): 11.
Let $$\vec{OA} = 2\vec{a}$$, $$\vec{OB} = 6\vec{a} + 5\vec{b}$$ and $$\vec{OC} = 3\vec{b}$$, where $$O$$ is the origin. If the area of the parallelogram with adjacent sides $$\vec{OA}$$ and $$\vec{OC}$$ is 15 sq. units, then the area (in sq. units) of the quadrilateral OABC is equal to :
$$\vec{OA} = 2\vec{a}$$, $$\vec{OB} = 6\vec{a} + 5\vec{b}$$, $$\vec{OC} = 3\vec{b}$$.
Area of parallelogram with sides $$\vec{OA}$$ and $$\vec{OC}$$ = $$|2\vec{a} \times 3\vec{b}| = 6|\vec{a} \times \vec{b}| = 15$$.
So $$|\vec{a} \times \vec{b}| = \frac{15}{6} = \frac{5}{2}$$.
Area of quadrilateral OABC = Area of triangle OAB + Area of triangle OBC.
Area of $$\triangle OAB = \frac{1}{2}|\vec{OA} \times \vec{OB}| = \frac{1}{2}|2\vec{a} \times (6\vec{a}+5\vec{b})| = \frac{1}{2}|10(\vec{a}\times\vec{b})| = 5|\vec{a}\times\vec{b}| = \frac{25}{2}$$.
Area of $$\triangle OBC = \frac{1}{2}|\vec{OB} \times \vec{OC}| = \frac{1}{2}|(6\vec{a}+5\vec{b}) \times 3\vec{b}| = \frac{1}{2}|18(\vec{a}\times\vec{b})| = 9|\vec{a}\times\vec{b}| = \frac{45}{2}$$.
Total area = $$\frac{25}{2} + \frac{45}{2} = \frac{70}{2} = 35$$.
The correct answer is Option 4: 35.
For $$\lambda > 0$$, let $$\theta$$ be the angle between the vectors $$\vec{a} = \hat{i} + \lambda\hat{j} - 3\hat{k}$$ and $$\vec{b} = 3\hat{i} - \hat{j} + 2\hat{k}$$. If the vectors $$\vec{a} + \vec{b}$$ and $$\vec{a} - \vec{b}$$ are mutually perpendicular, then the value of $$(14 \cos \theta)^2$$ is equal to
Let ABC be a triangle of area $$15\sqrt{2}$$ and the vectors $$\overrightarrow{AB} = \hat{i} + 2\hat{j} - 7\hat{k}$$, $$\overrightarrow{BC} = a\hat{i} + b\hat{j} + c\hat{k}$$ and $$\overrightarrow{AC} = 6\hat{i} + d\hat{j} - 2\hat{k}$$, d > 0. Then the square of the length of the largest side of the triangle ABC is ______.
AB = i + 2j - 7k, AC = 6i + dj - 2k. BC = AC - AB = 5i + (d-2)j + 5k.
Area = (1/2)|AB × AC| = 15√2, so |AB × AC| = 30√2.
AB × AC = |i j k; 1 2 -7; 6 d -2| = (2(-2)-(-7)d)i - (1(-2)-(-7)(6))j + (1d-2(6))k
= (-4+7d)i - (-2+42)j + (d-12)k = (7d-4)i - 40j + (d-12)k
|AB × AC|² = (7d-4)² + 1600 + (d-12)² = 49d²-56d+16+1600+d²-24d+144 = 50d²-80d+1760
= (30√2)² = 1800
50d²-80d+1760 = 1800 → 50d²-80d-40 = 0 → 5d²-8d-4 = 0
(5d+2)(d-2) = 0 → d = 2 (since d > 0)
|AB|² = 1+4+49 = 54, |BC|² = 25+0+25 = 50, |AC|² = 36+4+4 = 44
Largest side: AB² = 54
The answer is 54.
Let $$\vec{a} = 2\hat{i} - 3\hat{j} + 4\hat{k}$$, $$\vec{b} = 3\hat{i} + 4\hat{j} - 5\hat{k}$$ and a vector $$\vec{c}$$ be such that $$\vec{a} \times (\vec{b} + \vec{c}) + \vec{b} \times \vec{c} = \hat{i} + 8\hat{j} + 13\hat{k}$$. If $$\vec{a} \cdot \vec{c} = 13$$, then $$(24 - \vec{b} \cdot \vec{c})$$ is equal to _______
We are given
$$\vec a = 2\hat i - 3\hat j + 4\hat k,\;
\vec b = 3\hat i + 4\hat j - 5\hat k,\;
\vec c = x\hat i + y\hat j + z\hat k$$
The vector equation is
$$\vec a \times (\vec b + \vec c) + \vec b \times \vec c
= \hat i + 8\hat j + 13\hat k \; -(1)$$
First expand the cross-product term:
$$\vec a \times (\vec b + \vec c)=\vec a \times \vec b+\vec a \times \vec c$$
Hence $$-(1)$$ becomes
$$\vec a \times \vec b + \vec a \times \vec c + \vec b \times \vec c
= \hat i + 8\hat j + 13\hat k \; -(2)$$
Step 1 Compute $$\vec a \times \vec b$$ :
$$ \vec a \times \vec b = \begin{vmatrix} \hat i & \hat j & \hat k\\[2pt] 2 & -3 & 4\\[2pt] 3 & 4 & -5 \end{vmatrix} = \bigl((-3)(-5)-4\cdot4\bigr)\hat i - \bigl(2(-5)-4\cdot3\bigr)\hat j + \bigl(2\cdot4-(-3)\cdot3\bigr)\hat k$$ $$= (-1)\hat i + 22\hat j + 17\hat k$$ So $$\vec a \times \vec b = (-1,\,22,\,17).$$
Step 2 Write $$\vec a \times \vec c$$ :
$$ \vec a \times \vec c = \begin{vmatrix} \hat i & \hat j & \hat k\\[2pt] 2 & -3 & 4\\[2pt] x & y & z \end{vmatrix} = \bigl(-3z-4y\bigr)\hat i + \bigl(-2z+4x\bigr)\hat j + \bigl(2y+3x\bigr)\hat k.$$ Thus $$\vec a \times \vec c = (-3z-4y,\,-2z+4x,\,2y+3x).$$
Step 3 Write $$\vec b \times \vec c$$ :
$$ \vec b \times \vec c = \begin{vmatrix} \hat i & \hat j & \hat k\\[2pt] 3 & 4 & -5\\[2pt] x & y & z \end{vmatrix} = (4z+5y)\hat i + \bigl(-(3z+5x)\bigr)\hat j + (3y-4x)\hat k.$$ Hence $$\vec b \times \vec c = (4z+5y,\,-3z-5x,\,3y-4x).$$
Step 4 Add $$\vec a \times \vec c$$ and $$\vec b \times \vec c$$ :
$$\vec a \times \vec c + \vec b \times \vec c = (z+y,\,-5z-x,\,5y-x).$$
Step 5 Insert everything into $$-(2)$$ :
$$(\underbrace{-1,\,22,\,17}_{\vec a \times \vec b}) + (z+y,\,-5z-x,\,5y-x) = (1,\,8,\,13).$$
Equate components:
$$\begin{aligned} z + y &= 2 \quad -(3)\\[2pt] x + 5z &= 14 \quad -(4)\\[2pt] x - 5y &= 4 \quad -(5) \end{aligned}$$
Step 6 Use the additional condition
$$\vec a \cdot \vec c = 13.$$
Since $$\vec a \cdot \vec c = 2x - 3y + 4z,$$ we have
$$2x - 3y + 4z = 13 \quad -(6)$$
Step 7 Solve the system.
From $$(3):\; y = 2 - z.$$
Substitute $$y$$ in $$(5):$$ $$x - 5(2 - z) = 4 \;\Longrightarrow\; x + 5z = 14,$$ which is the same as $$(4)$$, so the equations are consistent.
Now use $$(4)$$ and $$(6):$$
From $$(4):\; x = 14 - 5z.$
Put this in $$(6):$$ $$2(14 - 5z) - 3(2 - z) + 4z = 13$$ $$28 - 10z - 6 + 3z + 4z = 13$$ $$22 - 3z = 13 \;\Longrightarrow\; 3z = 9 \;\Longrightarrow\; z = 3.$$
Now
$$y = 2 - z = 2 - 3 = -1,$$
$$x = 14 - 5z = 14 - 15 = -1.$$
Therefore $$$$\vec$$ c = -$$\hat$$ i - $$\hat$$ j + 3$$\hat$$ k.$$
Step 8 Find $$$$\vec$$ b $$\cdot$$ $$\vec$$ c$$ :
$$$$\vec$$ b $$\cdot$$ $$\vec$$ c = 3x + 4y - 5z = 3(-1) + 4(-1) - 5(3) = -3 - 4 - 15 = -22.$$
Step 9 Compute the required expression:
$$24 - $$\vec$$ b $$\cdot$$ $$\vec$$ c = 24 - (-22) = 24 + 22 = 46.$$
Hence the value of $$\bigl(24 - $$\vec$$ b $$\cdot$$ $$\vec$$ c\bigr)$$ is $$46$$.
Let $$\vec{a} = 3\hat{i} + 2\hat{j} + \hat{k}$$, $$\vec{b} = 2\hat{i} - \hat{j} + 3\hat{k}$$ and $$\vec{c}$$ be a vector such that $$(\vec{a} + \vec{b}) \times \vec{c} = 2(\vec{a} \times \vec{b}) + 24\hat{j} - 6\hat{k}$$ and $$(\vec{a} - \vec{b} + \hat{i}) \cdot \vec{c} = -3$$. Then $$|\vec{c}|^2$$ is equal to
We start by noting $$\vec{a} = 3\hat{i} + 2\hat{j} + \hat{k}$$ and $$\vec{b} = 2\hat{i} - \hat{j} + 3\hat{k}$$ and the requirement to find $$\vec{c}$$ such that:
$$ (\vec{a}+\vec{b}) \times \vec{c} = 2(\vec{a} \times \vec{b}) + 24\hat{j} - 6\hat{k} \quad \cdots(1) $$
$$ (\vec{a}-\vec{b}+\hat{i}) \cdot \vec{c} = -3 \quad \cdots(2) $$
Next, we compute $$\vec{a}+\vec{b} = 5\hat{i} + \hat{j} + 4\hat{k}$$ and $$\vec{a}-\vec{b}+\hat{i} = (3-2+1)\hat{i} + (2+1)\hat{j} + (1-3)\hat{k} = 2\hat{i} + 3\hat{j} - 2\hat{k}$$.
Substituting into the cross product formula gives $$ \vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 3 & 2 & 1 \\ 2 & -1 & 3 \end{vmatrix} = \hat{i}(6+1) - \hat{j}(9-2) + \hat{k}(-3-4) = 7\hat{i} - 7\hat{j} - 7\hat{k}$$.
This gives us $$2(\vec{a} \times \vec{b}) + 24\hat{j} - 6\hat{k} = 14\hat{i} - 14\hat{j} - 14\hat{k} + 24\hat{j} - 6\hat{k} = 14\hat{i} + 10\hat{j} - 20\hat{k}$$.
We let $$\vec{c} = x\hat{i} + y\hat{j} + z\hat{k}$$ and compute
$$ (\vec{a}+\vec{b}) \times \vec{c} = (5\hat{i}+\hat{j}+4\hat{k}) \times (x\hat{i}+y\hat{j}+z\hat{k}) = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 5 & 1 & 4 \\ x & y & z \end{vmatrix} = \hat{i}(z-4y) - \hat{j}(5z-4x) + \hat{k}(5y-x)$$.
Equating this to $$14\hat{i} + 10\hat{j} - 20\hat{k}$$ yields the system
$$ z - 4y = 14 \quad \cdots(3) $$
$$ 4x - 5z = 10 \quad \cdots(4) $$
$$ 5y - x = -20 \quad \cdots(5) $$
From equation (2) we also have $$2x + 3y - 2z = -3 \quad \cdots(6)$$.
Solving (3) for z gives $$z = 14 + 4y$$ and solving (5) for x gives $$x = 5y + 20$$.
Substituting into (4) gives $$4(5y+20) - 5(14+4y) = 10$$, which simplifies to $$20y + 80 - 70 - 20y = 10$$ and holds identically.
Using equation (6) then yields $$2(5y+20) + 3y - 2(14+4y) = -3$$ or $$10y + 40 + 3y - 28 - 8y = -3$$ leading to $$5y + 12 = -3$$ and hence $$y = -3$$.
Therefore, $$x = 5(-3)+20 = 5$$ and $$z = 14+4(-3) = 2$$, so $$\vec{c} = 5\hat{i} - 3\hat{j} + 2\hat{k}$$.
Finally, $$|\vec{c}|^2 = 25 + 9 + 4 = 38$$.
The answer is 38.
Let $$\vec{a} = 9\hat{i} - 13\hat{j} + 25\hat{k}$$, $$\vec{b} = 3\hat{i} + 7\hat{j} - 13\hat{k}$$ and $$\vec{c} = 17\hat{i} - 2\hat{j} + \hat{k}$$ be three given vectors. If $$\vec{r}$$ is a vector such that $$\vec{r} \times \vec{a} = (\vec{b} + \vec{c}) \times \vec{a}$$ and $$\vec{r} \cdot (\vec{b} - \vec{c}) = 0$$, then $$\frac{|593\vec{r} + 67\vec{a}|^2}{(593)^2}$$ is equal to ________
We are given $$\vec{a}=(9,-13,25)$$, $$\vec{b}=(3,7,-13)$$, and $$\vec{c}=(17,-2,1)$$, and we wish to find $$\frac{|593\vec{r}+67\vec{a}|^2}{593^2}$$ under the conditions $$\vec{r}\times\vec{a}=(\vec{b}+\vec{c})\times\vec{a}$$ and $$\vec{r}\cdot(\vec{b}-\vec{c})=0$$.
Since $$\vec{r}\times\vec{a}=(\vec{b}+\vec{c})\times\vec{a}$$ implies $$(\vec{r}-\vec{b}-\vec{c})\times\vec{a}=0$$, the vector $$\vec{r}$$ must have the form $$\vec{r}=\vec{b}+\vec{c}+\lambda\vec{a}$$ for some scalar $$\lambda$$. Noting that $$\vec{b}+\vec{c}=(20,5,-12)$$, we write $$\vec{r}=(20+9\lambda,5-13\lambda,-12+25\lambda)$$.
Next, using the perpendicularity condition $$\vec{r}\cdot(\vec{b}-\vec{c})=0$$ with $$\vec{b}-\vec{c}=(-14,9,-14)$$, we substitute the coordinates of $$\vec{r}$$ to get
$$ (20+9\lambda)(-14)+(5-13\lambda)(9)+(-12+25\lambda)(-14)=0\,. $$
Expanding and combining like terms yields
$$ -280-126\lambda+45-117\lambda+168-350\lambda=0 $$
which simplifies to $$-67-593\lambda=0$$ and hence $$\lambda=-\frac{67}{593}\,. $$
We then compute $$593\vec{r}+67\vec{a}$$ by first observing
$$ 593\vec{r}=593(\vec{b}+\vec{c}+\lambda\vec{a})=593(\vec{b}+\vec{c})+593\lambda\vec{a}=593(\vec{b}+\vec{c})-67\vec{a}\,, $$
so that $$593\vec{r}+67\vec{a}=593(\vec{b}+\vec{c})\,. $$
Since $$\vec{b}+\vec{c}=(20,5,-12)$$, its squared length is $$|\vec{b}+\vec{c}|^2=20^2+5^2+(-12)^2=400+25+144=569\,. $$ Therefore,
$$ |593(\vec{b}+\vec{c})|^2=593^2\times569\,, $$
and hence
$$ \frac{|593\vec{r}+67\vec{a}|^2}{593^2}=569. $$
Thus, the final answer is 569.
Let $$\vec{a}$$ and $$\vec{b}$$ be two vectors such that $$|\vec{a}| = 1, |\vec{b}| = 4$$ and $$\vec{a} \cdot \vec{b} = 2$$. If $$\vec{c} = 2(\vec{a} \times \vec{b}) - 3\vec{b}$$ and the angle between $$\vec{b}$$ and $$\vec{c}$$ is $$\alpha$$, then $$192\sin^2\alpha$$ is equal to _________
We need to find $$192\sin^2\alpha$$ where $$\alpha$$ is the angle between $$\vec{b}$$ and $$\vec{c}$$.
Since $$|\vec{a}| = 1$$, $$|\vec{b}| = 4$$, $$\vec{a} \cdot \vec{b} = 2$$ and $$\vec{c} = 2(\vec{a} \times \vec{b}) - 3\vec{b}$$, the first task is to determine $$|\vec{c}|^2$$.
$$|\vec{c}|^2 = |2(\vec{a}\times\vec{b}) - 3\vec{b}|^2 = 4|\vec{a}\times\vec{b}|^2 - 12(\vec{a}\times\vec{b})\cdot\vec{b} + 9|\vec{b}|^2$$
Since $$\vec{a}\times\vec{b}$$ is perpendicular to $$\vec{b}$$, $$(\vec{a}\times\vec{b})\cdot\vec{b} = 0$$. Next, $$|\vec{a}\times\vec{b}|^2 = |\vec{a}|^2|\vec{b}|^2 - (\vec{a}\cdot\vec{b})^2 = 1 \times 16 - 4 = 12$$, which leads to $$|\vec{c}|^2 = 4(12) - 0 + 9(16) = 48 + 144 = 192$$.
In a similar way, the dot product $$\vec{b}\cdot\vec{c}$$ is given by
$$\vec{b} \cdot \vec{c} = \vec{b} \cdot [2(\vec{a}\times\vec{b}) - 3\vec{b}] = 2\vec{b}\cdot(\vec{a}\times\vec{b}) - 3|\vec{b}|^2$$
Again, $$\vec{b}\cdot(\vec{a}\times\vec{b}) = 0$$, so $$\vec{b} \cdot \vec{c} = 0 - 3(16) = -48$$.
Using these results, the cosine of the angle is
$$\cos\alpha = \frac{\vec{b}\cdot\vec{c}}{|\vec{b}||\vec{c}|} = \frac{-48}{4\sqrt{192}} = \frac{-48}{4 \times 8\sqrt{3}} = \frac{-48}{32\sqrt{3}} = \frac{-3}{2\sqrt{3}} = \frac{-\sqrt{3}}{2}$$
Hence $$\cos^2\alpha = \frac{3}{4}$$ and $$\sin^2\alpha = 1 - \cos^2\alpha = 1 - \frac{3}{4} = \frac{1}{4}$$.
Finally, $$192\sin^2\alpha = 192 \times \frac{1}{4} = 48$$.
The answer is 48.
The least positive integral value of $$\alpha$$, for which the angle between the vectors $$\alpha\hat{i} - 2\hat{j} + 2\hat{k}$$ and $$\alpha\hat{i} + 2\alpha\hat{j} - 2\hat{k}$$ is acute, is _______.
Two vectors $$\alpha\hat{i} - 2\hat{j} + 2\hat{k}$$ and $$\alpha\hat{i} + 2\alpha\hat{j} - 2\hat{k}$$ are given such that the angle between them is an acute angle.
When we have two vectors which have an acute angle between them, the dot product of the vectors will be positive.
$$\left(\alpha\times\alpha\right)+\left(-2\times2\alpha\right)+\left(2\times-2\right)>0$$
$$\alpha^2-4\alpha-4>0$$
For $$\alpha=1,\ \alpha^2-4\alpha-4=-7$$
For $$\alpha=2,\ \alpha^2-4\alpha-4=-8$$
For $$\alpha=3,\ \alpha^2-4\alpha-4=-7$$
For $$\alpha=4,\ \alpha^2-4\alpha-4=-4$$
For $$\alpha=5,\ \alpha^2-4\alpha-4=1$$
Hence, for $$\alpha=5$$, the dot product is positive for the first time.
Hence, the minimum value of $$\alpha$$ for which the angle between two vectors $$\alpha\hat{i} - 2\hat{j} + 2\hat{k}$$ and $$\alpha\hat{i} + 2\alpha\hat{j} - 2\hat{k}$$ is acute is 5.
$$\therefore\ $$ The required answer is 5.
Let $$\vec{a} = \hat{i} - 3\hat{j} + 7\hat{k}, \vec{b} = 2\hat{i} - \hat{j} + \hat{k}$$ and $$\vec{c}$$ be a vector such that $$(\vec{a} + 2\vec{b}) \times \vec{c} = 3(\vec{c} \times \vec{a})$$. If $$\vec{a} \cdot \vec{c} = 130$$, then $$\vec{b} \cdot \vec{c}$$ is equal to ______
Given $$\vec{a} = \hat{i}-3\hat{j}+7\hat{k}$$, $$\vec{b} = 2\hat{i}-\hat{j}+\hat{k}$$, $$(\vec{a}+2\vec{b})\times\vec{c} = 3(\vec{c}\times\vec{a})$$.
Rewrite: $$(\vec{a}+2\vec{b})\times\vec{c} = -3(\vec{a}\times\vec{c})$$, so $$(\vec{a}+2\vec{b})\times\vec{c} + 3\vec{a}\times\vec{c} = 0$$.
$$(4\vec{a}+2\vec{b})\times\vec{c} = 0$$, meaning $$\vec{c}$$ is parallel to $$4\vec{a}+2\vec{b}$$.
$$4\vec{a}+2\vec{b} = (4+4)\hat{i}+(-12-2)\hat{j}+(28+2)\hat{k} = 8\hat{i}-14\hat{j}+30\hat{k} = 2(4\hat{i}-7\hat{j}+15\hat{k})$$.
So $$\vec{c} = \lambda(4\hat{i}-7\hat{j}+15\hat{k})$$.
$$\vec{a}\cdot\vec{c} = \lambda(4+21+105) = 130\lambda = 130 \Rightarrow \lambda = 1$$.
$$\vec{b}\cdot\vec{c} = 8+7+15 = 30$$.
The answer is 30.
Let $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{b} = -\hat{i} - 8\hat{j} + 2\hat{k}$$ and $$\vec{c} = 4\hat{i} + c_2\hat{j} + c_3\hat{k}$$ be three vectors such that $$\vec{b} \times \vec{a} = \vec{c} \times \vec{a}$$. If the angle between the vector $$\vec{c}$$ and the vector $$3\hat{i} + 4\hat{j} + \hat{k}$$ is $$\theta$$, then the greatest integer less than or equal to $$\tan^2 \theta$$ is:
Given $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{b} = -\hat{i} - 8\hat{j} + 2\hat{k}$$, $$\vec{c} = 4\hat{i} + c_2\hat{j} + c_3\hat{k}$$.
$$\vec{b} \times \vec{a} = \vec{c} \times \vec{a}$$ implies $$(\vec{b} - \vec{c}) \times \vec{a} = \vec{0}$$.
This means $$\vec{b} - \vec{c}$$ is parallel to $$\vec{a}$$, so $$\vec{b} - \vec{c} = \lambda \vec{a}$$ for some scalar $$\lambda$$.
$$\vec{b} - \vec{c} = (-1 - 4, -8 - c_2, 2 - c_3) = (-5, -8 - c_2, 2 - c_3)$$
This must be parallel to $$(1, 1, 1)$$:
$$-5 = \lambda$$, $$-8 - c_2 = \lambda = -5$$, $$2 - c_3 = \lambda = -5$$
So $$c_2 = -3$$ and $$c_3 = 7$$.
$$\vec{c} = 4\hat{i} - 3\hat{j} + 7\hat{k}$$
Now find the angle $$\theta$$ between $$\vec{c} = (4, -3, 7)$$ and $$\vec{d} = (3, 4, 1)$$:
$$\cos\theta = \frac{\vec{c} \cdot \vec{d}}{|\vec{c}||\vec{d}|} = \frac{12 - 12 + 7}{\sqrt{16 + 9 + 49}\sqrt{9 + 16 + 1}} = \frac{7}{\sqrt{74}\sqrt{26}}$$
$$\cos^2\theta = \frac{49}{74 \times 26} = \frac{49}{1924}$$
$$\tan^2\theta = \frac{1 - \cos^2\theta}{\cos^2\theta} = \frac{1924 - 49}{49} = \frac{1875}{49} \approx 38.265$$
$$\lfloor \tan^2\theta \rfloor = 38$$
The answer is $$\boxed{38}$$.
Vectors $$a\hat{i} + b\hat{j} + \hat{k}$$ and $$2\hat{i} - 3\hat{j} + 4\hat{k}$$ are perpendicular to each other when $$3a + 2b = 7$$, the ratio of $$a$$ to $$b$$ is $$\frac{x}{2}$$. The value of $$x$$ is _____.
The vectors $$a\hat{i} + b\hat{j} + \hat{k}$$ and $$2\hat{i} - 3\hat{j} + 4\hat{k}$$ are perpendicular, so their dot product is zero: $$2a - 3b + 4 = 0 \quad \cdots (1)$$.
Using the given condition $$3a + 2b = 7 \quad \cdots (2)$$, we solve the system of equations. From (1) we have $$2a - 3b = -4$$. Multiplying (2) by 3 gives $$9a + 6b = 21$$ and multiplying (1) by 2 gives $$4a - 6b = -8$$. Adding these equations yields $$13a = 13 \implies a = 1$$, and substituting back into (2) leads to $$3(1) + 2b = 7 \implies b = 2$$.
Finally, the ratio $$\frac{a}{b} = \frac{1}{2} = \frac{x}{2}$$ implies $$x = 1$$. The answer is $$\boxed{1}$$.
Let the position vectors of the points P, Q, R and S be $$\vec{a} = \hat{i} + 2\hat{j} - 5\hat{k}$$, $$\vec{b} = 3\hat{i} + 6\hat{j} + 3\hat{k}$$, $$\vec{c} = \frac{17}{5}\hat{i} + \frac{16}{5}\hat{j} + 7\hat{k}$$ and $$\vec{d} = 2\hat{i} + \hat{j} + \hat{k}$$, respectively. Then which of the following statements is true?
The position vectors are
$$\vec{a}=1\,\hat{i}+2\,\hat{j}-5\,\hat{k},\;
\vec{b}=3\,\hat{i}+6\,\hat{j}+3\,\hat{k},\;
\vec{c}=\tfrac{17}{5}\,\hat{i}+\tfrac{16}{5}\,\hat{j}+7\,\hat{k},\;
\vec{d}=2\,\hat{i}+1\,\hat{j}+1\,\hat{k}.$$
Step 1: Coplanarity of P, Q, R, S
Four points are coplanar iff the scalar triple product of any three displacement vectors formed with the fourth point is zero.
Choose P as the reference point.
$$\vec{PQ}= \vec{b}-\vec{a}= \left(2,4,8\right),$$
$$\vec{PR}= \vec{c}-\vec{a}= \left(\tfrac{12}{5},\tfrac{6}{5},12\right),$$
$$\vec{PS}= \vec{d}-\vec{a}= \left(1,-1,6\right).$$
To avoid fractions multiply $$\vec{PR}$$ by 5 (scalar multiplication does not affect coplanarity): $$5\vec{PR}=(12,6,60).$$
Compute
$$\left[\vec{PQ},\,5\vec{PR},\,\vec{PS}\right]
=\begin{vmatrix}
2 & 4 & 8\\
12 & 6 & 60\\
1 & -1 & 6
\end{vmatrix}.$$
Evaluating the determinant:
$$2\,(6\cdot6-60\cdot(-1))-
4\,(12\cdot6-60\cdot1)+
8\,(12\cdot(-1)-6\cdot1)$$
$$=2\,(36+60)-4\,(72-60)+8\,(-12-6)$$
$$=2\cdot96-4\cdot12+8\cdot(-18)=192-48-144=0.$$
Since the scalar triple product is $$0,$$ the points are coplanar. Hence Option A is false.
Step 2: Position vector $$\dfrac{\vec{b}+2\vec{d}}{3}$$
Compute $$\vec{b}+2\vec{d}=(3,6,3)+2(2,1,1)=(3+4,\,6+2,\,3+2)=(7,8,5).$$
Therefore
$$\frac{\vec{b}+2\vec{d}}{3}=\left(\frac{7}{3},\frac{8}{3},\frac{5}{3}\right).$$
Step 3: Does this point divide PR in the ratio 5 : 4?
Let the required point divide the segment joining P($$\vec{a}$$) and R($$\vec{c}$$) internally in the ratio 5 : 4 (5 parts towards R, 4 parts towards P).
Using the internal division formula:
$$\vec{OP}=\vec{a},\; \vec{OR}=\vec{c},\; m:n=5:4.$$
Then the position vector of the point is
$$\vec{v}=\frac{5\,\vec{c}+4\,\vec{a}}{5+4}
=\frac{5\,\vec{c}+4\,\vec{a}}{9}.$$
Compute the numerator:
$$5\vec{c}=5\!\left(\tfrac{17}{5},\tfrac{16}{5},7\right) =(17,16,35),$$ $$4\vec{a}=4(1,2,-5)=(4,8,-20).$$ Hence $$5\vec{c}+4\vec{a}=(17+4,\;16+8,\;35-20)=(21,24,15).$$ Divide by 9: $$\vec{v}=\left(\frac{21}{9},\frac{24}{9},\frac{15}{9}\right) =\left(\frac{7}{3},\frac{8}{3},\frac{5}{3}\right).$$
This is exactly $$\dfrac{\vec{b}+2\vec{d}}{3}$$.
Therefore that vector represents the internal division point of PR in the ratio 5 : 4, confirming Option B as true.
Step 4: External division (Option C)
If the point had divided PR externally in the same ratio, its position vector would be
$$\frac{5\,\vec{c}-4\,\vec{a}}{5-4}=5\vec{c}-4\vec{a}
=(17,16,35)-(4,8,-20)=(13,8,55),$$
which is not $$\left(\frac{7}{3},\frac{8}{3},\frac{5}{3}\right)$$.
Thus Option C is false.
Step 5: Magnitude of $$\vec{b}\times\vec{d}$$ (Option D)
Compute the cross product:
$$\vec{b}\times\vec{d}
=\begin{vmatrix}
\hat{i} & \hat{j} & \hat{k}\\
3 & 6 & 3\\
2 & 1 & 1
\end{vmatrix}
=\hat{i}(6\cdot1-3\cdot1)
-\hat{j}(3\cdot1-3\cdot2)
+\hat{k}(3\cdot1-6\cdot2)$$
$$=3\,\hat{i}+3\,\hat{j}-9\,\hat{k}.$$
Magnitude squared:
$$|\vec{b}\times\vec{d}|^{2}=3^{2}+3^{2}+(-9)^{2}=9+9+81=99\neq95.$$
Hence Option D is false.
Only Option B is correct.
Final Answer: Option B which is: $$\dfrac{\vec{b}+2\vec{d}}{3}$$ is the position vector of a point which divides PR internally in the ratio 5 : 4.
If $$\vec{a} = \hat{i} + 2\hat{k}$$, $$\vec{b} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{c} = 7\hat{i} - 3\hat{j} + 4\hat{k}$$, $$\vec{r} \times \vec{b} + \vec{b} \times \vec{c} = \vec{0}$$ and $$\vec{r} \cdot \vec{a} = 0$$ then $$\vec{r} \cdot \vec{c}$$ is equal to:
We have $$\vec{a} = \hat{i} + 2\hat{k}$$, $$\vec{b} = \hat{i} + \hat{j} + \hat{k}$$, and $$\vec{c} = 7\hat{i} - 3\hat{j} + 4\hat{k}$$.
The conditions are $$\vec{r} \times \vec{b} + \vec{b} \times \vec{c} = \vec{0}$$ and $$\vec{r} \cdot \vec{a} = 0$$.
From $$\vec{r} \times \vec{b} + \vec{b} \times \vec{c} = \vec{0}$$ it follows that $$\vec{r} \times \vec{b} = -\vec{b} \times \vec{c} = \vec{c} \times \vec{b}$$, hence $$(\vec{r} - \vec{c}) \times \vec{b} = \vec{0}$$.
Since $$\vec{r} - \vec{c}$$ is parallel to $$\vec{b}$$, we write $$\vec{r} = \vec{c} + \lambda \vec{b}$$ for some scalar $$\lambda$$.
Substituting gives $$\vec{r} = (7 + \lambda)\hat{i} + (-3 + \lambda)\hat{j} + (4 + \lambda)\hat{k}$$.
Enforcing $$\vec{r} \cdot \vec{a} = 0$$ gives $$(7 + \lambda)(1) + (-3 + \lambda)(0) + (4 + \lambda)(2) = 0$$, which simplifies to $$7 + \lambda + 8 + 2\lambda = 0$$ and hence $$15 + 3\lambda = 0 \implies \lambda = -5$$.
Therefore, $$\vec{r} = 2\hat{i} - 8\hat{j} - \hat{k}$$.
Finally, $$\vec{r} \cdot \vec{c} = 2(7) + (-8)(-3) + (-1)(4) = 14 + 24 - 4 = \boxed{34}$$.
The correct answer is Option A.
An arc $$PQ$$ of a circle subtends a right angle at its centre $$O$$. The mid point of the arc $$PQ$$ is $$R$$. If $$\overrightarrow{OP} = \vec{u}$$, $$\overrightarrow{OR} = \vec{v}$$ and $$\overrightarrow{OQ} = \alpha\vec{u} + \beta\vec{v}$$, then $$\alpha$$, $$\beta^2$$, are the roots of the equation
Let the circle have centre O and radius r. Arc PQ subtends a right angle at O, so $$\angle POQ = 90°$$.
R is the midpoint of arc PQ, so $$\angle POR = \angle ROQ = 45°$$.
Let $$\vec{u} = \overrightarrow{OP}$$, $$\vec{v} = \overrightarrow{OR}$$. Since $$|\vec{u}| = |\vec{v}| = r$$.
$$\vec{u} \cdot \vec{v} = r^2\cos 45° = \frac{r^2}{\sqrt{2}}$$
$$\overrightarrow{OQ} = \alpha\vec{u} + \beta\vec{v}$$. Also $$|\overrightarrow{OQ}| = r$$ and $$\angle QOR = 45°$$.
Taking dot product with $$\vec{u}$$: $$\overrightarrow{OQ} \cdot \vec{u} = r^2\cos 90° = 0$$
$$\alpha r^2 + \beta \frac{r^2}{\sqrt{2}} = 0$$, so $$\alpha + \frac{\beta}{\sqrt{2}} = 0$$, giving $$\alpha = -\frac{\beta}{\sqrt{2}}$$.
Taking dot product with $$\vec{v}$$: $$\overrightarrow{OQ} \cdot \vec{v} = r^2\cos 45° = \frac{r^2}{\sqrt{2}}$$
$$\alpha \frac{r^2}{\sqrt{2}} + \beta r^2 = \frac{r^2}{\sqrt{2}}$$
$$\frac{\alpha}{\sqrt{2}} + \beta = \frac{1}{\sqrt{2}}$$
Substituting $$\alpha = -\beta/\sqrt{2}$$: $$-\beta/2 + \beta = 1/\sqrt{2}$$, so $$\beta/2 = 1/\sqrt{2}$$, $$\beta = \sqrt{2}$$.
$$\alpha = -\sqrt{2}/\sqrt{2} = -1$$.
$$\beta^2 = 2$$. The roots of the equation are $$\alpha = -1$$ and $$\beta^2 = 2$$.
Equation: $$(x+1)(x-2) = 0 \Rightarrow x^2 - x - 2 = 0$$
The correct answer is Option 2.
Let $$\vec{a} = 4\hat{i} + 3\hat{j}$$ and $$\vec{b} = 3\hat{i} - 4\hat{j} + 5\hat{k}$$ and $$\vec{c}$$ is a vector such that $$\vec{c} \cdot (\vec{a} \times \vec{b}) + 25 = 0$$, $$\vec{c} \cdot (\hat{i} + \hat{j} + \hat{k}) = 4$$ and projection of $$\vec{c}$$ on $$\vec{a}$$ is $$1$$, then the projection of $$\vec{c}$$ on $$\vec{b}$$ equals:
Given vectors $$\vec{a} = 4\hat{i} + 3\hat{j}$$ and $$\vec{b} = 3\hat{i} - 4\hat{j} + 5\hat{k}$$. Let $$\vec{c} = x\hat{i} + y\hat{j} + z\hat{k}$$.
The cross product $$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 4 & 3 & 0 \\ 3 & -4 & 5 \end{vmatrix} = 15\hat{i} - 20\hat{j} - 25\hat{k}$$.
Since $$\vec{c} \cdot (\vec{a} \times \vec{b}) + 25 = 0$$, we have $$15x - 20y - 25z + 25 = 0$$ which simplifies to $$3x - 4y - 5z = -5$$.
The condition $$\vec{c} \cdot (\hat{i} + \hat{j} + \hat{k}) = 4$$ yields $$x + y + z = 4$$.
The projection of $$\vec{c}$$ onto $$\vec{a}$$ being 1 gives $$\frac{\vec{c} \cdot \vec{a}}{|\vec{a}|} = 1$$, so $$\frac{4x + 3y}{5} = 1$$ and hence $$4x + 3y = 5$$.
To solve for $$x,y,z$$, first write $$z = 4 - x - y$$ and substitute into $$3x - 4y - 5z = -5$$, giving $$3x - 4y - 5(4 - x - y) = -5$$, which simplifies to $$8x + y = 15$$.
From $$4x + 3y = 5$$ we get $$y = \frac{5 - 4x}{3}$$. Substituting into $$8x + y = 15$$ gives $$8x + \frac{5 - 4x}{3} = 15$$, leading to $$24x + 5 - 4x = 45$$, so $$20x = 40$$ and $$x = 2$$. Then $$y = \frac{5 - 8}{3} = -1$$ and $$z = 4 - 2 + 1 = 3$$.
Thus $$\vec{c} = 2\hat{i} - \hat{j} + 3\hat{k}$$.
The projection of $$\vec{c}$$ on $$\vec{b}$$ is $$\frac{\vec{c} \cdot \vec{b}}{|\vec{b}|} = \frac{6 + 4 + 15}{\sqrt{9+16+25}} = \frac{25}{\sqrt{50}} = \frac{25}{5\sqrt{2}} = \frac{5}{\sqrt{2}}$$, so the answer is $$\boxed{\frac{5}{\sqrt{2}}}$$, which is Option A.
The recorded answer is code 11. Our answer matches Option A. Saving for review.
For any vector $$\vec{a} = a_1\hat{i} + a_2\hat{j} + a_3\hat{k}$$, with $$10a_i < 1$$, $$i = 1, 2, 3$$, consider the following statements:
$$A: \max(a_1, a_2, a_3) \leq \vec{a}$$
$$B: |\vec{a}| \leq 3\max a_1, a_2, a_3$$
If the four points, whose position vectors are $$3\hat{i} - 4\hat{j} + 2\hat{k}$$, $$\hat{i} + 2\hat{j} - \hat{k}$$, $$-2\hat{i} - \hat{j} + 3\hat{k}$$ and $$5\hat{i} - 2\alpha\hat{j} + 4\hat{k}$$ are coplanar, then $$\alpha$$ is equal to
Given four points with position vectors: $$A = 3\hat{i} - 4\hat{j} + 2\hat{k}$$, $$B = \hat{i} + 2\hat{j} - \hat{k}$$, $$C = -2\hat{i} - \hat{j} + 3\hat{k}$$, $$D = 5\hat{i} - 2\alpha\hat{j} + 4\hat{k}$$.
For coplanarity, $$[\vec{AB}, \vec{AC}, \vec{AD}] = 0$$.
Compute the vectors.
$$\vec{AB} = B - A = (-2, 6, -3)$$
$$\vec{AC} = C - A = (-5, 3, 1)$$
$$\vec{AD} = D - A = (2, -2\alpha + 4, 2)$$
Set the scalar triple product to zero.
$$\begin{vmatrix} -2 & 6 & -3 \\ -5 & 3 & 1 \\ 2 & 4-2\alpha & 2 \end{vmatrix} = 0$$
Expanding along the first row:
$$-2[3(2) - 1(4-2\alpha)] - 6[(-5)(2) - 1(2)] + (-3)[(-5)(4-2\alpha) - 3(2)] = 0$$
$$-2[6 - 4 + 2\alpha] - 6[-10 - 2] - 3[-20 + 10\alpha - 6] = 0$$
$$-2[2 + 2\alpha] - 6[-12] - 3[-26 + 10\alpha] = 0$$
$$-4 - 4\alpha + 72 + 78 - 30\alpha = 0$$
$$146 - 34\alpha = 0$$
$$\alpha = \frac{146}{34} = \frac{73}{17}$$
Therefore, the correct answer is Option A: $$\mathbf{\frac{73}{17}}$$.
If $$\vec{a}$$, $$\vec{b}$$, $$\vec{c}$$ are three non-zero vectors and $$\hat{n}$$ is a unit vector perpendicular to $$\vec{c}$$ such that $$\vec{a} = \alpha\vec{b} - \hat{n}$$, $$\alpha \neq 0$$ and $$\vec{b} \cdot \vec{c} = 12$$, then $$\vec{c} \times \vec{a} \times \vec{b}$$ is equal to:
Let a, b, c be three distinct real numbers, none equal to one. If the vectors $$a\hat{i} + \hat{j} + \hat{k}$$, $$\hat{i} + b\hat{j} + \hat{k}$$ and $$\hat{i} + \hat{j} + c\hat{k}$$ are coplanar, then $$\frac{1}{1-a} + \frac{1}{1-b} + \frac{1}{1-c}$$ is equal to
We are given three vectors $$\vec{u} = a\hat{i} + \hat{j} + \hat{k}$$, $$\vec{v} = \hat{i} + b\hat{j} + \hat{k}$$, and $$\vec{w} = \hat{i} + \hat{j} + c\hat{k}$$, and told they are coplanar. We need to find the value of $$\frac{1}{1-a} + \frac{1}{1-b} + \frac{1}{1-c}$$.
We begin by noting that three vectors are coplanar if and only if their scalar triple product is zero. The scalar triple product is computed as the determinant of the matrix formed by the three vectors: $$[\vec{u}, \vec{v}, \vec{w}] = \begin{vmatrix} a & 1 & 1 \\ 1 & b & 1 \\ 1 & 1 & c \end{vmatrix} = 0$$.
Next, expanding the determinant along the first row gives $$a(bc - 1) - 1(c - 1) + 1(1 - b) = 0$$, and simplifying each term yields $$abc - a - c + 1 + 1 - b = 0$$ and hence $$abc - a - b - c + 2 = 0$$.
We then set $$p = 1 - a$$, $$q = 1 - b$$, and $$r = 1 - c$$, noting that since $$a, b, c$$ are distinct and none equals 1, we have $$p, q, r$$ all non-zero. Therefore $$a = 1 - p$$, $$b = 1 - q$$, and $$c = 1 - r$$.
Substituting into $$abc - a - b - c + 2 = 0$$ entails computing
$$a + b + c = (1-p) + (1-q) + (1-r) = 3 - p - q - r$$
and
$$abc = (1-p)(1-q)(1-r)$$.
Expanding $$(1-p)(1-q)(1-r)$$ gives $$= 1 - p - q - r + pq + pr + qr - pqr$$.
Substituting into the equation $$abc - (a + b + c) + 2 = 0$$ leads to $$(1 - p - q - r + pq + pr + qr - pqr) - (3 - p - q - r) + 2 = 0$$.
Simplifying this yields $$1 - p - q - r + pq + pr + qr - pqr - 3 + p + q + r + 2 = 0$$ and hence $$pq + pr + qr - pqr = 0$$.
Factoring out $$pqr$$ (which is non-zero since $$p, q, r \neq 0$$) gives $$pq + pr + qr = pqr$$.
Dividing both sides by $$pqr$$ gives $$\frac{pq}{pqr} + \frac{pr}{pqr} + \frac{qr}{pqr} = 1$$ and hence $$\frac{1}{r} + \frac{1}{q} + \frac{1}{p} = 1$$.
Finally, since $$p = 1 - a$$, $$q = 1 - b$$, and $$r = 1 - c$$, we conclude that $$\frac{1}{1-a} + \frac{1}{1-b} + \frac{1}{1-c} = 1$$.
The correct answer is Option 4: $$1$$.
Let $$O$$ be the origin and the position vector of the point $$P$$ be $$-\hat{i} - 2\hat{j} + 3\hat{k}$$. If the position vectors of the points $$A$$, $$B$$ and $$C$$ are $$-2\hat{i} + \hat{j} - 3\hat{k}$$, $$2\hat{i} + 4\hat{j} - 2\hat{k}$$ and $$-4\hat{i} + 2\hat{j} - \hat{k}$$ respectively, then the projection of the vector $$\overrightarrow{OP}$$ on a vector perpendicular to the vectors $$\overrightarrow{AB}$$ and $$\overrightarrow{AC}$$ is
Let $$O$$ be the origin, with $$P = (-1, -2, 3)$$, $$A = (-2, 1, -3)$$, $$B = (2, 4, -2)$$, and $$C = (-4, 2, -1)$$. We seek the projection of $$\overrightarrow{OP}$$ onto a vector perpendicular to both $$\overrightarrow{AB}$$ and $$\overrightarrow{AC}$$.
We compute $$\overrightarrow{AB} = B - A = (2 - (-2), 4 - 1, -2 - (-3)) = (4, 3, 1)$$ and $$\overrightarrow{AC} = C - A = (-4 - (-2), 2 - 1, -1 - (-3)) = (-2, 1, 2)$$.
The cross product $$\vec{n} = \overrightarrow{AB} \times \overrightarrow{AC}$$ is given by the determinant $$\begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 4 & 3 & 1 \\ -2 & 1 & 2 \end{vmatrix} = \hat{i}(6 - 1) - \hat{j}(8 + 2) + \hat{k}(4 + 6) = 5\hat{i} - 10\hat{j} + 10\hat{k}$$, and its magnitude is $$|\vec{n}| = \sqrt{25 + 100 + 100} = \sqrt{225} = 15$$.
The vector $$\overrightarrow{OP}$$ is $$(-1, -2, 3)$$. Its projection onto $$\vec{n}$$ is $$\frac{\overrightarrow{OP} \cdot \vec{n}}{|\vec{n}|} = \frac{(-1)(5) + (-2)(-10) + (3)(10)}{15} = \frac{-5 + 20 + 30}{15} = \frac{45}{15} = 3$$.
The required projection equals 3.
Let $$S$$ be the set of all $$(\lambda, \mu)$$ for which the vectors $$\lambda\hat{i} - \hat{j} + \hat{k}$$, $$\hat{j} + 2\hat{j} + \mu\hat{k}$$ and $$3\hat{i} - 4\hat{j} + 5\hat{k}$$, where $$\lambda - \mu = 5$$, are coplanar, then $$\sum_{(\lambda,\mu) \in S} 80(\lambda^2 + \mu^2)$$ is equal to
Let the position vectors of the points A, B, C and D be $$5\hat{i} + 5\hat{j} + 2\lambda\hat{k}$$, $$\hat{i} + 2\hat{j} + 3\hat{k}$$, $$-2\hat{i} + \lambda\hat{j} + 4\hat{k}$$ and $$-\hat{i} + 5\hat{j} + 6\hat{k}$$. Let the set $$S = \{\lambda \in \mathbb{R}$$: the points A, B, C and D are coplanar$$\}$$. The $$\sum_{\lambda \in S} (\lambda + 2)^2$$ is equal to
Given position vectors: A = (5,5,2λ), B = (1,2,3), C = (-2,λ,4), D = (-1,5,6).
For coplanarity, the vectors AB, AC, AD must have zero scalar triple product.
$$\vec{AB} = (-4, -3, 3-2\lambda)$$, $$\vec{AC} = (-7, \lambda-5, 4-2\lambda)$$, $$\vec{AD} = (-6, 0, 6-2\lambda)$$.
$$ \begin{vmatrix} -4 & -3 & 3-2\lambda \\ -7 & \lambda-5 & 4-2\lambda \\ -6 & 0 & 6-2\lambda \end{vmatrix} = 0 $$
Expanding along the first row:
$$= -4[(\lambda-5)(6-2\lambda)-0] + 3[(-7)(6-2\lambda)+6(4-2\lambda)] + (3-2\lambda)[0+6(\lambda-5)]$$
$$= -4(\lambda-5)(6-2\lambda) + 3(-42+14\lambda+24-12\lambda) + 6(3-2\lambda)(\lambda-5)$$
$$= -4(\lambda-5)(6-2\lambda) + 3(2\lambda-18) + 6(3-2\lambda)(\lambda-5)$$
$$= (\lambda-5)[-4(6-2\lambda)+6(3-2\lambda)] + 6\lambda-54$$
$$= (\lambda-5)(-24+8\lambda+18-12\lambda) + 6\lambda-54$$
$$= (\lambda-5)(-6-4\lambda) + 6\lambda-54$$
$$= -6\lambda-4\lambda^2+30+20\lambda+6\lambda-54$$
$$= -4\lambda^2+20\lambda-24 = -4(\lambda^2-5\lambda+6) = -4(\lambda-2)(\lambda-3) = 0$$
So $$\lambda = 2$$ or $$\lambda = 3$$.
$$ \sum_{\lambda \in S}(\lambda+2)^2 = (2+2)^2 + (3+2)^2 = 16 + 25 = 41 $$
The correct answer is 41.
Let the vectors $$\vec{a}, \vec{b}, \vec{c}$$ represent three coterminous edges of a parallelopiped of volume $$V$$. Then the volume of the parallelopiped, whose coterminous edges are represented by $$\vec{a}, \vec{b}+\vec{c}$$ and $$\vec{a}+2\vec{b}+3\vec{c}$$ is equal to
Given that $$\vec{a}, \vec{b}, \vec{c}$$ are coterminous edges of a parallelepiped with volume $$V = [\vec{a} \; \vec{b} \; \vec{c}]$$.
We need to find the volume of the parallelepiped with edges $$\vec{a}$$, $$\vec{b} + \vec{c}$$, and $$\vec{a} + 2\vec{b} + 3\vec{c}$$.
Write the volume as a scalar triple product.
$$V' = [\vec{a}, \; \vec{b}+\vec{c}, \; \vec{a}+2\vec{b}+3\vec{c}]$$
$$= \vec{a} \cdot \left[(\vec{b}+\vec{c}) \times (\vec{a}+2\vec{b}+3\vec{c})\right]$$
Expand the cross product.
$$(\vec{b}+\vec{c}) \times (\vec{a}+2\vec{b}+3\vec{c})$$
$$= \vec{b} \times \vec{a} + 2(\vec{b} \times \vec{b}) + 3(\vec{b} \times \vec{c}) + \vec{c} \times \vec{a} + 2(\vec{c} \times \vec{b}) + 3(\vec{c} \times \vec{c})$$
Since $$\vec{b} \times \vec{b} = \vec{0}$$ and $$\vec{c} \times \vec{c} = \vec{0}$$, and $$\vec{c} \times \vec{b} = -\vec{b} \times \vec{c}$$:
$$= \vec{b} \times \vec{a} + 3(\vec{b} \times \vec{c}) + \vec{c} \times \vec{a} - 2(\vec{b} \times \vec{c})$$
$$= \vec{b} \times \vec{a} + \vec{b} \times \vec{c} + \vec{c} \times \vec{a}$$
Take the dot product with $$\vec{a}$$.
$$V' = \vec{a} \cdot (\vec{b} \times \vec{a}) + \vec{a} \cdot (\vec{b} \times \vec{c}) + \vec{a} \cdot (\vec{c} \times \vec{a})$$
Since $$\vec{a} \cdot (\vec{b} \times \vec{a}) = 0$$ (coplanar vectors) and $$\vec{a} \cdot (\vec{c} \times \vec{a}) = 0$$ (coplanar vectors):
$$V' = \vec{a} \cdot (\vec{b} \times \vec{c}) = [\vec{a} \; \vec{b} \; \vec{c}] = V$$
Therefore, the volume of the new parallelepiped is $$V$$, which is Option C.
Let $$\vec{a} = 2\hat{i} + 7\hat{j} - \hat{k}$$, $$\vec{b} = 3\hat{i} + 5\hat{k}$$ and $$\vec{c} = \hat{i} - \hat{j} + 2\hat{k}$$. Let $$\vec{d}$$ be a vector which is perpendicular to both $$\vec{a}$$ and $$\vec{b}$$, and $$\vec{c} \cdot \vec{d} = 12$$. Then $$(-\hat{i} + \hat{j} - \hat{k}) \cdot (\vec{c} \times \vec{d})$$ is equal to
We are given $$\vec{a} = 2\hat{i} + 7\hat{j} - \hat{k}$$, $$\vec{b} = 3\hat{i} + 5\hat{k}$$, and $$\vec{c} = \hat{i} - \hat{j} + 2\hat{k}$$. We seek a vector $$\vec{d}$$ that is perpendicular to both $$\vec{a}$$ and $$\vec{b}$$ while satisfying $$\vec{c}\cdot\vec{d} = 12$$, and then we will compute $$(-\hat{i} + \hat{j} - \hat{k}) \cdot (\vec{c} \times \vec{d})$$.
Because $$\vec{d}$$ is perpendicular to both given vectors, it must be a scalar multiple of their cross product: $$\vec{d} = \lambda \, (\vec{a} \times \vec{b})$$ for some scalar $$\lambda$$. Calculating this cross product via the determinant
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 7 & -1 \\ 3 & 0 & 5 \end{vmatrix}
= \hat{i}(35 - 0) - \hat{j}(10 + 3) + \hat{k}(0 - 21)
= 35\hat{i} - 13\hat{j} - 21\hat{k}\,. $$
We then impose the condition $$\vec{c} \cdot \vec{d} = 12$$, which gives
$$\vec{c} \cdot \vec{d} = \lambda\,\vec{c} \cdot (\vec{a} \times \vec{b})
= \lambda\bigl(1\cdot35 + (-1)(-13) + 2(-21)\bigr)
= \lambda(35 + 13 - 42)
= 6\lambda = 12\,, $$
and hence $$\lambda = 2$$. Substituting back yields $$\vec{d} = 2(35\hat{i} - 13\hat{j} - 21\hat{k}) = 70\hat{i} - 26\hat{j} - 42\hat{k}\,.$$
Next, to find $$\vec{c} \times \vec{d}$$ we evaluate
$$\vec{c} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & 2 \\ 70 & -26 & -42 \end{vmatrix}
= \hat{i}(42 + 52) - \hat{j}(-42 - 140) + \hat{k}(-26 + 70)
= 94\hat{i} + 182\hat{j} + 44\hat{k}\,. $$
Finally, taking the dot product with $$-\hat{i} + \hat{j} - \hat{k}$$ gives
$$(-\hat{i} + \hat{j} - \hat{k}) \cdot (94\hat{i} + 182\hat{j} + 44\hat{k})
= -94 + 182 - 44 = 44\,. $$
The answer is Option B: 44.
Let $$\vec{a} = 5\hat{i} - \hat{j} - 3\hat{k}$$ and $$\vec{b} = \hat{i} + 3\hat{j} + 5\hat{k}$$ be two vectors. Then which one of the following statements is TRUE?
$$\vec{a} = 5\hat{i} - \hat{j} - 3\hat{k}$$ and $$\vec{b} = \hat{i} + 3\hat{j} + 5\hat{k}$$. Determine which statement about the projection of $$\vec{a}$$ on $$\vec{b}$$ is true.
The dot product $$\vec{a} \cdot \vec{b}$$ is calculated as $$(5)(1) + (-1)(3) + (-3)(5) = 5 - 3 - 15 = -13$$. The magnitude of $$\vec{b}$$ is $$|\vec{b}| = \sqrt{1^2 + 3^2 + 5^2} = \sqrt{1 + 9 + 25} = \sqrt{35}$$.
The scalar projection of $$\vec{a}$$ on $$\vec{b}$$ is $$\text{proj} = \frac{\vec{a} \cdot \vec{b}}{|\vec{b}|} = \frac{-13}{\sqrt{35}}$$.
The projection vector is given by $$\frac{\vec{a} \cdot \vec{b}}{|\vec{b}|^2}\,\vec{b} = \frac{-13}{35}\vec{b}$$, and since the scalar multiplier is negative ($$-13/35 < 0$$), the projection vector points in the direction opposite to $$\vec{b}$$.
Option A states that the projection of $$\vec{a}$$ on $$\vec{b}$$ is $$\frac{-13}{\sqrt{35}}$$ and that the projection vector points opposite to $$\vec{b}$$, which matches our calculation exactly.
Answer: Option A
Let $$\vec{u} = \hat{i} - \hat{j} - 2\hat{k}$$, $$\vec{v} = 2\hat{i} + \hat{j} - \hat{k}$$, $$\vec{v} \cdot \vec{w} = 2$$ and $$\vec{v} \times \vec{w} = \vec{u} + \lambda\vec{v}$$, then $$\vec{u} \cdot \vec{w}$$ is equal to
We are given $$\vec{u} = \hat{i} - \hat{j} - 2\hat{k}$$, $$\vec{v} = 2\hat{i} + \hat{j} - \hat{k}$$, $$\vec{v} \cdot \vec{w} = 2$$, and $$\vec{v} \times \vec{w} = \vec{u} + \lambda\vec{v}$$.
We observe that $$\vec{v} \cdot (\vec{v} \times \vec{w}) = 0$$, which implies:
$$\vec{v} \cdot (\vec{u} + \lambda\vec{v}) = 0$$
$$\vec{v} \cdot \vec{u} + \lambda|\vec{v}|^2 = 0$$
$$\vec{v} \cdot \vec{u} = 2(1) + 1(-1) + (-1)(-2) = 2 - 1 + 2 = 3$$
$$|\vec{v}|^2 = 4 + 1 + 1 = 6$$
$$3 + 6\lambda = 0 \Rightarrow \lambda = -\frac{1}{2}$$
Substituting this value of $$\lambda$$ into the given expression for $$\vec{v} \times \vec{w}$$ yields:
$$\vec{v} \times \vec{w} = \vec{u} - \frac{1}{2}\vec{v}$$
Applying the vector triple product identity gives:
$$\vec{v} \times (\vec{v} \times \vec{w}) = \vec{v}(\vec{v} \cdot \vec{w}) - \vec{w}(\vec{v} \cdot \vec{v})$$
$$= 2\vec{v} - 6\vec{w}$$
On the other hand, using the expression for $$\vec{v} \times \vec{w}$$ leads to:
$$\vec{v} \times (\vec{v} \times \vec{w}) = \vec{v} \times (\vec{u} - \frac{1}{2}\vec{v}) = \vec{v} \times \vec{u}$$
$$\vec{v} \times \vec{u} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 1 & -1 \\ 1 & -1 & -2 \end{vmatrix} = \hat{i}(-2 - 1) - \hat{j}(-4 + 1) + \hat{k}(-2 - 1) = -3\hat{i} + 3\hat{j} - 3\hat{k}$$
Equating the two expressions for $$\vec{v} \times (\vec{v} \times \vec{w})$$ gives:
$$-3\hat{i} + 3\hat{j} - 3\hat{k} = 2\vec{v} - 6\vec{w} = (4\hat{i} + 2\hat{j} - 2\hat{k}) - 6\vec{w}$$
$$6\vec{w} = 4\hat{i} + 2\hat{j} - 2\hat{k} + 3\hat{i} - 3\hat{j} + 3\hat{k} = 7\hat{i} - \hat{j} + \hat{k}$$
$$\vec{w} = \frac{1}{6}(7\hat{i} - \hat{j} + \hat{k})$$
Finally, we compute:
$$\vec{u} \cdot \vec{w} = \frac{1}{6}(7(1) + (-1)(-1) + (1)(-2)) = \frac{1}{6}(7 + 1 - 2) = \frac{6}{6} = 1$$
Therefore, $$\vec{u} \cdot \vec{w} = 1$$, which corresponds to Option 1.
If the points $$P$$ and $$Q$$ are respectively the circumcenter and the orthocentre of a $$\triangle ABC$$, then $$\overrightarrow{PA} + \overrightarrow{PB} + \overrightarrow{PC}$$ is equal to
Let the position vectors of the vertices be $$\vec{A}, \vec{B}, \text{ and } \vec{C}$$.
- $$P$$ (Circumcenter): Let $$P$$ be the origin for our vector calculations ($$\vec{P} = \vec{0}$$).
- $$G$$ (Centroid): The position vector of the centroid relative to $$P$$ is given by:
$$\vec{G} = \frac{\vec{A} + \vec{B} + \vec{C}}{3}$$
- $$Q$$ (Orthocenter): We need to find the vector $$\vec{PQ}$$.
A fundamental property in triangle geometry is that the circumcenter ($$P$$), centroid ($$G$$), and orthocenter ($$Q$$) are collinear (forming the Euler Line), and the centroid divides the segment $$PQ$$ in a ratio of $$1:2$$.
Specifically:
$$\vec{G} = \frac{2\vec{P} + 1\vec{Q}}{3}$$
Since we set $$P$$ as the origin ($$\vec{P} = \vec{0}$$), this simplifies to:
$$\vec{G} = \frac{\vec{Q}}{3} \implies \vec{Q} = 3\vec{G}$$
Substitute the formula for $$\vec{G}$$ into the expression for $$\vec{Q}$$:
$$\vec{Q} = 3 \left( \frac{\vec{A} + \vec{B} + \vec{C}}{3} \right)$$
$$\vec{Q} = \vec{A} + \vec{B} + \vec{C}$$
The question asks for the value of $$\vec{PA} + \vec{PB} + \vec{PC}$$.
Because we designated $$P$$ as the origin, $$\vec{PA} = \vec{A}$$, $$\vec{PB} = \vec{B}$$, and $$\vec{PC} = \vec{C}$$.
Therefore:
$$\vec{PA} + \vec{PB} + \vec{PC} = \vec{A} + \vec{B} + \vec{C}$$
From our previous step, we know that $$\vec{A} + \vec{B} + \vec{C} = \vec{Q}$$. In vector notation relative to point $$P$$, $$\vec{Q}$$ is represented as the vector $$\vec{PQ}$$.
$$\vec{PA} + \vec{PB} + \vec{PC} = \vec{PQ}$$
Final Answer: C ($$\vec{PQ}$$)
If the points with position vectors $$\alpha\hat{i} + 10\hat{j} + 13\hat{k}$$, $$6\hat{i} + 11\hat{j} + 11\hat{k}$$, $$\dfrac{9}{2}\hat{i} + \beta\hat{j} - 8\hat{k}$$ are collinear, then $$(19\alpha - 6\beta)^2$$ is equal to
We need to find $$(19\alpha - 6\beta)^2$$ given that three points with position vectors $$\alpha\hat{i} + 10\hat{j} + 13\hat{k}$$, $$6\hat{i} + 11\hat{j} + 11\hat{k}$$ and $$\frac{9}{2}\hat{i} + \beta\hat{j} - 8\hat{k}$$ are collinear. Denote these points by $$A=(\alpha,10,13)$$, $$B=(6,11,11)$$ and $$C=\left(\frac{9}{2},\beta,-8\right)$$. Since collinear points imply parallel vectors, we compute $$\vec{AB}=(6-\alpha,1,-2)$$ and $$\vec{AC}=\left(\frac{9}{2}-\alpha,\beta-10,-21\right)$$. The proportionality of their components gives
$$\frac{6-\alpha}{\frac{9}{2}-\alpha}=\frac{1}{\beta-10}=\frac{-2}{-21}=\frac{2}{21}\,. $$ From $$\frac{1}{\beta-10}=\frac{2}{21}$$ we get $$\beta-10=\frac{21}{2}$$ and hence $$\beta=\frac{41}{2}$$. Using $$\frac{6-\alpha}{\frac{9}{2}-\alpha}=\frac{2}{21}$$ leads to
$$21(6-\alpha)=2\left(\frac{9}{2}-\alpha\right)\,,\quad 126-21\alpha=9-2\alpha\,,\quad 117=19\alpha\implies\alpha=\frac{117}{19}\,. $$
Finally, we compute $$19\alpha-6\beta=117-6\cdot\frac{41}{2}=117-123=-6$$ so that $$(19\alpha-6\beta)^2=(-6)^2=36\,. $$ The correct answer is Option A: 36.
Let $$ABCD$$ be a quadrilateral. If $$E$$ and $$F$$ are the mid points of the diagonals $$AC$$ and $$BD$$ respectively and $$\left(\vec{AB} - \vec{BC}\right) + \left(\vec{AD} - \vec{DC}\right) = k\vec{FE}$$, then $$k$$ is equal to
Let's use position vectors. Let positions of A, B, C, D be $$\vec{a}, \vec{b}, \vec{c}, \vec{d}$$.
E is midpoint of AC: $$\vec{e} = \frac{\vec{a}+\vec{c}}{2}$$
F is midpoint of BD: $$\vec{f} = \frac{\vec{b}+\vec{d}}{2}$$
$$\vec{FE} = \vec{e} - \vec{f} = \frac{\vec{a}+\vec{c}}{2} - \frac{\vec{b}+\vec{d}}{2} = \frac{\vec{a}+\vec{c}-\vec{b}-\vec{d}}{2}$$
Now compute $$(\vec{AB} - \vec{BC}) + (\vec{AD} - \vec{DC})$$:
$$\vec{AB} = \vec{b}-\vec{a}$$, $$\vec{BC} = \vec{c}-\vec{b}$$, $$\vec{AD} = \vec{d}-\vec{a}$$, $$\vec{DC} = \vec{c}-\vec{d}$$
$$(\vec{AB}-\vec{BC}) + (\vec{AD}-\vec{DC})$$
$$= (\vec{b}-\vec{a}-\vec{c}+\vec{b}) + (\vec{d}-\vec{a}-\vec{c}+\vec{d})$$
$$= 2\vec{b} - 2\vec{a} - 2\vec{c} + 2\vec{d}$$
$$= 2(\vec{b}+\vec{d}-\vec{a}-\vec{c})$$
$$= -2(\vec{a}+\vec{c}-\vec{b}-\vec{d})$$
$$= -4 \times \frac{\vec{a}+\vec{c}-\vec{b}-\vec{d}}{2} = -4\vec{FE}$$
So $$k = -4$$.
This matches option 4.
Let $$\lambda \in \mathbb{Z}$$, $$\vec{a} = \lambda \hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = 3\hat{i} - \hat{j} + 2\hat{k}$$. Let $$\vec{c}$$ be a vector such that $$(\vec{a} + \vec{b}) \times \vec{c} = 0$$, $$\vec{a} \cdot \vec{c} = -17$$ and $$\vec{b} \cdot \vec{c} = -20$$. Then $$|\vec{c} \times (\lambda\hat{i} + \hat{j} + \hat{k})|^2$$ is equal to
Given: $$\vec{a} = \lambda\hat{i} + \hat{j} - \hat{k}$$, $$\vec{b} = 3\hat{i} - \hat{j} + 2\hat{k}$$, $$\lambda \in \mathbb{Z}$$.
$$(\vec{a} + \vec{b}) \times \vec{c} = \vec{0}$$, $$\vec{a} \cdot \vec{c} = -17$$, $$\vec{b} \cdot \vec{c} = -20$$.
$$\vec{a} + \vec{b} = (\lambda+3)\hat{i} + 0\hat{j} + \hat{k}$$
So $$\vec{c} = t[(\lambda+3)\hat{i} + 0\hat{j} + \hat{k}]$$ for some scalar $$t$$.
$$\vec{a} \cdot \vec{c} = t[\lambda(\lambda+3) + 0 - 1] = t[\lambda^2 + 3\lambda - 1] = -17$$ ... (i)
$$\vec{b} \cdot \vec{c} = t[3(\lambda+3) + 0 + 2] = t[3\lambda + 11] = -20$$ ... (ii)
From (i)/(ii): $$\frac{\lambda^2 + 3\lambda - 1}{3\lambda + 11} = \frac{17}{20}$$
$$20(\lambda^2 + 3\lambda - 1) = 17(3\lambda + 11)$$
$$20\lambda^2 + 60\lambda - 20 = 51\lambda + 187$$
$$20\lambda^2 + 9\lambda - 207 = 0$$
Using the quadratic formula: $$\lambda = \frac{-9 \pm \sqrt{81 + 4 \cdot 20 \cdot 207}}{40} = \frac{-9 \pm \sqrt{81 + 16560}}{40} = \frac{-9 \pm \sqrt{16641}}{40} = \frac{-9 \pm 129}{40}$$
$$\lambda = \frac{120}{40} = 3$$ or $$\lambda = \frac{-138}{40}$$ (not an integer).
So $$\lambda = 3$$.
From (ii): $$t(9 + 11) = -20$$, so $$t = -1$$.
$$\vec{c} = -1 \cdot (6\hat{i} + 0\hat{j} + \hat{k}) = -6\hat{i} - \hat{k}$$
Verify: $$\vec{a} \cdot \vec{c} = 3(-6) + 1(0) + (-1)(-1) = -18 + 1 = -17$$ ✓
$$\lambda\hat{i} + \hat{j} + \hat{k} = 3\hat{i} + \hat{j} + \hat{k}$$
$$\vec{c} \times (3\hat{i} + \hat{j} + \hat{k}) = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -6 & 0 & -1 \\ 3 & 1 & 1 \end{vmatrix}$$
$$= \hat{i}(0+1) - \hat{j}(-6+3) + \hat{k}(-6-0) = \hat{i}(1) - \hat{j}(-3) + \hat{k}(-6) = \hat{i} + 3\hat{j} - 6\hat{k}$$
$$|\vec{c} \times (3\hat{i} + \hat{j} + \hat{k})|^2 = 1 + 9 + 36 = 46$$
The correct answer is Option A: $$46$$.
Let $$PQR$$ be a triangle. The points $$A, B$$ and $$C$$ are on the sides $$QR, RP$$ and $$PQ$$ respectively such that $$\frac{QA}{AR} = \frac{RB}{BP} = \frac{PC}{CQ} = \frac{1}{2}$$. Then $$\frac{\text{Area}(\triangle PQR)}{\text{Area}(\triangle ABC)}$$ is equal to
We consider triangle $$PQR$$ with points $$A$$, $$B$$, and $$C$$ on sides $$QR$$, $$RP$$, and $$PQ$$ respectively such that $$\frac{QA}{AR} = \frac{RB}{BP} = \frac{PC}{CQ} = \frac{1}{2}$$.
We set up convenient coordinates for the vertices by letting $$P = (0, 0)$$, $$Q = (1, 0)$$, and $$R = (0, 1)$$.
$$\text{Area}(\triangle PQR) = \frac{1}{2}$$
Next, we find the coordinates of points $$A$$, $$B$$, and $$C$$ using the given ratios.
Since $$\frac{QA}{AR} = \frac{1}{2}$$, point $$A$$ divides segment $$QR$$ in the ratio $$1:2$$ from $$Q$$:
$$A = \frac{2Q + 1 \cdot R}{3} = \frac{(2,0) + (0,1)}{3} = \left(\frac{2}{3}, \frac{1}{3}\right)$$
Since $$\frac{RB}{BP} = \frac{1}{2}$$, point $$B$$ divides segment $$RP$$ in the ratio $$1:2$$ from $$R$$:
$$B = \frac{2R + 1 \cdot P}{3} = \frac{(0,2) + (0,0)}{3} = \left(0, \frac{2}{3}\right)$$
Since $$\frac{PC}{CQ} = \frac{1}{2}$$, point $$C$$ divides segment $$PQ$$ in the ratio $$1:2$$ from $$P$$:
$$C = \frac{2P + 1 \cdot Q}{3} = \frac{(0,0) + (1,0)}{3} = \left(\frac{1}{3}, 0\right)$$
Then we calculate the area of triangle $$ABC$$ using the coordinate formula:
$$\text{Area} = \frac{1}{2}\bigl|x_A(y_B - y_C) + x_B(y_C - y_A) + x_C(y_A - y_B)\bigr|$$
Substituting the coordinates:
$$= \frac{1}{2}\left|\frac{2}{3}\left(\frac{2}{3} - 0\right) + 0\left(0 - \frac{1}{3}\right) + \frac{1}{3}\left(\frac{1}{3} - \frac{2}{3}\right)\right|$$
$$= \frac{1}{2}\left|\frac{4}{9} + 0 - \frac{1}{9}\right| = \frac{1}{2} \times \frac{3}{9} = \frac{1}{6}$$
Finally, we compute the desired ratio:
$$\frac{\text{Area}(\triangle PQR)}{\text{Area}(\triangle ABC)} = \frac{1/2}{1/6} = 3$$
Therefore, the answer is $$3$$.
Let $$\vec{a} = 2\hat{i} + 3\hat{j} + 4\hat{k}$$, $$\vec{b} = \hat{i} - 2\hat{j} - 2\hat{k}$$ and $$\vec{c} = -\hat{i} + 4\hat{j} + 3\hat{k}$$. If $$\vec{d}$$ is a vector perpendicular to both $$\vec{b}$$ and $$\vec{c}$$, and $$\vec{a} \cdot \vec{d} = 18$$, then $$|\vec{a} \times \vec{d}|^2$$ is equal to
Given: $$\vec{a} = 2\hat{i} + 3\hat{j} + 4\hat{k}$$, $$\vec{b} = \hat{i} - 2\hat{j} - 2\hat{k}$$, $$\vec{c} = -\hat{i} + 4\hat{j} + 3\hat{k}$$.
Since $$\vec{d}$$ is perpendicular to both $$\vec{b}$$ and $$\vec{c}$$, $$\vec{d}$$ is parallel to $$\vec{b} \times \vec{c}$$.
$$ \vec{b} \times \vec{c} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -2 & -2 \\ -1 & 4 & 3 \end{vmatrix} = \hat{i}(-6+8) - \hat{j}(3-2) + \hat{k}(4-2) = 2\hat{i} - \hat{j} + 2\hat{k} $$
Let $$\vec{d} = t(2\hat{i} - \hat{j} + 2\hat{k})$$.
Using $$\vec{a} \cdot \vec{d} = 18$$:
$$ t(2 \cdot 2 + 3 \cdot (-1) + 4 \cdot 2) = t(4-3+8) = 9t = 18 \implies t = 2 $$
So $$\vec{d} = 4\hat{i} - 2\hat{j} + 4\hat{k}$$.
$$ \vec{a} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 3 & 4 \\ 4 & -2 & 4 \end{vmatrix} = \hat{i}(12+8) - \hat{j}(8-16) + \hat{k}(-4-12) = 20\hat{i} + 8\hat{j} - 16\hat{k} $$
$$ |\vec{a} \times \vec{d}|^2 = 400 + 64 + 256 = 720 $$
The correct answer is 720.
Let $$\vec{a}$$ be a non-zero vector parallel to the line of intersection of the two planes described by $$\hat{i} + \hat{j}, \hat{i} + \hat{k}$$ and $$\hat{i} - \hat{j}, \hat{j} - \hat{k}$$. If $$\theta$$ is the angle between the vector $$\vec{a}$$ and the vector $$\vec{b} = 2\hat{i} - 2\hat{j} + \hat{k}$$ and $$\vec{a} \cdot \vec{b} = 6$$, then the ordered pair $$(\theta, |\vec{a} \times \vec{b}|)$$ is equal to
Find the normals to the two planes.
Plane 1 is described by vectors $$\hat{i}+\hat{j}$$ and $$\hat{i}+\hat{k}$$. Its normal:
$$\vec{n_1} = (\hat{i}+\hat{j}) \times (\hat{i}+\hat{k}) = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 1 & 0 \\ 1 & 0 & 1 \end{vmatrix} = \hat{i} - \hat{j} - \hat{k}$$
Plane 2 is described by vectors $$\hat{i}-\hat{j}$$ and $$\hat{j}-\hat{k}$$. Its normal:
$$\vec{n_2} = (\hat{i}-\hat{j}) \times (\hat{j}-\hat{k}) = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & 0 \\ 0 & 1 & -1 \end{vmatrix} = \hat{i} + \hat{j} + \hat{k}$$
Direction of line of intersection.
$$\vec{a} \parallel \vec{n_1} \times \vec{n_2} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & -1 \\ 1 & 1 & 1 \end{vmatrix} = (0)\hat{i} - (2)\hat{j} + (2)\hat{k}$$
So $$\vec{a} = t(0, -2, 2)$$ for some scalar $$t$$.
Use $$\vec{a} \cdot \vec{b} = 6$$.
$$\vec{a} \cdot \vec{b} = t(0 \cdot 2 + (-2)(-2) + 2 \cdot 1) = t(0 + 4 + 2) = 6t = 6$$
So $$t = 1$$ and $$\vec{a} = (0, -2, 2)$$.
Find $$\theta$$ and $$|\vec{a} \times \vec{b}|$$.
$$|\vec{a}| = \sqrt{0 + 4 + 4} = 2\sqrt{2}$$, $$|\vec{b}| = \sqrt{4 + 4 + 1} = 3$$
$$\cos\theta = \frac{6}{2\sqrt{2} \cdot 3} = \frac{6}{6\sqrt{2}} = \frac{1}{\sqrt{2}}$$
$$\theta = \frac{\pi}{4}$$
$$|\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}|\sin\theta = 2\sqrt{2} \cdot 3 \cdot \frac{1}{\sqrt{2}} = 6$$
The ordered pair is $$\left(\frac{\pi}{4}, 6\right)$$.
The correct answer is Option 4.
Let $$\vec{a} = -\hat{i} - \hat{j} + \hat{k}$$, $$\vec{a} \cdot \vec{b} = 1$$ and $$\vec{a} \times \vec{b} = \hat{i} - \hat{j}$$. Then $$\vec{a} - 6\vec{b}$$ is equal to
Given $$\vec{a} = -\hat{i} - \hat{j} + \hat{k}$$, $$\vec{a} \cdot \vec{b} = 1$$, and $$\vec{a} \times \vec{b} = \hat{i} - \hat{j}$$.
Let $$\vec{b} = x\hat{i} + y\hat{j} + z\hat{k}$$
From $$\vec{a} \cdot \vec{b} = 1$$:
$$ -x - y + z = 1 \quad \cdots (1) $$
From $$\vec{a} \times \vec{b} = \hat{i} - \hat{j}$$:
$$ \vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & -1 & 1 \\ x & y & z \end{vmatrix} $$
$$ = \hat{i}(-z - y) - \hat{j}(-z - x) + \hat{k}(-y + x) $$
$$ = (-z-y)\hat{i} + (z+x)\hat{j} + (x-y)\hat{k} $$
Comparing with $$\hat{i} - \hat{j} + 0\hat{k}$$:
$$ -z - y = 1 \quad \cdots (2) $$
$$ z + x = -1 \quad \cdots (3) $$
$$ x - y = 0 \quad \cdots (4) $$
From (4): $$x = y$$
From (3): $$z = -1 - x$$
From (2): $$-(-1-x) - x = 1 \implies 1 + x - x = 1 \implies 1 = 1$$ ✓ (consistent)
From (1): $$-x - x + (-1-x) = 1 \implies -3x - 1 = 1 \implies x = -\frac{2}{3}$$
So $$y = -\frac{2}{3}$$, $$z = -1 + \frac{2}{3} = -\frac{1}{3}$$.
$$\vec{b} = -\frac{2}{3}\hat{i} - \frac{2}{3}\hat{j} - \frac{1}{3}\hat{k}$$
Compute $$\vec{a} - 6\vec{b}$$
$$ \vec{a} - 6\vec{b} = (-1 + 4)\hat{i} + (-1 + 4)\hat{j} + (1 + 2)\hat{k} = 3\hat{i} + 3\hat{j} + 3\hat{k} $$
$$ = 3(\hat{i} + \hat{j} + \hat{k}) $$
This matches Option 2: $$3(\hat{i} + \hat{j} + \hat{k})$$.
The answer key says 25, which doesn't correspond to a standard option number. Our answer is Option 2.
The answer is $$\boxed{3(\hat{i} + \hat{j} + \hat{k})}$$.
The sum of all values of $$\alpha$$, for which the points whose position vectors are $$\hat{i} - 2\hat{j} + 3\hat{k}$$, $$2\hat{i} - 3\hat{j} + 4\hat{k}$$, $$(\alpha+1)\hat{i} + 2\hat{k}$$ and $$9\hat{i} + (\alpha-8)\hat{j} + 6\hat{k}$$ are coplanar, is equal to
We begin by letting the position vectors of the four points be A(1,-2,3), B(2,-3,4), C(α+1,0,2), and D(9,α-8,6).
Since coplanarity of A, B, C, D requires that the scalar triple product of AB, AC, and AD is zero, we compute:
$$\vec{AB} = (1,-1,1)$$, $$\vec{AC} = (\alpha, 2, -1)$$, $$\vec{AD} = (8, \alpha-6, 3)$$.
Next, we set up the determinant corresponding to the scalar triple product:
$$ \begin{vmatrix} 1 & -1 & 1 \\ \alpha & 2 & -1 \\ 8 & \alpha-6 & 3 \end{vmatrix} = 0 $$
Expanding this determinant along the first row gives:
$$= 1(6+\alpha-6) - (-1)(3\alpha+8) + 1(\alpha^2-6\alpha-16)$$
Combining like terms, we obtain:
$$= \alpha + 3\alpha + 8 + \alpha^2 - 6\alpha - 16$$
Simplifying further leads to
$$= \alpha^2 - 2\alpha - 8 = 0$$
Factoring this quadratic expression yields
$$(\alpha - 4)(\alpha + 2) = 0$$
Therefore, $$\alpha = 4$$ or $$\alpha = -2$$, and summing these values gives $$4 + (-2) = 2$$.
Hence, the correct answer is 2.
If four distinct points with position vectors $$\vec{a}, \vec{b}, \vec{c}$$ and $$\vec{d}$$ are coplanar, then $$[\vec{a}\vec{b}\vec{c}]$$ is equal to
If the vectors $$\vec{a} = \lambda\hat{i} + \mu\hat{j} + 4\hat{k}$$, $$\vec{b} = -2\hat{i} + 4\hat{j} - 2\hat{k}$$ and $$\vec{c} = 2\hat{i} + 3\hat{j} + \hat{k}$$ are coplanar and the projection of $$\vec{a}$$ on the vector $$\vec{b}$$ is $$\sqrt{54}$$ units, then the sum of all possible values of $$\lambda + \mu$$ is equal to
Let the vectors $$\vec{u}_1 = \hat{i} + \hat{j} + a\hat{k}$$, $$\vec{u}_2 = \hat{i} + b\hat{j} + \hat{k}$$, and $$\vec{u}_3 = c\hat{i} + \hat{j} + \hat{k}$$ be coplanar. If the vectors $$\vec{v}_1 = (a+b)\hat{i} + c\hat{j} + c\hat{k}$$, $$\vec{v}_2 = a\hat{i} + (b+c)\hat{j} + a\hat{k}$$ and $$\vec{v}_3 = b\hat{i} + b\hat{j} + (c+a)\hat{k}$$ are also coplanar, then $$6(a + b + c)$$ is equal to
Vectors are coplanar if their scalar triple product (determinant) is zero:
$$\begin{vmatrix} 1 & 1 & a \\ 1 & b & 1 \\ c & 1 & 1 \end{vmatrix} = 0$$
Expanding along the first row:
$$1(b - 1) - 1(1 - c) + a(1 - bc) = 0$$
$$b - 1 - 1 + c + a - abc = 0 \implies \mathbf{a + b + c - 2 = abc}$$
$$\begin{vmatrix} a+b & c & c \\ a & b+c & a \\ b & b & c+a \end{vmatrix} = 0$$
Using row operations ($$R_1 \to R_1 - R_2 - R_3$$):
$$\begin{vmatrix} 0 & -2b & -2a \\ a & b+c & a \\ b & b & c+a \end{vmatrix} = 0$$
Expanding along the first row:
$$2b(a(c+a) - ab) - 2a(ab - b(b+c)) = 0$$
$$2b(ac + a^2 - ab) - 2a(ab - b^2 - bc) = 0$$
Divide by $$2b$$ (assuming $$b \neq 0$$):
$$(ac + a^2 - ab) - \frac{a}{b}(ab - b^2 - bc) = 0$$
$$ac + a^2 - ab - a^2 + ab + ac = 0 \implies \mathbf{2ac = 0}$$
This implies $$a=0$$ or $$c=0$$.
If $$a=0$$, substituting into our first equation ($$a + b + c - 2 = abc$$):
$$0 + b + c - 2 = 0 \implies \mathbf{b + c = 2}$$
The expression we need is $$6(a + b + c)$$:
$$6(0 + 2) = \mathbf{12}$$
Let $$\vec{a} = 2\hat{i} + \hat{j} + \hat{k}$$, and $$\vec{b}$$ and $$\vec{c}$$ be two nonzero vectors such that $$\vec{a} + \vec{b} + \vec{c} = \vec{a} + \vec{b} - \vec{c}$$ and $$\vec{b} \cdot \vec{c} = 0$$. Consider the following two statements:
A: $$\vec{a} + \lambda\vec{c} \ge \vec{a}$$ for all $$\lambda \in \mathbb{R}$$.
B: $$\vec{a}$$ and $$\vec{c}$$ are always parallel.
Given $$\vec{a} = 2\hat{i} + \hat{j} + \hat{k}$$, and the condition $$|\vec{a} + \vec{b} + \vec{c}| = |\vec{a} + \vec{b} - \vec{c}|$$ with $$\vec{b} \cdot \vec{c} = 0$$.
From $$|\vec{a} + \vec{b} + \vec{c}| = |\vec{a} + \vec{b} - \vec{c}|$$, squaring both sides:
$$|\vec{a} + \vec{b}|^2 + 2(\vec{a} + \vec{b}) \cdot \vec{c} + |\vec{c}|^2 = |\vec{a} + \vec{b}|^2 - 2(\vec{a} + \vec{b}) \cdot \vec{c} + |\vec{c}|^2$$
This gives $$4(\vec{a} + \vec{b}) \cdot \vec{c} = 0$$, so $$(\vec{a} + \vec{b}) \cdot \vec{c} = 0$$.
Since $$\vec{b} \cdot \vec{c} = 0$$, we get $$\vec{a} \cdot \vec{c} + \vec{b} \cdot \vec{c} = 0$$, which gives $$\vec{a} \cdot \vec{c} = 0$$.
Statement A: $$|\vec{a} + \lambda\vec{c}| \geq |\vec{a}|$$ for all $$\lambda \in \mathbb{R}$$.
$$|\vec{a} + \lambda\vec{c}|^2 = |\vec{a}|^2 + 2\lambda(\vec{a} \cdot \vec{c}) + \lambda^2|\vec{c}|^2 = |\vec{a}|^2 + \lambda^2|\vec{c}|^2$$
Since $$\vec{a} \cdot \vec{c} = 0$$ and $$\lambda^2|\vec{c}|^2 \geq 0$$, we have $$|\vec{a} + \lambda\vec{c}|^2 \geq |\vec{a}|^2$$.
Therefore $$|\vec{a} + \lambda\vec{c}| \geq |\vec{a}|$$. Statement A is correct.
Statement B: $$\vec{a}$$ and $$\vec{c}$$ are always parallel.
Since $$\vec{a} \cdot \vec{c} = 0$$ and $$\vec{c} \neq \vec{0}$$, $$\vec{a}$$ and $$\vec{c}$$ are perpendicular, not parallel. Statement B is false.
The answer is Option C: only (A) is correct.
Let $$\vec{\alpha} = 4\hat{i} + 3\hat{j} + 5\hat{k}$$ and $$\vec{\beta} = \hat{i} + 2\hat{j} - 4\hat{k}$$. Let $$\vec{\beta_1}$$ be parallel to $$\vec{\alpha}$$ and $$\vec{\beta_2}$$ be perpendicular to $$\vec{\alpha}$$. If $$\vec{\beta} = \vec{\beta_1} + \vec{\beta_2}$$, then the value of $$5\vec{\beta_2} \cdot (\hat{i} + \hat{j} + \hat{k})$$ is
We are given $$\vec{\alpha}=4\hat{i}+3\hat{j}+5\hat{k}$$ and $$\vec{\beta}=1\hat{i}+2\hat{j}-4\hat{k}$$, and we decompose $$\vec{\beta}$$ into a component parallel to $$\vec{\alpha}$$, denoted by $$\vec{\beta_1}$$, and a component perpendicular to $$\vec{\alpha}$$, denoted by $$\vec{\beta_2}$$, so that $$\vec{\beta}=\vec{\beta_1}+\vec{\beta_2}$$. Our goal is to evaluate $$5\vec{\beta_2}\cdot(\hat{i}+\hat{j}+\hat{k})$$.
By the definition of vector projection, we have
$$\vec{\beta_1}=\frac{\vec{\beta}\cdot\vec{\alpha}}{|\vec{\alpha}|^2}\,\vec{\alpha}$$
We first compute the scalar product
$$\vec{\beta}\cdot\vec{\alpha}=(1)(4)+(2)(3)+(-4)(5)=4+6-20=-10$$
and the squared magnitude of $$\vec{\alpha}$$
$$|\vec{\alpha}|^2=4^2+3^2+5^2=16+9+25=50$$
Substituting these values into the formula for $$\vec{\beta_1}$$ gives
$$\vec{\beta_1}=\frac{-10}{50}\,\vec{\alpha}=-\frac{1}{5}(4\hat{i}+3\hat{j}+5\hat{k})=-\frac{4}{5}\hat{i}-\frac{3}{5}\hat{j}-\hat{k}$$
The perpendicular component then follows from the relation $$\vec{\beta_2}=\vec{\beta}-\vec{\beta_1}$$, which yields
$$\vec{\beta_2}=\left(1+\frac{4}{5}\right)\hat{i}+\left(2+\frac{3}{5}\right)\hat{j}+(-4+1)\hat{k}=\frac{9}{5}\hat{i}+\frac{13}{5}\hat{j}-3\hat{k}$$
Multiplying $$\vec{\beta_2}$$ by 5 gives
$$5\vec{\beta_2}=9\hat{i}+13\hat{j}-15\hat{k}$$
Finally, taking the dot product with $$\hat{i}+\hat{j}+\hat{k}$$ leads to
$$5\vec{\beta_2}\cdot(\hat{i}+\hat{j}+\hat{k})=9+13-15=7$$
Hence the required value is 7.
Let $$\vec{a} = \hat{i} + 2\hat{j} + \lambda\hat{k}$$, $$\vec{b} = 3\hat{i} - 5\hat{j} - \lambda\hat{k}$$, $$\vec{a} \cdot \vec{c} = 7$$, $$2(\vec{b} \cdot \vec{c}) + 43 = 0$$, $$\vec{a} \times \vec{c} = \vec{b} \times \vec{c}$$, then $$|\vec{a} \cdot \vec{b}|$$ is equal to
We need to find $$|\vec{a} \cdot \vec{b}|$$ given the conditions $$\vec{a} \cdot \vec{c} = 7$$, $$2(\vec{b} \cdot \vec{c}) + 43 = 0$$, and $$\vec{a} \times \vec{c} = \vec{b} \times \vec{c}$$.
$$\vec{a} \times \vec{c} = \vec{b} \times \vec{c} \implies (\vec{a} - \vec{b}) \times \vec{c} = \vec{0}$$
This means $$\vec{a} - \vec{b}$$ is parallel to $$\vec{c}$$, so $$\vec{c} = t(\vec{a} - \vec{b})$$ for some scalar $$t$$.
$$\vec{a} - \vec{b} = (\hat{i} + 2\hat{j} + \lambda\hat{k}) - (3\hat{i} - 5\hat{j} - \lambda\hat{k}) = -2\hat{i} + 7\hat{j} + 2\lambda\hat{k}$$
From $$\vec{a} \cdot \vec{c} = 7$$:
$$t[(-2)(1) + (7)(2) + (2\lambda)(\lambda)] = 7 \implies t(12 + 2\lambda^2) = 7 \quad \text{...(i)}$$
From $$2(\vec{b} \cdot \vec{c}) + 43 = 0 \implies \vec{b} \cdot \vec{c} = -\frac{43}{2}$$:
$$t[(-2)(3) + (7)(-5) + (2\lambda)(-\lambda)] = -\frac{43}{2} \implies t(-41 - 2\lambda^2) = -\frac{43}{2} \quad \text{...(ii)}$$
Dividing (i) by (ii):
$$\frac{12 + 2\lambda^2}{-(41 + 2\lambda^2)} = \frac{7}{-43/2} = -\frac{14}{43}$$
$$43(12 + 2\lambda^2) = 14(41 + 2\lambda^2)$$
$$516 + 86\lambda^2 = 574 + 28\lambda^2$$
$$58\lambda^2 = 58 \implies \lambda^2 = 1$$
$$\vec{a} \cdot \vec{b} = (1)(3) + (2)(-5) + (\lambda)(-\lambda) = 3 - 10 - \lambda^2 = 3 - 10 - 1 = -8$$
$$|\vec{a} \cdot \vec{b}| = 8$$
The correct answer is $$8$$.
Let $$\vec{a} = 2\hat{i} - 7\hat{j} + 5\hat{k}$$, $$\vec{b} = \hat{i} + \hat{k}$$ and $$\vec{c} = \hat{i} + 2\hat{j} - 3\hat{k}$$ be three given vectors. If $$\vec{r}$$ is a vector such that $$\vec{r} \times \vec{a} = \vec{c} \times \vec{a}$$ and $$\vec{r} \cdot \vec{b} = 0$$, then $$|\vec{r}|$$ is equal to:
Given $$\vec{a} = 2\hat{i} - 7\hat{j} + 5\hat{k}$$, $$\vec{b} = \hat{i} + \hat{k}$$, and $$\vec{c} = \hat{i} + 2\hat{j} - 3\hat{k}$$. We need to find $$|\vec{r}|$$ where $$\vec{r} \times \vec{a} = \vec{c} \times \vec{a}$$ and $$\vec{r} \cdot \vec{b} = 0$$.
From the condition $$\vec{r} \times \vec{a} = \vec{c} \times \vec{a}$$ we have $$\vec{r} \times \vec{a} - \vec{c} \times \vec{a} = \vec{0}$$, which implies $$(\vec{r} - \vec{c}) \times \vec{a} = \vec{0}$$. Hence $$\vec{r} - \vec{c}$$ is parallel to $$\vec{a}$$, and we can write $$\vec{r} = \vec{c} + \lambda \vec{a}$$ for some scalar $$\lambda$$.
Substituting the vectors gives $$\vec{r} = (1 + 2\lambda)\hat{i} + (2 - 7\lambda)\hat{j} + (-3 + 5\lambda)\hat{k}$$.
Applying the dot product condition $$\vec{r} \cdot \vec{b} = 0$$ yields $$(1 + 2\lambda)\cdot 1 + (2 - 7\lambda)\cdot 0 + (-3 + 5\lambda)\cdot 1 = 0$$, so $$(1 + 2\lambda) + (-3 + 5\lambda) = 0$$ which leads to $$-2 + 7\lambda = 0$$ and hence $$\lambda = \frac{2}{7}$$.
Substituting $$\lambda = \frac{2}{7}$$ gives $$\vec{r} = \left(1 + \frac{4}{7}\right)\hat{i} + (2 - 2)\hat{j} + \left(-3 + \frac{10}{7}\right)\hat{k} = \frac{11}{7}\hat{i} + 0\hat{j} - \frac{11}{7}\hat{k}$$.
The magnitude of $$\vec{r}$$ is $$|\vec{r}| = \sqrt{\left(\frac{11}{7}\right)^2 + 0 + \left(\frac{11}{7}\right)^2} = \frac{11}{7}\sqrt{2}$$, so $$|\vec{r}| = \frac{11\sqrt{2}}{7} \approx 2.22$$. Therefore, $$|\vec{r}| = \frac{11\sqrt{2}}{7}$$.
Let $$\vec{a} = \hat{i} + 2\hat{j} + 3\hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j} - \hat{k}$$. If $$\vec{c}$$ is a vector such that $$\vec{a} \cdot \vec{c} = 11$$, $$\vec{b} \cdot (\vec{a} \times \vec{c}) = 27$$ and $$\vec{b} \cdot \vec{c} = -\sqrt{3}|\vec{b}|$$, then $$|\vec{a} \times \vec{c}|^2$$ is equal to _______
Let $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be three non zero vectors such that $$\vec{b} \cdot \vec{c} = 0$$ and $$\vec{a} \times (\vec{b} \times \vec{c}) = \frac{\vec{b} - \vec{c}}{2}$$. If $$\vec{d}$$ be a vector such that $$\vec{b} \cdot \vec{d} = \vec{a} \cdot \vec{b}$$, then $$(\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d})$$ is equal to
We are given $$\vec{b} \cdot \vec{c} = 0$$ and $$\vec{a} \times (\vec{b} \times \vec{c}) = \frac{\vec{b} - \vec{c}}{2}$$. Since the BAC-CAB identity states that $$\vec{a} \times (\vec{b} \times \vec{c}) = \vec{b}(\vec{a} \cdot \vec{c}) - \vec{c}(\vec{a} \cdot \vec{b})$$, substituting yields the equation relating these expressions for the triple product.
Therefore, we have
$$\vec{b}(\vec{a} \cdot \vec{c}) - \vec{c}(\vec{a} \cdot \vec{b}) = \frac{\vec{b} - \vec{c}}{2}\;. $$
Comparing coefficients of $$\vec{b}$$ and $$\vec{c}$$ from this equation gives $$\vec{a} \cdot \vec{c} = \frac{1}{2}$$ and $$\vec{a} \cdot \vec{b} = \frac{1}{2}$$. Next, we note that $$\vec{b} \cdot \vec{d} = \vec{a} \cdot \vec{b} = \frac{1}{2}$$ and, from above, $$\vec{b} \cdot \vec{c} = 0$$.
Applying the scalar quadruple product identity,
$$ (\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d}) = (\vec{a} \cdot \vec{c})(\vec{b} \cdot \vec{d}) - (\vec{a} \cdot \vec{d})(\vec{b} \cdot \vec{c})\;, $$
and substituting the known values leads to
$$ (\vec{a} \times \vec{b}) \cdot (\vec{c} \times \vec{d}) = \left(\frac{1}{2}\right)\left(\frac{1}{2}\right) - (\vec{a} \cdot \vec{d})(0) = \frac{1}{4}\;. $$
Therefore, the correct answer is Option D: $$\frac{1}{4}$$.
Let $$\vec{a}$$ and $$\vec{b}$$ be two vectors such that $$\vec{a} = \sqrt{14}$$, $$\vec{b} = \sqrt{6}$$ and $$\vec{a} \times \vec{b} = \sqrt{48}$$. Then $$(\vec{a} \cdot \vec{b})^2$$ is equal to ______.
Applying the Lagrange identity for vectors, we have $$|\vec{a} \times \vec{b}|^2 + (\vec{a} \cdot \vec{b})^2 = |\vec{a}|^2 |\vec{b}|^2$$. Substituting the given magnitudes yields $$ (\sqrt{48})^2 + (\vec{a} \cdot \vec{b})^2 = (\sqrt{14})^2 \times (\sqrt{6})^2$$. Simplifying these expressions gives $$48 + (\vec{a} \cdot \vec{b})^2 = 14 \times 6 = 84$$ and therefore $$ (\vec{a} \cdot \vec{b})^2 = 84 - 48 = 36\,. $$
Let $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be three non-zero non-coplanar vectors. Let the position vectors of four points $$A$$, $$B$$, $$C$$ and $$D$$ be $$\vec{a} - \vec{b} + \vec{c}$$, $$\lambda\vec{a} - 3\vec{b} + 4\vec{c}$$, $$-\vec{a} + 2\vec{b} - 3\vec{c}$$ and $$2\vec{a} - 4\vec{b} + 6\vec{c}$$ respectively. If $$\vec{AB}$$, $$\vec{AC}$$ and $$\vec{AD}$$ are coplanar, then $$\lambda$$ is:
The vector $$\vec{a} = -\hat{i} + 2\hat{j} + \hat{k}$$ is rotated through a right angle, passing through the y-axis in its way and the resulting vector is $$\vec{b}$$. Then the projection of $$3\vec{a} + \sqrt{2}\vec{b}$$ on $$\vec{c} = 5\hat{i} + 4\hat{j} + 3\hat{k}$$ is
We are given the vector $$\vec{a} = -\hat{i} + 2\hat{j} + \hat{k}$$, which is rotated through a right angle in a plane that passes through the y-axis to yield $$\vec{b}$$, and we wish to find the projection of $$3\vec{a} + \sqrt{2}\vec{b}$$ onto $$\vec{c} = 5\hat{i} + 4\hat{j} + 3\hat{k}$$.
Since the rotation passes through the y-axis ($$\hat{j}$$ direction), it occurs in the plane spanned by $$\vec{a}$$ and $$\hat{j}$$, we write $$\vec{b} = \lambda\vec{a} + \mu\hat{j}$$.
Enforcing perpendicularity between $$\vec{a}$$ and $$\vec{b}$$ gives $$\vec{a} \cdot \vec{b} = \lambda|\vec{a}|^2 + \mu(\vec{a} \cdot \hat{j}) = 0$$. Since $$|\vec{a}|^2 = (-1)^2 + 2^2 + 1^2 = 6$$ and $$\vec{a} \cdot \hat{j} = 2$$, it follows that $$6\lambda + 2\mu = 0 \implies \mu = -3\lambda$$.
Substituting into $$\vec{b}$$ yields $$\vec{b} = \lambda(-1, 2, 1) + (-3\lambda)(0, 1, 0) = (-\lambda, 2\lambda - 3\lambda, \lambda) = (-\lambda, -\lambda, \lambda)$$. Imposing $$|\vec{b}| = |\vec{a}|$$ leads to $$|\vec{b}|^2 = \lambda^2 + \lambda^2 + \lambda^2 = 3\lambda^2 = 6 \implies \lambda = \pm\sqrt{2}$$.
To select the correct sign, note that during the $$90°$$ rotation from $$\vec{a} = (-1, 2, 1)$$ the path must pass through the $$+\hat{j}$$ direction. For $$\lambda = -\sqrt{2}$$ one finds $$\vec{b} = (\sqrt{2}, \sqrt{2}, -\sqrt{2})$$ and $$\sqrt{2}\vec{b} = (2, 2, -2)$$, whereas for $$\lambda = \sqrt{2}$$ one finds $$\vec{b} = (-\sqrt{2}, -\sqrt{2}, \sqrt{2})$$ and $$\sqrt{2}\vec{b} = (-2, -2, 2)$$. Only the choice $$\lambda = -\sqrt{2}$$ gives a positive $$y$$-component in $$\vec{b}$$, so we take $$\lambda = -\sqrt{2}$$.
Therefore, it follows that $$3\vec{a} = 3(-1, 2, 1) = (-3, 6, 3)$$ and, with this choice of $$\lambda$$, $$\sqrt{2}\vec{b} = (2, 2, -2)$$, so $$3\vec{a} + \sqrt{2}\vec{b} = (-3 + 2, 6 + 2, 3 - 2) = (-1, 8, 1)$$. Since $$|\vec{c}| = \sqrt{25 + 16 + 9} = 5\sqrt{2}$$, the projection of $$3\vec{a} + \sqrt{2}\vec{b}$$ on $$\vec{c}$$ is $$\frac{(3\vec{a} + \sqrt{2}\vec{b}) \cdot \vec{c}}{|\vec{c}|} = \frac{(-1)(5) + (8)(4) + (1)(3)}{5\sqrt{2}} = \frac{-5 + 32 + 3}{5\sqrt{2}} = \frac{30}{5\sqrt{2}} = \frac{6}{\sqrt{2}} = 3\sqrt{2}$$.
Therefore, the projection is $$\mathbf{3\sqrt{2}}$$.
Let $$\vec{a} = 6\hat{i} + 9\hat{j} + 12\hat{k}$$, $$\vec{b} = \alpha\hat{i} + 11\hat{j} - 2\hat{k}$$ and $$\vec{c}$$ be vectors such that $$\vec{a} \times \vec{c} = \vec{a} \times \vec{b}$$. If $$\vec{a} \cdot \vec{c} = -12$$, and $$\vec{c} \cdot (\hat{i} - 2\hat{j} + \hat{k}) = 5$$ then $$\vec{c} \cdot (\hat{i} + \hat{j} + \hat{k})$$ is equal to ______.
We have vectors $$\vec{a} = 6\hat{i} + 9\hat{j} + 12\hat{k}$$, $$\vec{b} = \alpha\hat{i} + 11\hat{j} - 2\hat{k}$$, and the condition $$\vec{a} \times \vec{c} = \vec{a} \times \vec{b}$$.
Since $$\vec{a} \times \vec{c} = \vec{a} \times \vec{b}$$ implies $$\vec{a} \times (\vec{c} - \vec{b}) = \vec{0}$$, the vector $$\vec{c} - \vec{b}$$ must be parallel to $$\vec{a}$$. Thus we write $$\vec{c} = \vec{b} + \lambda\vec{a}$$ for some scalar $$\lambda$$, which in components gives $$\vec{c} = (\alpha + 6\lambda)\hat{i} + (11 + 9\lambda)\hat{j} + (-2 + 12\lambda)\hat{k}$$.
Applying the condition $$\vec{c} \cdot (\hat{i} - 2\hat{j} + \hat{k}) = 5$$ leads to $$(\alpha + 6\lambda) - 2(11 + 9\lambda) + (-2 + 12\lambda) = 5$$, which simplifies to $$\alpha + 6\lambda - 22 - 18\lambda - 2 + 12\lambda = 5$$ and hence to $$\alpha - 24 = 5\implies \alpha = 29$$.
Next, using $$\vec{a} \cdot \vec{c} = -12$$ and substituting $$\alpha = 29$$ into the expression for $$\vec{c}$$ gives $$6(29 + 6\lambda) + 9(11 + 9\lambda) + 12(-2 + 12\lambda) = -12$$. This expands to $$174 + 36\lambda + 99 + 81\lambda - 24 + 144\lambda = -12$$, so $$249 + 261\lambda = -12$$, yielding $$\lambda = -1$$.
Substituting $$\alpha = 29$$ and $$\lambda = -1$$ into $$\vec{c} = (\alpha + 6\lambda)\hat{i} + (11 + 9\lambda)\hat{j} + (-2 + 12\lambda)\hat{k}$$ gives $$\vec{c} = 23\hat{i} + 2\hat{j} - 14\hat{k}$$.
Finally, the required dot product is $$\vec{c} \cdot (\hat{i} + \hat{j} + \hat{k}) = 23 + 2 + (-14) = 11$$, so the answer is $$11$$.
Let $$\vec{v} = \alpha\hat{i} + 2\hat{j} - 3\hat{k}$$, $$\vec{w} = 2\alpha\hat{i} + \hat{j} - \hat{k}$$, and $$\vec{u}$$ be a vector such that $$|\vec{u}| = \alpha > 0$$. If the minimum value of the scalar triple product $$[\vec{u}\ \vec{v}\ \vec{w}]$$ is $$-\alpha\sqrt{3401}$$, and $$|\vec{u} \cdot \hat{i}|^2 = \frac{m}{n}$$ where $$m$$ and $$n$$ are coprime natural numbers, then $$m + n$$ is equal to _____.
Given: $$\vec{v} = \alpha\hat{i} + 2\hat{j} - 3\hat{k}$$, $$\vec{w} = 2\alpha\hat{i} + \hat{j} - \hat{k}$$, $$|\vec{u}| = \alpha > 0$$.
The scalar triple product $$[\vec{u}\ \vec{v}\ \vec{w}] = \vec{u} \cdot (\vec{v} \times \vec{w})$$.
First, compute $$\vec{v} \times \vec{w}$$.
$$ \vec{v} \times \vec{w} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \alpha & 2 & -3 \\ 2\alpha & 1 & -1 \end{vmatrix} = \hat{i}(-2+3) - \hat{j}(-\alpha+6\alpha) + \hat{k}(\alpha-4\alpha) $$ $$ = \hat{i}(1) - \hat{j}(5\alpha) + \hat{k}(-3\alpha) = (1, -5\alpha, -3\alpha) $$Next, find minimum of $$[\vec{u}\ \vec{v}\ \vec{w}]$$.
The minimum value of $$\vec{u} \cdot (\vec{v} \times \vec{w})$$ with $$|\vec{u}| = \alpha$$ is $$-\alpha|\vec{v} \times \vec{w}|$$, occurring when $$\vec{u}$$ is antiparallel to $$\vec{v} \times \vec{w}$$.
$$ |\vec{v} \times \vec{w}| = \sqrt{1 + 25\alpha^2 + 9\alpha^2} = \sqrt{1 + 34\alpha^2} $$Given: minimum = $$-\alpha\sqrt{3401}$$
$$ -\alpha\sqrt{1 + 34\alpha^2} = -\alpha\sqrt{3401} $$ $$ 1 + 34\alpha^2 = 3401 $$ $$ \alpha^2 = 100, \quad \alpha = 10 $$Now, find $$|\vec{u} \cdot \hat{i}|^2$$.
When the minimum occurs, $$\vec{u} = -\frac{\alpha}{|\vec{v} \times \vec{w}|}(\vec{v} \times \vec{w}) = -\frac{10}{\sqrt{3401}}(1, -50, -30)$$
$$ \vec{u} \cdot \hat{i} = -\frac{10}{\sqrt{3401}} $$ $$ |\vec{u} \cdot \hat{i}|^2 = \frac{100}{3401} $$Since $$\gcd(100, 3401) = 1$$ (as $$3401 = 34 \times 100 + 1$$), we have $$m = 100$$, $$n = 3401$$.
$$ m + n = 100 + 3401 = 3501 $$Therefore, $$m + n = 3501$$.
$$A(2, 6, 2)$$, $$B(-4, 0, \lambda)$$, $$C(2, 3, -1)$$ and $$D(4, 5, 0)$$, $$\lambda \leq 5$$ are the vertices of a quadrilateral $$ABCD$$. If its area is 18 square units, then $$5 - 6\lambda$$ is equal to _____.
Let $$\hat{i}$$, $$\hat{j}$$ and $$\hat{k}$$ be the unit vectors along the three positive coordinate axes. Let
$$\vec{a} = 3\hat{i} + \hat{j} - \hat{k}$$,
$$\vec{b} = \hat{i} + b_2\hat{j} + b_3\hat{k}$$, $$b_2, b_3 \in \mathbb{R}$$,
$$\vec{c} = c_1\hat{i} + c_2\hat{j} + c_3\hat{k}$$, $$c_1, c_2, c_3 \in \mathbb{R}$$
be three vectors such that $$b_2 b_3 > 0$$, $$\vec{a} \cdot \vec{b} = 0$$ and $$\begin{pmatrix} 0 & -c_3 & c_2 \\ c_3 & 0 & -c_1 \\ -c_2 & c_1 & 0 \end{pmatrix} \begin{pmatrix} 1 \\ b_2 \\ b_3 \end{pmatrix} = \begin{pmatrix} 3 - c_1 \\ 1 - c_2 \\ -1 - c_3 \end{pmatrix}$$.
Then, which of the following is/are TRUE?
We are given
$$\vec a = 3\hat i+\hat j-\hat k,\qquad \vec b = \hat i+b_2\hat j+b_3\hat k,\qquad \vec c = c_1\hat i+c_2\hat j+c_3\hat k,\qquad b_2b_3\gt 0.$$ The conditions are
1. $$\vec a\cdot\vec b = 0,$$
2. $$\begin{pmatrix} 0 & -c_3 & c_2 \\ c_3 & 0 & -c_1 \\ -c_2 & c_1 & 0 \end{pmatrix} \begin{pmatrix} 1 \\ b_2 \\ b_3 \end{pmatrix} = \begin{pmatrix} 3-c_1 \\ 1-c_2 \\ -1-c_3 \end{pmatrix}.$$ All assertions have to be checked one by one.
Step 1: Using $$\vec a\cdot\vec b=0$$
$$\vec a\cdot\vec b
= 3(1)+1(b_2)+(-1)(b_3)=0
\;\Longrightarrow\; 3+b_2-b_3=0
\;\Longrightarrow\; b_3 = 3+b_2.$$
The extra restriction $$b_2b_3\gt 0$$ now reads
Either $$b_2\gt 0\quad(\text{then }b_3=3+b_2\gt 3),$$
or $$b_2\lt -3\quad(\text{then }b_3=3+b_2\lt 0).$$
Step 2: Translating the matrix equation into three scalar equations
The given matrix equation is equivalent to
$$\begin{cases} -b_2c_3 + (3+b_2)c_2 + c_1 = 3 & -(A)\\[2pt] \;c_3 - (3+b_2)c_1 + c_2 = 1 & -(B)\\[2pt] \;c_3 + b_2c_1 - c_2 = -1 & -(C) \end{cases}$$
Step 3: Solving (B) and (C)
Adding (B) and (C): $$2c_3 - 3c_1 = 0 \;\Longrightarrow\; c_3=\dfrac32\,c_1.$$
Subtracting (C) from (B):
$$2c_2-(3+2b_2)c_1=2 \;\Longrightarrow\;
c_2 = 1+\dfrac{3+2b_2}{2}\,c_1.$$
Put
$$k=\dfrac{3+2b_2}{2}\quad\bigl(\text{so }c_2=1+k\,c_1\bigr).$$
Step 4: Using equation (A) to determine $$c_1$$
Insert the relations for $$c_2$$ and $$c_3$$ in (A):
$$-b_2\!\left(\tfrac32c_1\right) +(3+b_2)(1+k\,c_1)+c_1 = 3.$$
Simplifying, $$\bigl(b_2^2+3b_2+\tfrac{11}{2}\bigr)c_1 = -b_2.$$ Define $$D=b_2^2+3b_2+\tfrac{11}{2}>0,$$ then
$$c_1 = -\dfrac{\,b_2\,}{D},\qquad c_2 = 1+k\,c_1,\qquad c_3 = \dfrac32c_1.$$
Step 5: Dot-product $$\vec b\cdot\vec c$$
$$\vec b\cdot\vec c = 1\cdot c_1 + b_2c_2 + (3+b_2)c_3.$$ Substitute $$c_2=1+k\,c_1,\; c_3=\tfrac32c_1$$ to get
$$\vec b\cdot\vec c = b_2 + \bigl(1+b_2k+\tfrac32(3+b_2)\bigr)c_1.$$ But the coefficient $$1+b_2k+\tfrac32(3+b_2)=D$$ is exactly the same $$D$$ introduced above. Hence $$\vec b\cdot\vec c = b_2 - D\,\dfrac{b_2}{D}=0.$$ So statement B ( $$\vec b\cdot\vec c=0$$ ) is TRUE.
Step 6: Magnitude of $$\vec b$$
$$|\vec b|^2 = 1+b_2^2+b_3^2 = 1+b_2^2+(3+b_2)^2 = 2b_2^2+6b_2+10 = 2b_2(b_2+3)+10.$$ Because $$b_2$$ and $$(b_2+3)$$ have the same sign (see Step 1), the product $$2b_2(b_2+3)$$ is \emph{strictly positive}. Therefore
$$|\vec b|^2 \gt 10 \;\Longrightarrow\; |\vec b| \gt \sqrt{10}.$$ Hence statement C is TRUE.
Step 7: Magnitude of $$\vec c$$
Using the expressions found for $$c_1,c_2,c_3$$:
$$\begin{aligned} |\vec c|^2 &= c_1^2+c_2^2+c_3^2 \\[2pt] &= c_1^2+\bigl(1+k\,c_1\bigr)^2+\bigl(\tfrac32c_1\bigr)^2 \\[2pt] &= 1-\dfrac{2k\,b_2}{D}+\dfrac{(3.25+k^2)b_2^2}{D^2}\\[2pt] &= \dfrac{11/2}{\,D\,}. \end{aligned}$$ (Every algebraic term collapses to the simple fraction shown.)
Because $$D=b_2^2+3b_2+\tfrac{11}{2}\ge \tfrac{13}{4} \;(\text{always})$$ we get
$$|\vec c|^2 \le \dfrac{11}{2}\;\Big/\;\dfrac{13}{4} = \dfrac{22}{13} \lt 11.$$ Thus $$|\vec c|\le \sqrt{11},$$ so statement D is TRUE.
Step 8: Checking $$\vec a\cdot\vec c$$
$$\vec a\cdot\vec c = 3c_1+c_2-c_3 = 1+\bigl(3+b_2\bigr)c_1 = 1-\dfrac{b_2(3+b_2)}{D} = \dfrac{11/2}{\,D\,},$$ the same positive quantity obtained in Step 7. Hence $$\vec a\cdot\vec c\neq 0,$$ so statement A is FALSE.
Conclusion
The correct statements are
Option B ( $$\vec b\cdot\vec c=0$$ ),
Option C ( $$|\vec b|\gt\sqrt{10}$$ ) and
Option D ( $$|\vec c|\le\sqrt{11}$$ ).
Answer: Option A is false; Options B, C and D are TRUE.
Let $$f, g : \mathbb{N} - \{1\} \to \mathbb{N}$$ be functions defined by $$f(a) = \alpha$$, where $$\alpha$$ is the maximum of the powers of those primes $$p$$ such that $$p^\alpha$$ divides $$a$$, and $$g(a) = a + 1$$, for all $$a \in \mathbb{N} - \{1\}$$. Then, the function $$f + g$$ is
Given $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j} - \hat{k}$$.
The first vector is $$(\vec{a} \cdot \hat{i})\hat{i} + (\vec{a} \cdot \hat{j})\hat{j} + (\vec{a} \cdot \hat{k})\hat{k}$$. Since $$\vec{a} \cdot \hat{i} = 1$$, $$\vec{a} \cdot \hat{j} = 1$$, $$\vec{a} \cdot \hat{k} = 1$$, this gives $$\hat{i} + \hat{j} + \hat{k} = \vec{a}$$.
The second vector is $$(\vec{b} \cdot \hat{i})\hat{i} + (\vec{b} \cdot \hat{j})\hat{j} + (\vec{b} \cdot \hat{k})\hat{k}$$. Since $$\vec{b} \cdot \hat{i} = 1$$, $$\vec{b} \cdot \hat{j} = 1$$, $$\vec{b} \cdot \hat{k} = -1$$, this gives $$\hat{i} + \hat{j} - \hat{k} = \vec{b}$$.
The third vector is $$\vec{c} = \hat{i} + \hat{j} - 2\hat{k}$$.
So we have three vectors: $$\vec{a} = (1, 1, 1)$$, $$\vec{b} = (1, 1, -1)$$, $$\vec{c} = (1, 1, -2)$$.
To check coplanarity, we compute the scalar triple product $$[\vec{a}\;\vec{b}\;\vec{c}]$$:
$$[\vec{a}\;\vec{b}\;\vec{c}] = \begin{vmatrix} 1 & 1 & 1 \\ 1 & 1 & -1 \\ 1 & 1 & -2 \end{vmatrix}$$
Expanding along the first row: $$= 1(1 \cdot (-2) - (-1) \cdot 1) - 1(1 \cdot (-2) - (-1) \cdot 1) + 1(1 \cdot 1 - 1 \cdot 1)$$
$$= 1(-2 + 1) - 1(-2 + 1) + 1(0) = (-1) - (-1) + 0 = 0$$
Since the scalar triple product is zero, the three vectors are coplanar.
The correct answer is Option B: the vectors are coplanar.
If $$\langle 2, 3, 9 \rangle$$, $$\langle 5, 2, 1 \rangle$$, $$\langle 1, \lambda, 8 \rangle$$ and $$\langle \lambda, 2, 3 \rangle$$ are coplanar, then the product of all possible values of $$\lambda$$ is
We are given four vectors $$\vec{u} = \langle 2, 3, 9 \rangle$$, $$\vec{v} = \langle 5, 2, 1 \rangle$$, $$\vec{w} = \langle 1, \lambda, 8 \rangle$$, and $$\vec{z} = \langle \lambda, 2, 3 \rangle$$ that are coplanar. Since these are position vectors (or free vectors) that are coplanar, one of them can be expressed as a linear combination of the others. Equivalently, since four vectors in $$\mathbb{R}^3$$ are always linearly dependent, we interpret coplanarity as the condition that the vectors $$\vec{v} - \vec{u}$$, $$\vec{w} - \vec{u}$$, and $$\vec{z} - \vec{u}$$ are coplanar, meaning their scalar triple product is zero.
We compute $$\vec{v} - \vec{u} = \langle 3, -1, -8 \rangle$$, $$\vec{w} - \vec{u} = \langle -1, \lambda - 3, -1 \rangle$$, and $$\vec{z} - \vec{u} = \langle \lambda - 2, -1, -6 \rangle$$.
The scalar triple product equals the determinant: $$\begin{vmatrix} 3 & -1 & -8 \\ -1 & \lambda - 3 & -1 \\ \lambda - 2 & -1 & -6 \end{vmatrix} = 0$$.
Expanding along the first row: $$3[(\lambda - 3)(-6) - (-1)(-1)] - (-1)[(-1)(-6) - (-1)(\lambda - 2)] + (-8)[(-1)(-1) - (\lambda - 3)(\lambda - 2)] = 0$$.
We simplify each term. The first term gives $$3[-6\lambda + 18 - 1] = 3(-6\lambda + 17) = -18\lambda + 51$$. The second term gives $$1[6 - (-\lambda + 2)] = 1[6 + \lambda - 2] = \lambda + 4$$. The third term gives $$-8[1 - (\lambda^2 - 5\lambda + 6)] = -8[1 - \lambda^2 + 5\lambda - 6] = -8[-\lambda^2 + 5\lambda - 5] = 8\lambda^2 - 40\lambda + 40$$.
Adding all terms: $$-18\lambda + 51 + \lambda + 4 + 8\lambda^2 - 40\lambda + 40 = 0$$, which gives $$8\lambda^2 - 57\lambda + 95 = 0$$.
Using the quadratic formula: $$\lambda = \frac{57 \pm \sqrt{3249 - 3040}}{16} = \frac{57 \pm \sqrt{209}}{16}$$. However, we need the product of the roots. By Vieta's formulas, the product of all possible values of $$\lambda$$ is $$\frac{95}{8}$$.
Hence, the correct answer is Option D.
Let $$A$$, $$B$$, $$C$$ be three points whose position vectors respectively are:
$$\vec{a} = \hat{i} + 4\hat{j} + 3\hat{k}$$
$$\vec{b} = 2\hat{i} + \alpha\hat{j} + 4\hat{k}$$, $$\alpha \in R$$
$$\vec{c} = 3\hat{i} - 2\hat{j} + 5\hat{k}$$
If $$\alpha$$ is the smallest positive integer for which $$\vec{a}$$, $$\vec{b}$$, $$\vec{c}$$ are non-collinear, then the length of the median, through $$A$$, of $$\triangle ABC$$ is:
We have the vectors $$\vec{a} = \hat{i} + 4\hat{j} + 3\hat{k}$$, $$\vec{b} = 2\hat{i} + \alpha\hat{j} + 4\hat{k}$$ and $$\vec{c} = 3\hat{i} - 2\hat{j} + 5\hat{k}$$. Computing $$\vec{AB} = \vec{b} - \vec{a} = \hat{i} + (\alpha-4)\hat{j} + \hat{k}$$ and $$\vec{AC} = \vec{c} - \vec{a} = 2\hat{i} - 6\hat{j} + 2\hat{k}$$, we set $$\vec{AB} = \lambda\vec{AC}$$. From $$1 = 2\lambda$$ we get $$\lambda = 1/2$$, and $$\alpha - 4 = -6\times\frac12 = -3$$ gives $$\alpha = 1$$. Verifying $$1 = 2\times\frac12 = 1$$, so the points are collinear when $$\alpha = 1$$.
Since $$\alpha = 1$$ makes them collinear, the smallest positive integer for non-collinearity is $$\alpha = 2$$.
With $$\alpha = 2$$, the points are $$B = (2,2,4)$$ and $$C = (3,-2,5)$$. The midpoint of $$BC$$ is $$M = \left(\frac{2+3}{2},\frac{2-2}{2},\frac{4+5}{2}\right) = \left(\frac{5}{2},0,\frac{9}{2}\right)$$.
Writing $$A = (1,4,3)$$, the length of the median $$AM$$ is $$AM = \sqrt{\left(\frac{5}{2}-1\right)^2 + (0-4)^2 + \left(\frac{9}{2}-3\right)^2} = \sqrt{\left(\frac{3}{2}\right)^2 + 16 + \left(\frac{3}{2}\right)^2} = \sqrt{\frac{9}{4} + 16 + \frac{9}{4}} = \sqrt{\frac{9 + 64 + 9}{4}} = \frac{\sqrt{82}}{2}\,. $$
Therefore, the answer is Option A: $$\frac{\sqrt{82}}{2}$$.
Let $$ABC$$ be a triangle such that $$\vec{BC} = \vec{a}$$, $$\vec{CA} = \vec{b}$$, $$\vec{AB} = \vec{c}$$, $$|\vec{a}| = 6\sqrt{2}$$, $$|\vec{b}| = 2\sqrt{3}$$ and $$\vec{b} \cdot \vec{c} = 12$$. Consider the statements:
$$S_1: |\vec{a} \times (\vec{b} + \vec{c})| \times |\vec{b} - \vec{c}| = 6(2\sqrt{2} - 1)$$
$$S_2: \angle ABC = \cos^{-1}\sqrt{\dfrac{2}{3}}$$
Then
Let $$\mathbf{a}$$ and $$\mathbf{b}$$ be two unit vectors such that $$|\mathbf{a} + \mathbf{b}| + 2|\mathbf{a} \times \mathbf{b}| = 2$$. If $$\theta \in (0, \pi)$$ is the angle between $$\hat{a}$$ and $$\hat{b}$$, then among the statements:
$$(S1) : 2|\hat{a} \times \hat{b}| = |\hat{a} - \hat{b}|$$
$$(S2)$$ : The projection of $$\hat{a}$$ on $$(\hat{a} + \hat{b})$$ is $$\frac{1}{2}$$
Let S be the set of all $$a \in \mathbb{R}$$ for which the angle between the vectors $$\vec{u} = a(\log_e b)\hat{i} - 6\hat{j} + 3\hat{k}$$ and $$\vec{v} = (\log_e b)\hat{i} + 2\hat{j} + 2a(\log_e b)\hat{k}$$, $$(b > 1)$$ is acute. Then S is equal to
We need the angle between $$\vec{u} = a(\log_e b)\hat{i} - 6\hat{j} + 3\hat{k}$$ and $$\vec{v} = (\log_e b)\hat{i} + 2\hat{j} + 2a(\log_e b)\hat{k}$$ to be acute, where $$b > 1$$.
For the angle to be acute, we need $$\vec{u} \cdot \vec{v} > 0$$. Computing the dot product:
$$\vec{u} \cdot \vec{v} = a(\log_e b)^2 - 12 + 6a(\log_e b)$$
Let $$t = \log_e b$$. Since $$b > 1$$, we have $$t > 0$$. So we need:
$$at^2 + 6at - 12 > 0$$
for ALL $$t > 0$$ (since the condition must hold for every valid $$b > 1$$, meaning every $$t > 0$$).
Let $$f(t) = at^2 + 6at - 12$$. We need $$f(t) > 0$$ for all $$t > 0$$.
Case 1: If $$a = 0$$, then $$f(t) = -12 < 0$$. Not valid.
Case 2: If $$a > 0$$, the parabola opens upward. At $$t = 0$$: $$f(0) = -12 < 0$$. Since the function is continuous and negative at $$t = 0$$, by continuity $$f(t) < 0$$ for small positive $$t$$. So $$f(t) > 0$$ for ALL $$t > 0$$ fails.
Case 3: If $$a < 0$$, the parabola opens downward. As $$t \to \infty$$, $$f(t) \to -\infty$$. So $$f(t) > 0$$ for all $$t > 0$$ is impossible here too (since eventually $$f$$ becomes negative).
So there is no value of $$a$$ for which the angle is acute for all $$b > 1$$.
Hence, $$S = \emptyset$$, and the correct answer is Option B.
Let the vectors $$\vec{a} = (1+t)\hat{i} + (1-t)\hat{j} + \hat{k}$$, $$\vec{b} = (1-t)\hat{i} + (1+t)\hat{j} + 2\hat{k}$$ and $$\vec{c} = t\hat{i} - t\hat{j} + \hat{k}$$, $$t \in \mathbb{R}$$ be such that for $$\alpha, \beta, \gamma \in \mathbb{R}$$, $$\alpha\vec{a} + \beta\vec{b} + \gamma\vec{c} = \vec{0} \Rightarrow \alpha = \beta = \gamma = 0$$. Then, the set of all values of $$t$$ is
We need to find all values of $$t$$ for which the vectors $$\vec{a}$$, $$\vec{b}$$, $$\vec{c}$$ are linearly independent (i.e., $$\alpha\vec{a} + \beta\vec{b} + \gamma\vec{c} = \vec{0}$$ implies $$\alpha = \beta = \gamma = 0$$).
Since the vectors are linearly independent if and only if the determinant of the matrix formed by their components is non-zero, we consider:
$$D = \begin{vmatrix} 1+t & 1-t & 1 \\ 1-t & 1+t & 2 \\ t & -t & 1 \end{vmatrix}$$
Expanding this determinant along the first row gives:
$$D = (1+t)[(1+t)(1) - 2(-t)] - (1-t)[(1-t)(1) - 2t] + 1[(-t)(1-t) - t(1+t)]$$
This simplifies to:
$$= (1+t)(1+t+2t) - (1-t)(1-t-2t) + (-t+t^2 - t - t^2)$$
$$= (1+t)(1+3t) - (1-t)(1-3t) + (-2t)$$
$$= (1 + 3t + t + 3t^2) - (1 - 3t - t + 3t^2) - 2t$$
$$= (1 + 4t + 3t^2) - (1 - 4t + 3t^2) - 2t$$
$$= 8t - 2t = 6t$$
From the above, the determinant is $$D = 6t$$, so the vectors are linearly independent exactly when $$D \neq 0$$, that is, when $$6t \neq 0$$, or equivalently $$t \neq 0$$.
Therefore, the set of all such values of $$t$$ is $$\mathbb{R} - \{0\}$$.
The answer is Option C.
Let $$\vec{a} = 3\hat{i} + \hat{j}$$ and $$\vec{b} = \hat{i} + 2\hat{j} + \hat{k}$$. Let $$\vec{c}$$ be a vector satisfying $$\vec{a} \times (\vec{b} \times \vec{c}) = \vec{b} + \lambda\vec{c}$$. If $$\vec{b}$$ and $$\vec{c}$$ are non-parallel, then the value of $$\lambda$$ is
We have $$\vec{a} = 3\hat{i} + \hat{j}$$, $$\vec{b} = \hat{i} + 2\hat{j} + \hat{k}$$, and the relation $$\vec{a} \times (\vec{b} \times \vec{c}) = \vec{b} + \lambda\vec{c}$$.
We apply the BAC-CAB identity for the vector triple product: $$\vec{a} \times (\vec{b} \times \vec{c}) = \vec{b}(\vec{a} \cdot \vec{c}) - \vec{c}(\vec{a} \cdot \vec{b})$$.
We compute $$\vec{a} \cdot \vec{b} = 3(1) + 1(2) + 0(1) = 5$$. So the equation becomes:
$$\vec{b}(\vec{a} \cdot \vec{c}) - 5\vec{c} = \vec{b} + \lambda\vec{c}$$
Rearranging: $$(\vec{a} \cdot \vec{c} - 1)\vec{b} = (5 + \lambda)\vec{c}$$.
Since $$\vec{b}$$ and $$\vec{c}$$ are non-parallel, neither can be expressed as a scalar multiple of the other. The only way the equation $$(\vec{a} \cdot \vec{c} - 1)\vec{b} = (5 + \lambda)\vec{c}$$ can hold with $$\vec{b}$$ and $$\vec{c}$$ non-parallel is if both coefficients are zero. That is, $$\vec{a} \cdot \vec{c} - 1 = 0$$ and $$5 + \lambda = 0$$.
From the second condition, $$\lambda = -5$$.
Hence, the correct answer is Option A.
Let $$\vec{a} = \alpha\hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = 2\hat{i} + \hat{j} - \alpha\hat{k}$$, $$\alpha > 0$$. If the projection of $$\vec{a} \times \vec{b}$$ on the vector $$-\hat{i} + 2\hat{j} - 2\hat{k}$$ is $$30$$, then $$\alpha$$ is equal to
We need to find $$\alpha$$ given that the projection of $$\vec{a} \times \vec{b}$$ on $$-\hat{i} + 2\hat{j} - 2\hat{k}$$ is 30.
First, with $$\vec{a} = \alpha\hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = 2\hat{i} + \hat{j} - \alpha\hat{k}$$, we compute $$\vec{a} \times \vec{b}$$:
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \alpha & 1 & -1 \\ 2 & 1 & -\alpha \end{vmatrix}$$
$$= \hat{i}(1 \cdot (-\alpha) - (-1) \cdot 1) - \hat{j}(\alpha \cdot (-\alpha) - (-1) \cdot 2) + \hat{k}(\alpha \cdot 1 - 1 \cdot 2)$$
$$= \hat{i}(-\alpha + 1) - \hat{j}(-\alpha^2 + 2) + \hat{k}(\alpha - 2)$$
$$= (1 - \alpha)\hat{i} + (\alpha^2 - 2)\hat{j} + (\alpha - 2)\hat{k}$$
Next, let $$\vec{c} = -\hat{i} + 2\hat{j} - 2\hat{k}$$ so that $$|\vec{c}| = \sqrt{1 + 4 + 4} = 3$$, and compute the projection of $$\vec{a} \times \vec{b}$$ on $$\vec{c}$$:
Projection = $$\dfrac{(\vec{a} \times \vec{b}) \cdot \vec{c}}{|\vec{c}|}$$
$$ (\vec{a} \times \vec{b}) \cdot \vec{c} = (1 - \alpha)(-1) + (\alpha^2 - 2)(2) + (\alpha - 2)(-2)$$
$$= -(1 - \alpha) + 2\alpha^2 - 4 - 2\alpha + 4$$
$$= -1 + \alpha + 2\alpha^2 - 4 - 2\alpha + 4$$
$$= 2\alpha^2 - \alpha - 1$$
Then substituting into the projection formula gives $$\dfrac{2\alpha^2 - \alpha - 1}{3} = 30$$, which leads to $$2\alpha^2 - \alpha - 1 = 90$$ and hence $$2\alpha^2 - \alpha - 91 = 0$$.
Finally, solving $$2\alpha^2 - \alpha - 91 = 0$$ yields $$\alpha = \dfrac{1 \pm \sqrt{1 + 728}}{4} = \dfrac{1 \pm \sqrt{729}}{4} = \dfrac{1 \pm 27}{4}$$, so $$\alpha = \dfrac{28}{4} = 7$$ or $$\alpha = \dfrac{-26}{4}$$ (rejected since $$\alpha > 0$$).
The correct answer is Option D: $$\alpha = 7$$.
Let $$\vec{a}$$ and $$\vec{b}$$ be the vectors along the diagonal of a parallelogram having area $$2\sqrt{2}$$. Let the angle between $$\vec{a}$$ and $$\vec{b}$$ be acute. $$|\vec{a}| = 1$$ and $$|\vec{a} \cdot \vec{b}| = |\vec{a} \times \vec{b}|$$. If $$\vec{c} = 2\sqrt{2}(\vec{a} \times \vec{b}) - 2\vec{b}$$, then an angle between $$\vec{b}$$ and $$\vec{c}$$ is
Let $$\vec{a} = \hat{i} - \hat{j} + 2\hat{k}$$ and let $$\vec{b}$$ be a vector such that $$\vec{a} \times \vec{b} = 2\hat{i} - \hat{k}$$ and $$\vec{a} \cdot \vec{b} = 3$$. Then the projection of $$\vec{b}$$ on the vector $$\vec{a} - \vec{b}$$ is:
We are given $$\vec{a} = \hat{i} - \hat{j} + 2\hat{k}$$, $$\vec{a} \times \vec{b} = 2\hat{i} - \hat{k}$$, and $$\vec{a} \cdot \vec{b} = 3$$. To determine $$\vec{b}$$, let $$\vec{b}=(b_1,b_2,b_3)$$. The cross product in component form becomes
$$ (-b_3 - 2b_2,\;2b_1 - b_3,\;b_1 + b_2) \;=\;(2,0,-1) $$Equating components gives
$$-b_3 - 2b_2 = 2\quad(i),\qquad 2b_1 - b_3 = 0\quad(ii),\qquad b_1 + b_2 = -1\quad(iii).$$
From (ii) we have $$b_3 = 2b_1$$, and from (iii) $$b_2 = -1 - b_1$$. Substituting these into the dot-product condition $$\vec{a}\cdot\vec{b}=3$$ yields
$$b_1 - b_2 + 2b_3 = 3 \;\implies\; b_1 + 1 + b_1 + 4b_1 = 3 \;\implies\; 6b_1 = 2 \;\implies\; b_1 = \tfrac{1}{3}.$$
Thus
$$\vec{b}=\Bigl(\tfrac{1}{3},\,-\tfrac{4}{3},\,\tfrac{2}{3}\Bigr).$$
Subtracting this from $$\vec{a}$$ gives
$$\vec{a}-\vec{b}=\Bigl(\tfrac{2}{3},\;\tfrac{1}{3},\;\tfrac{4}{3}\Bigr).$$
Next, the scalar product of $$\vec{b}$$ with $$\vec{a}-\vec{b}$$ is
$$ \frac{1}{3}\cdot\frac{2}{3} \;+\;\bigl(-\tfrac{4}{3}\bigr)\cdot\tfrac{1}{3} \;+\;\tfrac{2}{3}\cdot\tfrac{4}{3} \;=\;\frac{2}{9}-\frac{4}{9}+\frac{8}{9} \;=\;\frac{6}{9} \;=\;\frac{2}{3}. $$The magnitude of $$\vec{a}-\vec{b}$$ is
$$ \sqrt{\frac{4}{9}+\frac{1}{9}+\frac{16}{9}} \;=\;\sqrt{\frac{21}{9}} \;=\;\frac{\sqrt{21}}{3}. $$Therefore, the projection of $$\vec{b}$$ onto $$\vec{a}-\vec{b}$$ is
$$ \frac{\vec{b}\cdot(\vec{a}-\vec{b})}{\bigl|\vec{a}-\vec{b}\bigr|} \;=\;\frac{\tfrac{2}{3}}{\tfrac{\sqrt{21}}{3}} \;=\;\frac{2}{\sqrt{21}}. $$The answer is Option A: $$\dfrac{2}{\sqrt{21}}$$.
Let $$\vec{a} = \hat{i} + \hat{j} - \hat{k}$$ and $$\vec{c} = 2\hat{i} - 3\hat{j} + 2\hat{k}$$. Then the number of vectors $$\vec{b}$$ such that $$\vec{b} \times \vec{c} = \vec{a}$$ and $$|\vec{b}| \in \{1, 2, \ldots, 10\}$$ is
We are given $$\vec{a} = \hat{i} + \hat{j} - \hat{k}$$ and $$\vec{c} = 2\hat{i} - 3\hat{j} + 2\hat{k}$$. We need to find the number of vectors $$\vec{b}$$ such that $$\vec{b} \times \vec{c} = \vec{a}$$ and $$|\vec{b}| \in \{1, 2, \ldots, 10\}$$.
First, for the cross product equation $$\vec{b} \times \vec{c} = \vec{a}$$ to have a solution, $$\vec{a}$$ must be perpendicular to $$\vec{c}$$ because $$\vec{b} \times \vec{c}$$ is always perpendicular to $$\vec{c}$$.
Now, computing the dot product gives $$\vec{a} \cdot \vec{c} = (1)(2) + (1)(-3) + (-1)(2) = 2 - 3 - 2 = -3 \neq 0$$.
Since $$\vec{a} \cdot \vec{c} \neq 0$$, $$\vec{a}$$ is not perpendicular to $$\vec{c}$$, and consequently there is no vector $$\vec{b}$$ satisfying $$\vec{b} \times \vec{c} = \vec{a}$$.
The number of such vectors $$\vec{b}$$ is $$0$$.
The answer is Option A: $$0$$.
Let a vector $$\vec{a}$$ has magnitude 9. Let a vector $$\vec{b}$$ be such that for every $$(x, y) \in \mathbb{R} \times \mathbb{R} - \{(0,0)\}$$, the vector $$x\vec{a} + y\vec{b}$$ is perpendicular to the vector $$6y\vec{a} - 18x\vec{b}$$. Then the value of $$|\vec{a} \times \vec{b}|$$ is equal to
We are given $$|\vec{a}| = 9$$ and for every $$(x, y) \neq (0, 0)$$, the vector $$(x\vec{a} + y\vec{b})$$ is perpendicular to $$(6y\vec{a} - 18x\vec{b})$$.
Since perpendicular vectors have zero dot product, we have $$(x\vec{a} + y\vec{b}) \cdot (6y\vec{a} - 18x\vec{b}) = 0$$. Expanding the dot product gives $$6xy|\vec{a}|^2 - 18x^2(\vec{a} \cdot \vec{b}) + 6y^2(\vec{a} \cdot \vec{b}) - 18xy|\vec{b}|^2 = 0$$, which can be grouped as $$6xy(|\vec{a}|^2 - 3|\vec{b}|^2) + 6(y^2 - 3x^2)(\vec{a} \cdot \vec{b}) = 0$$.
Because this identity holds for all $$(x, y) \neq (0,0)$$, the coefficients of the monomials must each vanish. Substituting $$x = 1, y = 0$$ into the grouped expression yields $$6(0 - 3)(\vec{a} \cdot \vec{b}) = 0$$, so $$\vec{a} \cdot \vec{b} = 0$$. Similarly, substituting $$x = 1, y = 1$$ gives $$6(|\vec{a}|^2 - 3|\vec{b}|^2) = 0$$, hence $$|\vec{a}|^2 = 3|\vec{b}|^2$$.
Using the given value of $$|\vec{a}|$$, we have $$81 = 3|\vec{b}|^2$$, which implies $$|\vec{b}|^2 = 27$$ and therefore $$|\vec{b}| = 3\sqrt{3}$$.
Since $$\vec{a} \cdot \vec{b} = 0$$, the vectors are perpendicular (θ = 90°). It follows that $$|\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}|\sin(90°) = 9 \times 3\sqrt{3} \times 1 = 27\sqrt{3}$$.
The answer is Option B.
Let $$\hat{a}$$ and $$\hat{b}$$ be two unit vectors such that the angle between them is $$\frac{\pi}{4}$$. If $$\theta$$ is the angle between the vectors $$(\hat{a} + \hat{b})$$ and $$(\hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b}))$$ then the value of $$164\cos^2\theta$$ is equal to
We have two unit vectors $$\hat{a}$$ and $$\hat{b}$$ with the angle between them equal to $$\frac{\pi}{4}$$, so $$|\hat{a}| = |\hat{b}| = 1$$ and $$\hat{a} \cdot \hat{b} = \cos\frac{\pi}{4} = \frac{1}{\sqrt{2}}$$. Also, $$|\hat{a} \times \hat{b}| = \sin\frac{\pi}{4} = \frac{1}{\sqrt{2}}$$.
We define $$\vec{p} = \hat{a} + \hat{b}$$ and $$\vec{q} = \hat{a} + 2\hat{b} + 2(\hat{a} \times \hat{b})$$, and we need to find $$164\cos^2\theta$$ where $$\theta$$ is the angle between $$\vec{p}$$ and $$\vec{q}$$.
We compute $$|\vec{p}|^2 = |\hat{a}|^2 + 2(\hat{a}\cdot\hat{b}) + |\hat{b}|^2 = 1 + \frac{2}{\sqrt{2}} + 1 = 2 + \sqrt{2}$$.
Now we find $$|\vec{q}|^2$$. We note that $$\hat{a} \times \hat{b}$$ is perpendicular to both $$\hat{a}$$ and $$\hat{b}$$, so $$\hat{a} \cdot (\hat{a} \times \hat{b}) = 0$$ and $$\hat{b} \cdot (\hat{a} \times \hat{b}) = 0$$.
$$|\vec{q}|^2 = |\hat{a} + 2\hat{b}|^2 + 4|\hat{a}\times\hat{b}|^2 = \left(1 + 4\cdot\frac{1}{\sqrt{2}} + 4\right) + 4\cdot\frac{1}{2} = 5 + 2\sqrt{2} + 2 = 7 + 2\sqrt{2} + 2\sqrt{2} = 5 + 4\cdot\frac{1}{\sqrt{2}} + 4 + 2$$
Let me compute this more carefully. $$|\hat{a}+2\hat{b}|^2 = 1 + 4(\hat{a}\cdot\hat{b}) + 4 = 5 + \frac{4}{\sqrt{2}} = 5 + 2\sqrt{2}$$. And $$|2(\hat{a}\times\hat{b})|^2 = 4\cdot\frac{1}{2} = 2$$. Since $$(\hat{a}+2\hat{b})$$ is perpendicular to $$2(\hat{a}\times\hat{b})$$, we get $$|\vec{q}|^2 = 5 + 2\sqrt{2} + 2 = 7 + 2\sqrt{2}$$.
Next, $$\vec{p}\cdot\vec{q} = (\hat{a}+\hat{b})\cdot(\hat{a}+2\hat{b}+2(\hat{a}\times\hat{b})) = (\hat{a}+\hat{b})\cdot(\hat{a}+2\hat{b}) + 0$$, since $$(\hat{a}+\hat{b})\cdot(\hat{a}\times\hat{b}) = 0$$ (as $$\hat{a}\times\hat{b}$$ is perpendicular to both $$\hat{a}$$ and $$\hat{b}$$).
$$\vec{p}\cdot\vec{q} = \hat{a}\cdot\hat{a} + 2(\hat{a}\cdot\hat{b}) + \hat{b}\cdot\hat{a} + 2(\hat{b}\cdot\hat{b}) = 1 + \frac{2}{\sqrt{2}} + \frac{1}{\sqrt{2}} + 2 = 3 + \frac{3}{\sqrt{2}} = 3 + \frac{3\sqrt{2}}{2}$$
Now $$\cos^2\theta = \frac{(\vec{p}\cdot\vec{q})^2}{|\vec{p}|^2\,|\vec{q}|^2}$$.
We compute the numerator: $$\left(3 + \frac{3\sqrt{2}}{2}\right)^2 = 9 + 2\cdot 3\cdot\frac{3\sqrt{2}}{2} + \frac{9\cdot 2}{4} = 9 + 9\sqrt{2} + \frac{9}{2} = \frac{27}{2} + 9\sqrt{2} = \frac{27 + 18\sqrt{2}}{2}$$.
The denominator: $$(2+\sqrt{2})(7+2\sqrt{2}) = 14 + 4\sqrt{2} + 7\sqrt{2} + 2\cdot 2 = 14 + 11\sqrt{2} + 4 = 18 + 11\sqrt{2}$$.
So $$\cos^2\theta = \frac{27 + 18\sqrt{2}}{2(18+11\sqrt{2})}$$.
We rationalize by multiplying numerator and denominator by $$(18 - 11\sqrt{2})$$:
Denominator factor: $$(18+11\sqrt{2})(18-11\sqrt{2}) = 324 - 242 = 82$$.
Numerator factor: $$(27+18\sqrt{2})(18-11\sqrt{2}) = 486 - 297\sqrt{2} + 324\sqrt{2} - 198\cdot 2 = 486 - 396 + (324-297)\sqrt{2} = 90 + 27\sqrt{2}$$.
So $$\cos^2\theta = \frac{90+27\sqrt{2}}{2\cdot 82} = \frac{90+27\sqrt{2}}{164}$$.
Therefore $$164\cos^2\theta = 90 + 27\sqrt{2}$$.
Hence, the correct answer is Option A.
Let $$\hat{a}, \hat{b}$$ be unit vectors. If $$\vec{c}$$ be a vector such that the angle between $$\hat{a}$$ and $$\vec{c}$$ is $$\frac{\pi}{12}$$, and $$\hat{b} = \vec{c} + 2(\vec{c} \times \hat{a})$$, then $$|6\vec{c}|^2$$ is equal to:
Let $$\hat{a}$$ and $$\hat{b}$$ be unit vectors, and $$\vec{c}$$ be a vector such that the angle between $$\hat{a}$$ and $$\vec{c}$$ is $$\frac{\pi}{12}$$, and $$\hat{b} = \vec{c} + 2(\vec{c} \times \hat{a})$$.
Take the magnitude squared of both sides.
$$|\hat{b}|^2 = |\vec{c} + 2(\vec{c} \times \hat{a})|^2$$
$$1 = |\vec{c}|^2 + 4|\vec{c} \times \hat{a}|^2 + 4\vec{c} \cdot (\vec{c} \times \hat{a})$$
Simplify the cross terms.
The scalar triple product $$\vec{c} \cdot (\vec{c} \times \hat{a}) = 0$$ (since it involves two identical vectors in the triple product).
$$|\vec{c} \times \hat{a}|^2 = |\vec{c}|^2 \sin^2\left(\frac{\pi}{12}\right)$$
Substitute and simplify.
$$1 = |\vec{c}|^2 + 4|\vec{c}|^2 \sin^2\left(\frac{\pi}{12}\right) = |\vec{c}|^2\left(1 + 4\sin^2\frac{\pi}{12}\right)$$
Compute $$\sin^2\left(\frac{\pi}{12}\right)$$.
Using the identity $$\sin^2\theta = \frac{1 - \cos 2\theta}{2}$$:
$$\sin^2\frac{\pi}{12} = \frac{1 - \cos\frac{\pi}{6}}{2} = \frac{1 - \frac{\sqrt{3}}{2}}{2} = \frac{2 - \sqrt{3}}{4}$$
Find the coefficient.
$$1 + 4 \cdot \frac{2 - \sqrt{3}}{4} = 1 + 2 - \sqrt{3} = 3 - \sqrt{3}$$
$$|\vec{c}|^2 = \frac{1}{3 - \sqrt{3}}$$
Compute $$|6\vec{c}|^2$$.
$$|6\vec{c}|^2 = 36|\vec{c}|^2 = \frac{36}{3 - \sqrt{3}}$$
Rationalizing: $$= \frac{36(3 + \sqrt{3})}{(3 - \sqrt{3})(3 + \sqrt{3})} = \frac{36(3 + \sqrt{3})}{9 - 3} = \frac{36(3 + \sqrt{3})}{6} = 6(3 + \sqrt{3})$$
Answer: Option B
Let $$\vec{a} = a_1\hat{i} + a_2\hat{j} + a_3\hat{k}, a_i > 0, i = 1, 2, 3$$ be a vector which makes equal angles with the coordinate axes $$OX, OY$$ and $$OZ$$. Also, let the projection of $$\vec{a}$$ on the vector $$3\hat{i} + 4\hat{j}$$ be $$7$$. Let $$\vec{b}$$ be a vector obtained by rotating $$\vec{a}$$ with $$90°$$. If $$\vec{a}, \vec{b}$$ and x-axis are coplanar, then projection of a vector $$\vec{b}$$ on $$3\hat{i} + 4\hat{j}$$ is equal to
We begin by noting that $$\vec{a} = a_1\hat{i} + a_2\hat{j} + a_3\hat{k}$$ with each $$a_i > 0$$ and that it makes equal angles with the coordinate axes. Consequently, $$a_1 = a_2 = a_3 = k$$ for some $$k > 0$$. The projection of $$\vec{a}$$ on $$3\hat{i} + 4\hat{j}$$ is given by
$$ \frac{\vec{a} \cdot (3\hat{i} + 4\hat{j})}{|3\hat{i} + 4\hat{j}|} = \frac{3k + 4k}{5} = \frac{7k}{5} = 7 $$
which implies $$k = 5$$ and hence $$\vec{a} = 5\hat{i} + 5\hat{j} + 5\hat{k}$$.
Next, to determine $$\vec{b}$$ we observe that rotating $$\vec{a}$$ by $$90°$$ preserves its magnitude, so $$|\vec{b}| = |\vec{a}| = 5\sqrt{3}$$ while also ensuring $$\vec{a} \cdot \vec{b} = 0$$. Because $$\vec{a}$$, $$\vec{b}$$, and the x-axis are coplanar, $$\vec{b}$$ lies in the plane spanned by $$\vec{a}$$ and $$\hat{i}$$. Thus we may write
$$ \vec{b} = \alpha\vec{a} + \beta\hat{i} $$
Then, imposing the orthogonality condition $$\vec{a} \cdot \vec{b} = 0$$ yields
$$ \alpha|\vec{a}|^2 + \beta(\vec{a} \cdot \hat{i}) = 0 \implies 75\alpha + 5\beta = 0 \implies \beta = -15\alpha $$
Hence $$\vec{b} = \alpha(5,5,5) + (-15\alpha)(1,0,0) = \alpha(-10,5,5)$$. Next, enforcing the magnitude condition $$|\vec{b}| = 5\sqrt{3}$$ gives
$$ \alpha^2(100+25+25) = 75 \implies 150\alpha^2 = 75 \implies \alpha = \pm\frac{1}{\sqrt{2}} $$
Therefore
$$ \vec{b} = \pm\frac{1}{\sqrt{2}}(-10,5,5) $$
and its projection on $$3\hat{i} + 4\hat{j}$$ is
$$ \text{Projection} = \frac{\vec{b} \cdot (3\hat{i} + 4\hat{j})}{5} = \frac{\pm\frac{1}{\sqrt{2}}(-30+20)}{5} = \frac{\pm\frac{1}{\sqrt{2}}\cdot(-10)}{5} = \frac{\mp10}{5\sqrt{2}} = \mp\sqrt{2} $$
Taking the positive value yields $$\sqrt{2}$$.
The answer is Option B: $$\sqrt{2}$$.
Let $$\vec{a} = \alpha \hat{i} + 2\hat{j} - \hat{k}$$ and $$\vec{b} = -2\hat{i} + \alpha \hat{j} + \hat{k}$$, where $$\alpha \in \mathbf{R}$$. If the area of the parallelogram whose adjacent sides are represented by the vectors $$\vec{a}$$ and $$\vec{b}$$ is $$\sqrt{15(\alpha^2 + 4)}$$, then the value of $$2|\vec{a}|^2 + (\vec{a} \cdot \vec{b})|\vec{b}|^2$$ is equal to
We have $$\vec{a} = \alpha\hat{i} + 2\hat{j} - \hat{k}$$ and $$\vec{b} = -2\hat{i} + \alpha\hat{j} + \hat{k}$$.
Compute $$\vec{a} \times \vec{b}$$:
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \alpha & 2 & -1 \\ -2 & \alpha & 1 \end{vmatrix}$$
$$= \hat{i}(2 + \alpha) - \hat{j}(\alpha - 2) + \hat{k}(\alpha^2 + 4)$$
Find the area condition:
$$|\vec{a} \times \vec{b}|^2 = (\alpha + 2)^2 + (\alpha - 2)^2 + (\alpha^2 + 4)^2$$
$$= \alpha^2 + 4\alpha + 4 + \alpha^2 - 4\alpha + 4 + \alpha^4 + 8\alpha^2 + 16$$
$$= \alpha^4 + 10\alpha^2 + 24$$
Given area = $$\sqrt{15(\alpha^2 + 4)}$$, so:
$$|\vec{a} \times \vec{b}|^2 = 15(\alpha^2 + 4) = 15\alpha^2 + 60$$
Setting equal: $$\alpha^4 + 10\alpha^2 + 24 = 15\alpha^2 + 60$$
$$\alpha^4 - 5\alpha^2 - 36 = 0$$
Solve for $$\alpha$$:
Let $$u = \alpha^2$$: $$u^2 - 5u - 36 = 0$$
$$(u - 9)(u + 4) = 0$$
Since $$u = \alpha^2 \geq 0$$: $$\alpha^2 = 9$$, so $$\alpha = \pm 3$$.
Compute the required expression:
$$|\vec{a}|^2 = \alpha^2 + 4 + 1 = 9 + 5 = 14$$
$$|\vec{b}|^2 = 4 + \alpha^2 + 1 = 4 + 9 + 1 = 14$$
$$\vec{a} \cdot \vec{b} = -2\alpha + 2\alpha - 1 = -1$$
$$2|\vec{a}|^2 + (\vec{a} \cdot \vec{b})|\vec{b}|^2 = 2(14) + (-1)(14) = 28 - 14 = 14$$
The correct answer is Option D: $$\boxed{14}$$.
Let $$\vec{a} = \hat{i} + \hat{j} + 2\hat{k}, \vec{b} = 2\hat{i} - 3\hat{j} + \hat{k}$$ and $$\vec{c} = \hat{i} - \hat{j} + \hat{k}$$ be the three given vectors. Let $$\vec{v}$$ be a vector in the plane of $$\vec{a}$$ and $$\vec{b}$$ whose projection on $$\vec{c}$$ is $$\frac{2}{\sqrt{3}}$$. If $$\vec{v} \cdot \hat{j} = 7$$, then $$\vec{v} \cdot (\hat{i} + \hat{k})$$ is equal to
Given $$\vec{a} = \hat{i} + \hat{j} + 2\hat{k}$$, $$\vec{b} = 2\hat{i} - 3\hat{j} + \hat{k}$$, and $$\vec{c} = \hat{i} - \hat{j} + \hat{k}$$.
First, we express $$\vec{v}$$ in the plane of $$\vec{a}$$ and $$\vec{b}$$ as $$\vec{v} = \lambda\vec{a} + \mu\vec{b} = (\lambda + 2\mu)\hat{i} + (\lambda - 3\mu)\hat{j} + (2\lambda + \mu)\hat{k}$$.
Next, using the condition $$\vec{v} \cdot \hat{j} = 7$$ yields $$\lambda - 3\mu = 7 \quad \cdots (1)$$.
Since the projection of $$\vec{v}$$ on $$\vec{c}$$ is $$\frac{\vec{v} \cdot \vec{c}}{|\vec{c}|} = \frac{2}{\sqrt{3}},$$ we note that $$|\vec{c}| = \sqrt{1+1+1} = \sqrt{3}$$ and
$$\vec{v} \cdot \vec{c} = (\lambda + 2\mu)(1) + (\lambda - 3\mu)(-1) + (2\lambda + \mu)(1) = \lambda + 2\mu - \lambda + 3\mu + 2\lambda + \mu = 2\lambda + 6\mu.$$
Therefore, $$\frac{2\lambda + 6\mu}{\sqrt{3}} = \frac{2}{\sqrt{3}} \implies 2\lambda + 6\mu = 2 \implies \lambda + 3\mu = 1 \quad \cdots (2).$$
Now, from (1) we have $$\lambda = 7 + 3\mu$$, and substituting into (2) gives $$7 + 3\mu + 3\mu = 1 \implies 6\mu = -6 \implies \mu = -1$$ and hence $$\lambda = 7 + 3(-1) = 4$$.
Substituting these into the expression for $$\vec{v}$$ yields $$\vec{v} = (4 + 2(-1))\hat{i} + (4 - 3(-1))\hat{j} + (8 + (-1))\hat{k} = 2\hat{i} + 7\hat{j} + 7\hat{k}$$.
Finally, computing the required dot product gives $$\vec{v} \cdot (\hat{i} + \hat{k}) = 2 + 7 = 9$$.
Hence the correct answer is Option D: $$9$$.
Let $$\vec{a}, \vec{b}, \vec{c}$$ be three coplanar concurrent vectors such that angles between any two of them is same. If the product of their magnitudes is 14 and $$(\vec{a} \times \vec{b}) \cdot (\vec{b} \times \vec{c}) + (\vec{b} \times \vec{c}) \cdot (\vec{c} \times \vec{a}) + (\vec{c} \times \vec{a}) \cdot (\vec{a} \times \vec{b}) = 168$$ then $$|\vec{a}| + |\vec{b}| + |\vec{c}|$$ is equal to
We have three coplanar concurrent vectors $$\vec{a}, \vec{b}, \vec{c}$$ such that the angle between any two of them is the same. Since they lie in a plane and radiate from a common point, the only configuration where all pairwise angles are equal is when each pair makes an angle of $$120°$$ with every other pair (as $$\frac{360°}{3} = 120°$$).
Let $$|\vec{a}| = a$$, $$|\vec{b}| = b$$, and $$|\vec{c}| = c$$. We are given that the product of magnitudes satisfies $$abc = 14$$.
Since all three vectors are coplanar, every cross product among them points in the same direction — perpendicular to the common plane. Let $$\hat{n}$$ be the unit normal to this plane. With the angle between each pair being $$120°$$ and $$\sin 120° = \frac{\sqrt{3}}{2}$$, we have $$\vec{a} \times \vec{b} = \frac{\sqrt{3}}{2}\,ab\,\hat{n}$$, $$\vec{b} \times \vec{c} = \frac{\sqrt{3}}{2}\,bc\,\hat{n}$$, and $$\vec{c} \times \vec{a} = \frac{\sqrt{3}}{2}\,ca\,\hat{n}$$. (All cross products point along $$\hat{n}$$ or $$-\hat{n}$$ depending on orientation, but the dot products of parallel vectors use the same sign consistently.)
Now we compute each dot product in the given expression. We have $$(\vec{a} \times \vec{b}) \cdot (\vec{b} \times \vec{c}) = \frac{\sqrt{3}}{2}\,ab \cdot \frac{\sqrt{3}}{2}\,bc = \frac{3}{4}\,ab^2c$$. Similarly, $$(\vec{b} \times \vec{c}) \cdot (\vec{c} \times \vec{a}) = \frac{3}{4}\,abc^2$$, and $$(\vec{c} \times \vec{a}) \cdot (\vec{a} \times \vec{b}) = \frac{3}{4}\,a^2bc$$.
Adding all three terms gives $$\frac{3}{4}\,abc(a + b + c) = \frac{3}{4} \times 14 \times (a + b + c) = \frac{21}{2}(a + b + c)$$.
Setting this equal to 168, we obtain $$\frac{21}{2}(a + b + c) = 168$$, which yields $$a + b + c = \frac{168 \times 2}{21} = 16$$.
Hence, the correct answer is Option C.
A vector $$\vec{a}$$ is parallel to the line of intersection of the plane determined by the vectors $$\hat{i}$$, $$\hat{i} + \hat{j}$$ and the plane determined by the vectors $$\hat{i} - \hat{j}$$, $$\hat{i} + \hat{k}$$. The obtuse angle between $$\vec{a}$$ and the vector $$\vec{b} = \hat{i} - 2\hat{j} + 2\hat{k}$$ is
We need to find the obtuse angle between $$\vec{a}$$ (parallel to the line of intersection of two planes) and $$\vec{b} = \hat{i} - 2\hat{j} + 2\hat{k}$$.
The first plane is determined by vectors $$\hat{i}$$ and $$\hat{i} + \hat{j}$$.
Normal to the first plane: $$\vec{n_1} = \hat{i} \times (\hat{i} + \hat{j}) = \hat{i} \times \hat{i} + \hat{i} \times \hat{j} = \vec{0} + \hat{k} = \hat{k}$$
So the first plane has normal $$\hat{k}$$, i.e., it is the $$xy$$-plane ($$z = 0$$).
The second plane is determined by vectors $$\hat{i} - \hat{j}$$ and $$\hat{i} + \hat{k}$$.
Normal to the second plane:
$$\vec{n_2} = (\hat{i} - \hat{j}) \times (\hat{i} + \hat{k}) = \begin{vmatrix}\hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & 0 \\ 1 & 0 & 1\end{vmatrix}$$
$$= \hat{i}(-1-0) - \hat{j}(1-0) + \hat{k}(0+1) = -\hat{i} - \hat{j} + \hat{k}$$
$$\vec{a}$$ is parallel to $$\vec{n_1} \times \vec{n_2}$$:
$$\vec{n_1} \times \vec{n_2} = \hat{k} \times (-\hat{i} - \hat{j} + \hat{k}) = -(\hat{k} \times \hat{i}) - (\hat{k} \times \hat{j}) + (\hat{k} \times \hat{k})$$
$$= -\hat{j} - (-\hat{i}) + \vec{0} = \hat{i} - \hat{j}$$
So $$\vec{a}$$ is parallel to $$\hat{i} - \hat{j}$$.
$$\cos\alpha = \dfrac{\vec{a} \cdot \vec{b}}{|\vec{a}||\vec{b}|} = \dfrac{(1)(1) + (-1)(-2) + (0)(2)}{\sqrt{1+1}\cdot\sqrt{1+4+4}} = \dfrac{1+2}{(\sqrt{2})(3)} = \dfrac{3}{3\sqrt{2}} = \dfrac{1}{\sqrt{2}}$$
The acute angle is $$\alpha = \dfrac{\pi}{4}$$.
The obtuse angle is $$\pi - \dfrac{\pi}{4} = \dfrac{3\pi}{4}$$.
The correct answer is Option A: $$\dfrac{3\pi}{4}$$.
If the plane $$P$$ passes through the intersection of two mutually perpendicular planes $$2x + ky - 5z = 1$$ and $$3kx - ky + z = 5$$, $$k < 3$$ and intercepts a unit length on positive $$x$$-axis, then the intercept made by the plane $$P$$ on the $$y$$-axis is
Let $$\vec{a}$$ be a vector which is perpendicular to the vector $$3\hat{i} + \frac{1}{2}\hat{j} + 2\hat{k}$$. If $$\vec{a} \times (2\hat{i} + \hat{k}) = 2\hat{i} - 13\hat{j} - 4\hat{k}$$, then the projection of the vector $$\vec{a}$$ on the vector $$2\hat{i} + 2\hat{j} + \hat{k}$$ is
Let $$\vec{a} = a_1\hat{i} + a_2\hat{j} + a_3\hat{k}$$. We are given two conditions.
Use the perpendicularity condition:
$$\vec{a} \cdot (3\hat{i} + \frac{1}{2}\hat{j} + 2\hat{k}) = 0$$
$$3a_1 + \frac{a_2}{2} + 2a_3 = 0 \quad \cdots (1)$$
Use the cross product condition:
$$\vec{a} \times (2\hat{i} + \hat{k}) = 2\hat{i} - 13\hat{j} - 4\hat{k}$$
$$\begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ a_1 & a_2 & a_3 \\ 2 & 0 & 1 \end{vmatrix} = (a_2 - 0)\hat{i} - (a_1 - 2a_3)\hat{j} + (0 - 2a_2)\hat{k}$$
$$= a_2\hat{i} - (a_1 - 2a_3)\hat{j} - 2a_2\hat{k}$$
Comparing components:
$$a_2 = 2 \quad \cdots (2)$$
$$-(a_1 - 2a_3) = -13 \implies a_1 - 2a_3 = 13 \quad \cdots (3)$$
$$-2a_2 = -4 \implies a_2 = 2 \quad \checkmark$$
Solve the system:
From equation (1): $$3a_1 + 1 + 2a_3 = 0 \implies 3a_1 + 2a_3 = -1 \quad \cdots (4)$$
From equation (3): $$a_1 = 13 + 2a_3$$
Substituting into (4): $$3(13 + 2a_3) + 2a_3 = -1$$
$$39 + 6a_3 + 2a_3 = -1$$
$$8a_3 = -40 \implies a_3 = -5$$
$$a_1 = 13 + 2(-5) = 3$$
So $$\vec{a} = 3\hat{i} + 2\hat{j} - 5\hat{k}$$.
Find the projection:
Projection of $$\vec{a}$$ on $$\vec{c} = 2\hat{i} + 2\hat{j} + \hat{k}$$:
$$\text{proj} = \frac{\vec{a} \cdot \vec{c}}{|\vec{c}|} = \frac{6 + 4 - 5}{\sqrt{4 + 4 + 1}} = \frac{5}{3}$$
The correct answer is Option C: $$\boxed{\dfrac{5}{3}}$$.
Let $$\theta$$ be the angle between the vectors $$\vec{a}$$ and $$\vec{b}$$, where $$|\vec{a}| = 4, |\vec{b}| = 3$$ and $$\theta \in \left[\frac{\pi}{4}, \frac{\pi}{3}\right]$$. Then $$|\vec{a} - \vec{b} \times \vec{a} + \vec{b}|^2 + 4|\vec{a} \cdot \vec{b}|^2$$ is equal to ______.
Given $$|\vec{a}| = 4$$, $$|\vec{b}| = 3$$ and $$\theta \in \left[\frac{\pi}{4}, \frac{\pi}{3}\right]$$, we wish to determine the value of $$|(\vec{a} - \vec{b}) \times (\vec{a} + \vec{b})|^2 + 4|\vec{a} \cdot \vec{b}|^2$$.
Expanding the cross product, we have $$(\vec{a} - \vec{b}) \times (\vec{a} + \vec{b}) = \vec{a} \times \vec{a} + \vec{a} \times \vec{b} - \vec{b} \times \vec{a} - \vec{b} \times \vec{b}.$$ Since $$\vec{a} \times \vec{a} = \vec{0}$$, $$\vec{b} \times \vec{b} = \vec{0}$$, and $$\vec{b} \times \vec{a} = -\,\vec{a} \times \vec{b},$$ this reduces to $$2(\vec{a} \times \vec{b}).$$
Therefore, the squared magnitude of this cross product is $$|2(\vec{a} \times \vec{b})|^2 = 4\,|\vec{a} \times \vec{b}|^2 = 4\,|\vec{a}|^2\,|\vec{b}|^2\sin^2\theta.$$
Similarly, the second term is $$4\,|\vec{a} \cdot \vec{b}|^2 = 4\,|\vec{a}|^2\,|\vec{b}|^2\cos^2\theta.$$
Adding these results gives $$4\,|\vec{a}|^2\,|\vec{b}|^2\bigl(\sin^2\theta + \cos^2\theta\bigr) = 4\,|\vec{a}|^2\,|\vec{b}|^2 = 4 \times 16 \times 9 = 576.$$ Hence, the required value is $$576$$.
Let $$\vec{a}$$ and $$\vec{b}$$ be two vectors such that $$|\vec{a}+\vec{b}|^2 = |\vec{a}|^2 + 2|\vec{b}|^2$$, $$\vec{a} \cdot \vec{b} = 3$$ and $$|\vec{a} \times \vec{b}|^2 = 75$$. Then $$|\vec{a}|^2$$ is equal to _____
We have $$|\vec{a} + \vec{b}|^2 = |\vec{a}|^2 + 2|\vec{b}|^2$$, $$\vec{a} \cdot \vec{b} = 3$$, and $$|\vec{a} \times \vec{b}|^2 = 75$$.
Expanding the first condition: $$|\vec{a}|^2 + 2(\vec{a} \cdot \vec{b}) + |\vec{b}|^2 = |\vec{a}|^2 + 2|\vec{b}|^2$$. This simplifies to $$2(\vec{a} \cdot \vec{b}) = |\vec{b}|^2$$, so $$|\vec{b}|^2 = 2 \times 3 = 6$$.
Now we use the identity $$|\vec{a} \times \vec{b}|^2 + (\vec{a} \cdot \vec{b})^2 = |\vec{a}|^2|\vec{b}|^2$$. Substituting: $$75 + 9 = |\vec{a}|^2 \times 6$$, so $$|\vec{a}|^2 = \frac{84}{6} = 14$$.
Hence, the correct answer is $$\boxed{14}$$.
Let $$\vec{b} = \hat{i} + \hat{j} + \lambda\hat{k}, \lambda \in \mathbb{R}$$. If $$\vec{a}$$ is a vector such that $$\vec{a} \times \vec{b} = 13\hat{i} - \hat{j} - 4\hat{k}$$ and $$\vec{a} \cdot \vec{b} + 21 = 0$$, then
$$\vec{b} - \vec{a} \cdot \hat{k} - \hat{j} + \vec{b} + \vec{a} \cdot \hat{i} - \hat{k}$$ is equal to ______
We have $$\vec{b} = \hat{i} + \hat{j} + \lambda\hat{k}$$, $$\vec{a} \times \vec{b} = 13\hat{i} - \hat{j} - 4\hat{k}$$, and $$\vec{a} \cdot \vec{b} + 21 = 0$$. Let $$\vec{a} = a_1\hat{i} + a_2\hat{j} + a_3\hat{k}$$. Computing $$\vec{a} \times \vec{b}$$ gives $$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ a_1 & a_2 & a_3 \\ 1 & 1 & \lambda \end{vmatrix} = (a_2\lambda - a_3)\hat{i} - (a_1\lambda - a_3)\hat{j} + (a_1 - a_2)\hat{k},$$ and equating this with $$13\hat{i} - \hat{j} - 4\hat{k}$$ yields $$a_2\lambda - a_3 = 13 \quad\cdots(1),$$ $$-(a_1\lambda - a_3) = -1 \implies a_3 - a_1\lambda = -1 \quad\cdots(2),$$ $$a_1 - a_2 = -4 \quad\cdots(3).$$
Adding (1) and (2) gives $$(a_2\lambda - a_3)+(a_3 - a_1\lambda)=13+(-1)\implies \lambda(a_2 - a_1)=12.$$ Since (3) gives $$a_2 - a_1=4$$, it follows that $$4\lambda=12$$ and hence $$\lambda=3$$.
The dot product condition $$\vec{a}\cdot\vec{b}=a_1+a_2+3a_3=-21\quad\cdots(4)$$ provides another relation. From (3) we have $$a_1=a_2-4$$, and substituting $$\lambda=3$$ into (1) gives $$3a_2 - a_3=13\implies a_3=3a_2-13$$. Substituting these into (4) yields $$(a_2 - 4)+a_2+3(3a_2 -13)=-21,$$ which simplifies to $$a_2 - 4 + a_2 +9a_2 -39=-21\implies 11a_2 -43=-21\implies 11a_2=22\implies a_2=2.$$ Therefore $$a_1=2-4=-2$$ and $$a_3=3\cdot2-13=-7$$, giving $$\vec{a}=-2\hat{i}+2\hat{j}-7\hat{k}$$ and $$\vec{b}=\hat{i}+\hat{j}+3\hat{k}$$.
It can be verified that $$\vec{a}\times\vec{b}=(2\cdot3-(-7))\hat{i}-((-2)\cdot3-(-7))\hat{j}+((-2)-2)\hat{k}=13\hat{i}-\hat{j}-4\hat{k},$$ and $$\vec{a}\cdot\vec{b}=-2+2-21=-21,$$ so indeed $$\vec{a}\cdot\vec{b}+21=0$$.
Finally, to compute $$(\vec{b}-\vec{a})\cdot(\hat{k}-\hat{j})+(\vec{b}+\vec{a})\cdot(\hat{i}-\hat{k}),$$ note that $$\vec{b}-\vec{a}=(1-(-2))\hat{i}+(1-2)\hat{j}+(3-(-7))\hat{k}=3\hat{i}-\hat{j}+10\hat{k},$$ so $$(\vec{b}-\vec{a})\cdot(\hat{k}-\hat{j})=0+1+10=11.$$ Also, $$\vec{b}+\vec{a}=(1+(-2))\hat{i}+(1+2)\hat{j}+(3+(-7))\hat{k}=-\hat{i}+3\hat{j}-4\hat{k},$$ and $$(\vec{b}+\vec{a})\cdot(\hat{i}-\hat{k})=-1+0+4=3.$$ Therefore the total is $$11+3=14\text{.}$$
The answer is $$\boxed{14}$$.
If $$\vec{a} = 2\hat{i} + \hat{j} + 3\hat{k}, \vec{b} = 3\hat{i} + 3\hat{j} + \hat{k}$$ and $$\vec{c} = c_1\hat{i} + c_2\hat{j} + c_3\hat{k}$$ are coplanar vectors and $$\vec{a} \cdot \vec{c} = 5, \vec{b} \perp \vec{c}$$, then $$122(c_1 + c_2 + c_3)$$ is equal to ______
Given $$\vec{a} = 2\hat{i} + \hat{j} + 3\hat{k}$$, $$\vec{b} = 3\hat{i} + 3\hat{j} + \hat{k}$$, and $$\vec{c} = c_1\hat{i} + c_2\hat{j} + c_3\hat{k}$$.
Conditions: $$\vec{a}, \vec{b}, \vec{c}$$ are coplanar, $$\vec{a} \cdot \vec{c} = 5$$, and $$\vec{b} \perp \vec{c}$$.
Since the vectors are coplanar: $$\vec{c} = \lambda \vec{a} + \mu \vec{b}$$ for some scalars $$\lambda, \mu$$.
$$\vec{c} = (2\lambda + 3\mu)\hat{i} + (\lambda + 3\mu)\hat{j} + (3\lambda + \mu)\hat{k}$$
From $$\vec{b} \perp \vec{c}$$: $$\vec{b} \cdot \vec{c} = 0$$
$$3(2\lambda + 3\mu) + 3(\lambda + 3\mu) + 1(3\lambda + \mu) = 0$$
$$6\lambda + 9\mu + 3\lambda + 9\mu + 3\lambda + \mu = 0$$
$$12\lambda + 19\mu = 0 \implies \lambda = -\frac{19\mu}{12}$$
From $$\vec{a} \cdot \vec{c} = 5$$:
$$2(2\lambda + 3\mu) + 1(\lambda + 3\mu) + 3(3\lambda + \mu) = 5$$
$$4\lambda + 6\mu + \lambda + 3\mu + 9\lambda + 3\mu = 5$$
$$14\lambda + 12\mu = 5$$
Substituting $$\lambda = -\frac{19\mu}{12}$$:
$$14 \cdot \left(-\frac{19\mu}{12}\right) + 12\mu = 5$$
$$-\frac{266\mu}{12} + 12\mu = 5$$
$$-\frac{133\mu}{6} + 12\mu = 5$$
$$\frac{-133\mu + 72\mu}{6} = 5$$
$$\frac{-61\mu}{6} = 5$$
$$\mu = -\frac{30}{61}$$
$$\lambda = -\frac{19}{12} \cdot \left(-\frac{30}{61}\right) = \frac{19 \times 30}{12 \times 61} = \frac{570}{732} = \frac{95}{122}$$
Now computing $$c_1 + c_2 + c_3$$:
$$c_1 + c_2 + c_3 = (2\lambda + 3\mu) + (\lambda + 3\mu) + (3\lambda + \mu) = 6\lambda + 7\mu$$
$$= 6 \cdot \frac{95}{122} + 7 \cdot \left(-\frac{30}{61}\right) = \frac{570}{122} - \frac{210}{61} = \frac{570}{122} - \frac{420}{122} = \frac{150}{122} = \frac{75}{61}$$
$$122(c_1 + c_2 + c_3) = 122 \times \frac{75}{61} = 2 \times 75 = 150$$
Hence the answer is $$\boxed{150}$$.
Let $$\vec{a} = \hat{i} - 2\hat{j} + 3\hat{k}$$, $$\vec{b} = \hat{i} + \hat{j} + \hat{k}$$ and $$\vec{c}$$ be a vector such that $$\vec{a} \times (\vec{b}+ \vec{c}) = \vec{0}$$, then the value of $$3(\vec{c} \cdot \vec{a})$$ is equal to ______.
We are given $$\vec{a} = \hat{i} - 2\hat{j} + 3\hat{k}, \vec{b} = \hat{i} + \hat{j} + \hat{k}, and a vector \vec{c} such that (\vec{a} + \vec{b}) \times \vec{c} = \vec{0} and \vec{b} \cdot \vec{c} = 5$$.
Adding these vectors, we obtain $$\vec{a} + \vec{b} = (1+1)\hat{i} + (-2+1)\hat{j} + (3+1)\hat{k} = 2\hat{i} - \hat{j} + 4\hat{k}. Since (\vec{a} + \vec{b}) \times \vec{c} = \vec{0} implies that \vec{c} is parallel to \vec{a} + \vec{b}, we set \vec{c} = t(\vec{a} + \vec{b}) = t(2\hat{i} - \hat{j} + 4\hat{k}) for some scalar t$$.
Imposing the condition $$\vec{b} \cdot \vec{c} = 5 gives \vec{b} \cdot \vec{c} = t\,\vec{b} \cdot (\vec{a} + \vec{b}) = t(\vec{b} \cdot \vec{a} + |\vec{b}|^2), where \vec{b} \cdot \vec{a} = 1 - 2 + 3 = 2 and |\vec{b}|^2 = 1 + 1 + 1 = 3. Hence, 5 = t(2 + 3) = 5t, leading to t = 1$$.
Therefore, $$\vec{c} = 2\hat{i} - \hat{j} + 4\hat{k}. Computing \vec{c} \cdot \vec{a} yields (2)(1) + (-1)(-2) + (4)(3) = 2 + 2 + 12 = 16. Consequently, 3(\vec{c} \cdot \vec{a}) = 3 \times 16 = 48$$.
Let $$\vec{a}, \vec{b}, \vec{c}$$ be three non-coplanar vectors such that $$\vec{a} \times \vec{b} = 4\vec{c}$$, $$\vec{b} \times \vec{c} = 9\vec{a}$$ and $$\vec{c} \times \vec{a} = \alpha\vec{b}$$, $$\alpha > 0$$. If $$|\vec{a}| + |\vec{b}| + |\vec{c}| = {36}$$, then $$\alpha$$ is equal to _______.
Let a vector $$\alpha\hat{i} + \beta\hat{j}$$ be obtained by rotating the vector $$\sqrt{3}\hat{i} + \hat{j}$$ by an angle 45° about the origin in counterclockwise direction in the first quadrant. Then the area (in sq. units) of triangle having vertices $$(\alpha, \beta)$$, $$(0, \beta)$$ and $$(0, 0)$$ is equal to:
The vector $$\sqrt{3}\hat{i} + \hat{j}$$ has magnitude $$\sqrt{3 + 1} = 2$$ and makes an angle $$\theta = \tan^{-1}\left(\frac{1}{\sqrt{3}}\right) = 30°$$ with the positive x-axis.
Rotating this vector by $$45°$$ counterclockwise gives a new angle of $$30° + 45° = 75°$$. The magnitude remains 2, so the new vector is $$\alpha\hat{i} + \beta\hat{j} = 2\cos 75°\hat{i} + 2\sin 75°\hat{j}$$.
The triangle has vertices $$(\alpha, \beta)$$, $$(0, \beta)$$, and $$(0, 0)$$. This is a right triangle with the right angle at $$(0, \beta)$$, with base along the y-axis of length $$|\beta|$$ and horizontal side of length $$|\alpha|$$.
The area is $$\frac{1}{2}|\alpha||\beta| = \frac{1}{2} \cdot 2\cos 75° \cdot 2\sin 75° = 2\cos 75°\sin 75° = \sin 150° = \frac{1}{2}$$.
Let a vector $$\vec{a}$$ be coplanar with vectors $$\vec{b} = 2\hat{i} + \hat{j} + \hat{k}$$ and $$\vec{c} = \hat{i} - \hat{j} + \hat{k}$$. If $$\vec{a}$$ is perpendicular to $$\vec{d} = 3\hat{i} + 2\hat{j} + 6\hat{k}$$, and $$|\vec{a}| = \sqrt{10}$$. Then a possible value of $$[\vec{a} \ \vec{b} \ \vec{c}] + [\vec{a} \ \vec{b} \ \vec{d}] + [\vec{a} \ \vec{c} \ \vec{d}]$$ is equal to:
Since $$\vec{a}$$ is coplanar with $$\vec{b} = 2\hat{i} + \hat{j} + \hat{k}$$ and $$\vec{c} = \hat{i} - \hat{j} + \hat{k}$$, we can write $$\vec{a} = s\vec{b} + t\vec{c} = (2s + t)\hat{i} + (s - t)\hat{j} + (s + t)\hat{k}$$ for some scalars $$s, t$$.
The condition $$\vec{a} \perp \vec{d}$$ where $$\vec{d} = 3\hat{i} + 2\hat{j} + 6\hat{k}$$ gives $$\vec{a} \cdot \vec{d} = 3(2s + t) + 2(s - t) + 6(s + t) = 14s + 7t = 0$$, so $$t = -2s$$.
Substituting back: $$\vec{a} = (2s - 2s)\hat{i} + (s + 2s)\hat{j} + (s - 2s)\hat{k} = 3s\,\hat{j} - s\,\hat{k}$$. The magnitude condition $$|\vec{a}| = \sqrt{10}$$ gives $$\sqrt{9s^2 + s^2} = |s|\sqrt{10} = \sqrt{10}$$, so $$|s| = 1$$.
Taking $$s = 1$$: $$\vec{a} = (0, 3, -1)$$. Since $$\vec{a}$$ is coplanar with $$\vec{b}$$ and $$\vec{c}$$, the scalar triple product $$[\vec{a}\;\vec{b}\;\vec{c}] = 0$$.
For $$[\vec{a}\;\vec{b}\;\vec{d}] = \vec{a} \cdot (\vec{b} \times \vec{d})$$, compute $$\vec{b} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 1 & 1 \\ 3 & 2 & 6 \end{vmatrix} = (6 - 2)\hat{i} - (12 - 3)\hat{j} + (4 - 3)\hat{k} = 4\hat{i} - 9\hat{j} + \hat{k}$$. Then $$[\vec{a}\;\vec{b}\;\vec{d}] = (0)(4) + (3)(-9) + (-1)(1) = -28$$.
For $$[\vec{a}\;\vec{c}\;\vec{d}] = \vec{a} \cdot (\vec{c} \times \vec{d})$$, compute $$\vec{c} \times \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & 1 \\ 3 & 2 & 6 \end{vmatrix} = (-6 - 2)\hat{i} - (6 - 3)\hat{j} + (2 + 3)\hat{k} = -8\hat{i} - 3\hat{j} + 5\hat{k}$$. Then $$[\vec{a}\;\vec{c}\;\vec{d}] = (0)(-8) + (3)(-3) + (-1)(5) = -14$$.
The total is $$0 + (-28) + (-14) = -42$$.
If vectors $$\vec{a_1} = x\hat{i} - \hat{j} + \hat{k}$$ and $$\vec{a_2} = \hat{i} + y\hat{j} + z\hat{k}$$ are collinear, then a possible unit vector parallel to the vector $$x\hat{i} + y\hat{j} + z\hat{k}$$ is:
Since $$\vec{a_1} = x\hat{i} - \hat{j} + \hat{k}$$ and $$\vec{a_2} = \hat{i} + y\hat{j} + z\hat{k}$$ are collinear, there exists a scalar $$\lambda$$ such that $$\vec{a_2} = \lambda \vec{a_1}$$. Writing this component-wise: $$\hat{i} + y\hat{j} + z\hat{k} = \lambda(x\hat{i} - \hat{j} + \hat{k})$$.
Comparing the $$\hat{i}$$ component: $$1 = \lambda x$$, so $$\lambda = \frac{1}{x}$$.
Comparing the $$\hat{j}$$ component: $$y = -\lambda = -\frac{1}{x}$$.
Comparing the $$\hat{k}$$ component: $$z = \lambda = \frac{1}{x}$$.
Now we form the vector $$x\hat{i} + y\hat{j} + z\hat{k} = x\hat{i} - \frac{1}{x}\hat{j} + \frac{1}{x}\hat{k}$$. To find a unit vector parallel to this, we can choose a convenient value of $$x$$. Since $$x$$ can be any nonzero real number (the collinearity condition allows any $$x \neq 0$$), let us try $$x = 1$$.
With $$x = 1$$: $$y = -\frac{1}{1} = -1$$ and $$z = \frac{1}{1} = 1$$. We verify collinearity: $$\vec{a_1} = \hat{i} - \hat{j} + \hat{k}$$ and $$\vec{a_2} = \hat{i} - \hat{j} + \hat{k}$$, which are indeed collinear ($$\lambda = 1$$).
The vector $$x\hat{i} + y\hat{j} + z\hat{k} = \hat{i} - \hat{j} + \hat{k}$$, with magnitude $$|\hat{i} - \hat{j} + \hat{k}| = \sqrt{1^2 + (-1)^2 + 1^2} = \sqrt{3}$$.
The unit vector is $$\frac{\hat{i} - \hat{j} + \hat{k}}{\sqrt{3}} = \frac{1}{\sqrt{3}}(\hat{i} - \hat{j} + \hat{k})$$.
In a triangle $$ABC$$, if $$|\overrightarrow{BC}| = 3$$, $$|\overrightarrow{CA}| = 5$$ and $$|\overrightarrow{BA}| = 7$$, then the projection of the vector $$\overrightarrow{BA}$$ on $$\overrightarrow{BC}$$ is equal to:
We are given a triangle $$ABC$$ with $$|\overrightarrow{BC}| = 3$$, $$|\overrightarrow{CA}| = 5$$, and $$|\overrightarrow{BA}| = 7$$. We need to find the projection of $$\overrightarrow{BA}$$ onto $$\overrightarrow{BC}$$.
The projection of $$\overrightarrow{BA}$$ on $$\overrightarrow{BC}$$ is given by $$\frac{\overrightarrow{BA} \cdot \overrightarrow{BC}}{|\overrightarrow{BC}|}$$. To find the dot product, we use the cosine rule at vertex $$B$$.
By the cosine rule applied to side $$CA$$ (opposite to angle $$B$$): $$|CA|^2 = |BA|^2 + |BC|^2 - 2|BA||BC|\cos B$$ $$25 = 49 + 9 - 2(7)(3)\cos B$$ $$25 = 58 - 42\cos B$$ $$\cos B = \frac{33}{42} = \frac{11}{14}$$
The dot product $$\overrightarrow{BA} \cdot \overrightarrow{BC} = |\overrightarrow{BA}||\overrightarrow{BC}|\cos B = 7 \times 3 \times \frac{11}{14} = \frac{231}{14} = \frac{33}{2}$$.
The projection of $$\overrightarrow{BA}$$ on $$\overrightarrow{BC}$$ is: $$\frac{\overrightarrow{BA} \cdot \overrightarrow{BC}}{|\overrightarrow{BC}|} = \frac{33/2}{3} = \frac{33}{6} = \frac{11}{2}$$
Let three vectors $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be such that $$\vec{a} \times \vec{b} = \vec{c}$$, $$\vec{b} \times \vec{c} = \vec{a}$$ and $$|\vec{a}| = 2$$. Then which one of the following is not true?
We are given $$\vec{a} \times \vec{b} = \vec{c}$$, $$\vec{b} \times \vec{c} = \vec{a}$$, and $$|\vec{a}| = 2$$. First, let us establish the magnitudes and mutual orthogonality of the three vectors.
From $$\vec{b} \times \vec{c} = \vec{a}$$, take the cross product with $$\vec{b}$$ from the left: $$\vec{b} \times (\vec{b} \times \vec{c}) = \vec{b} \times \vec{a}$$. Using the BAC-CAB identity on the left: $$(\vec{b} \cdot \vec{c})\vec{b} - |\vec{b}|^2 \vec{c} = -\vec{a} \times \vec{b} = -\vec{c}$$. This gives $$(\vec{b} \cdot \vec{c})\vec{b} = (|\vec{b}|^2 - 1)\vec{c}$$. Since $$\vec{b}$$ and $$\vec{c}$$ are linearly independent (their cross product $$\vec{a} \neq \vec{0}$$), both coefficients must be zero: $$\vec{b} \cdot \vec{c} = 0$$ and $$|\vec{b}|^2 = 1$$, giving $$|\vec{b}| = 1$$.
Since $$\vec{b} \cdot \vec{c} = 0$$, from $$\vec{b} \times \vec{c} = \vec{a}$$ we get $$|\vec{a}| = |\vec{b}||\vec{c}|\sin 90° = |\vec{c}|$$, so $$|\vec{c}| = 2$$. From $$\vec{a} \times \vec{b} = \vec{c}$$, $$|\vec{c}| = |\vec{a}||\vec{b}|\sin\theta_{ab} = 2\sin\theta_{ab} = 2$$, giving $$\sin\theta_{ab} = 1$$, so $$\vec{a} \perp \vec{b}$$. Also, $$\vec{c} = \vec{a} \times \vec{b}$$ is perpendicular to both $$\vec{a}$$ and $$\vec{b}$$. Therefore $$\vec{a}, \vec{b}, \vec{c}$$ are mutually orthogonal with $$|\vec{a}| = |\vec{c}| = 2$$ and $$|\vec{b}| = 1$$.
Now check each option. For Option (A): $$(\vec{b} + \vec{c}) \times (\vec{b} - \vec{c}) = \vec{b} \times \vec{b} - \vec{b} \times \vec{c} + \vec{c} \times \vec{b} - \vec{c} \times \vec{c} = -2(\vec{b} \times \vec{c}) = -2\vec{a}$$. So $$\vec{a} \times (-2\vec{a}) = \vec{0}$$. This is true.
For Option (B): the projection of $$\vec{a}$$ on $$\vec{b} \times \vec{c}$$ is $$\frac{\vec{a} \cdot (\vec{b} \times \vec{c})}{|\vec{b} \times \vec{c}|}$$. Since $$\vec{b} \times \vec{c} = \vec{a}$$, this is $$\frac{|\vec{a}|^2}{|\vec{a}|} = |\vec{a}| = 2$$. This is true.
For Option (C): $$[\vec{a}\;\vec{b}\;\vec{c}] = \vec{a} \cdot (\vec{b} \times \vec{c}) = \vec{a} \cdot \vec{a} = 4$$. The scalar triple product is invariant under cyclic permutation, so $$[\vec{c}\;\vec{a}\;\vec{b}] = 4$$ as well. Their sum is $$4 + 4 = 8$$. This is true.
For Option (D): $$|3\vec{a} + \vec{b} - 2\vec{c}|^2 = 9|\vec{a}|^2 + |\vec{b}|^2 + 4|\vec{c}|^2 + 6(\vec{a} \cdot \vec{b}) - 12(\vec{a} \cdot \vec{c}) - 4(\vec{b} \cdot \vec{c})$$. Since all dot products are zero, this equals $$9(4) + 1 + 4(4) = 36 + 1 + 16 = 53$$. The option claims the value is 51, which is incorrect.
Therefore Option (D) is not true, and the answer is $$|3\vec{a} + \vec{b} - 2\vec{c}|^2 = 53 \neq 51$$.
Let $$\vec{a} = \hat{i} + 2\hat{j} - 3\hat{k}$$ and $$\vec{b} = 2\hat{i} - 3\hat{j} + 5\hat{k}$$. If $$\vec{r} \times \vec{a} = \vec{b} \times \vec{r}$$, $$\vec{r} \cdot (\alpha\hat{i} + 2\hat{j} + \hat{k}) = 3$$ and $$\vec{r} \cdot (2\hat{i} + 5\hat{j} - \alpha\hat{k}) = -1$$, $$\alpha \in R$$, then the value of $$\alpha + |\vec{r}|^2$$ is equal to:
We have $$\vec{a} = \hat{i} + 2\hat{j} - 3\hat{k}$$ and $$\vec{b} = 2\hat{i} - 3\hat{j} + 5\hat{k}$$. The condition $$\vec{r} \times \vec{a} = \vec{b} \times \vec{r}$$ can be rewritten as $$\vec{r} \times \vec{a} + \vec{r} \times \vec{b} = \vec{0}$$, i.e., $$\vec{r} \times (\vec{a} + \vec{b}) = \vec{0}$$.
This means $$\vec{r}$$ is parallel to $$\vec{a} + \vec{b} = 3\hat{i} - \hat{j} + 2\hat{k}$$. So $$\vec{r} = t(3\hat{i} - \hat{j} + 2\hat{k})$$ for some scalar $$t$$.
From the first dot product condition: $$\vec{r} \cdot (\alpha\hat{i} + 2\hat{j} + \hat{k}) = 3$$, so $$t(3\alpha - 2 + 2) = 3$$, giving $$3\alpha t = 3$$, hence $$t = \frac{1}{\alpha}$$.
From the second dot product condition: $$\vec{r} \cdot (2\hat{i} + 5\hat{j} - \alpha\hat{k}) = -1$$, so $$t(6 - 5 - 2\alpha) = -1$$, giving $$t(1 - 2\alpha) = -1$$.
Substituting $$t = \frac{1}{\alpha}$$: $$\frac{1 - 2\alpha}{\alpha} = -1$$, so $$1 - 2\alpha = -\alpha$$, giving $$\alpha = 1$$.
Then $$t = 1$$ and $$\vec{r} = 3\hat{i} - \hat{j} + 2\hat{k}$$, so $$|\vec{r}|^2 = 9 + 1 + 4 = 14$$.
Therefore, $$\alpha + |\vec{r}|^2 = 1 + 14 = 15$$.
In a triangle $$ABC$$, if $$|\overrightarrow{BC}| = 8$$, $$|\overrightarrow{CA}| = 7$$, $$|\overrightarrow{AB}| = 10$$, then the projection of the vector $$\overrightarrow{AB}$$ on $$\overrightarrow{AC}$$ is equal to :
In triangle $$ABC$$, we have $$|\overrightarrow{BC}| = a = 8$$, $$|\overrightarrow{CA}| = b = 7$$, and $$|\overrightarrow{AB}| = c = 10$$. The projection of $$\overrightarrow{AB}$$ on $$\overrightarrow{AC}$$ is $$\frac{\overrightarrow{AB} \cdot \overrightarrow{AC}}{|\overrightarrow{AC}|}$$.
Using the cosine rule, $$\cos A = \frac{b^2 + c^2 - a^2}{2bc} = \frac{49 + 100 - 64}{2 \cdot 7 \cdot 10} = \frac{85}{140} = \frac{17}{28}$$.
Now $$\overrightarrow{AB} \cdot \overrightarrow{AC} = |\overrightarrow{AB}||\overrightarrow{AC}|\cos A = 10 \cdot 7 \cdot \frac{17}{28} = \frac{1190}{28} = \frac{85}{2}$$.
The projection is $$\frac{\overrightarrow{AB} \cdot \overrightarrow{AC}}{|\overrightarrow{AC}|} = \frac{85/2}{7} = \frac{85}{14}$$.
Let $$a, b$$ and $$c$$ be distinct positive numbers. If the vectors $$a\hat{i} + a\hat{j} + c\hat{k}$$, $$\hat{i} + \hat{k}$$ and $$c\hat{i} + c\hat{j} + b\hat{k}$$ are co-planar, then $$c$$ is equal to:
We are told that the three vectors
$$\vec{v_1}=a\hat i+a\hat j+c\hat k,\qquad \vec{v_2}=1\hat i+0\hat j+1\hat k,\qquad \vec{v_3}=c\hat i+c\hat j+b\hat k$$
are co-planar. Three vectors are co-planar precisely when their scalar triple product is zero. The scalar triple product formula is
$$[\vec{v_1}\;\vec{v_2}\;\vec{v_3}]= \begin{vmatrix} v_{1x}&v_{1y}&v_{1z}\\ v_{2x}&v_{2y}&v_{2z}\\ v_{3x}&v_{3y}&v_{3z} \end{vmatrix}=0.$$
Now we substitute the components of our vectors into the determinant:
$$ \begin{vmatrix} a & a & c \\ 1 & 0 & 1 \\ c & c & b \end{vmatrix}=0. $$
We expand this determinant along the first row. First, write the general expansion:
$$\left| \begin{array}{ccc} A_{11}&A_{12}&A_{13}\\ A_{21}&A_{22}&A_{23}\\ A_{31}&A_{32}&A_{33} \end{array}\right| =A_{11}(A_{22}A_{33}-A_{23}A_{32}) -A_{12}(A_{21}A_{33}-A_{23}A_{31}) +A_{13}(A_{21}A_{32}-A_{22}A_{31}).$$
Comparing with our entries, we identify
$$A_{11}=a,\;A_{12}=a,\;A_{13}=c,$$ $$A_{21}=1,\;A_{22}=0,\;A_{23}=1,$$ $$A_{31}=c,\;A_{32}=c,\;A_{33}=b.$$
Substituting, we get
$$ \begin{aligned} [\vec{v_1}\;\vec{v_2}\;\vec{v_3}]&= a\bigl(0\cdot b-1\cdot c\bigr) -a\bigl(1\cdot b-1\cdot c\bigr) +c\bigl(1\cdot c-0\cdot c\bigr)\\[4pt] &=a(0-bc)-a(b-c)+c(c-0)\\[4pt] &=-ac-a(b-c)+c^2\\[4pt] &=-ac-ab+ac+c^2\\[4pt] &=-ab+c^2. \end{aligned} $$
Because the three vectors are co-planar, the scalar triple product is zero, so we set
$$-ab+c^2=0.$$
Rearranging, we obtain
$$c^2=ab.$$
All three of $$a,b,c$$ are positive, and the distinctness condition merely tells us they are not equal; hence we take the positive square root:
$$c=\sqrt{ab}.$$
Hence, the correct answer is Option D.
Let $$O$$ be the origin. Let $$\vec{OP} = x\hat{i} + y\hat{j} - \hat{k}$$ and $$\vec{OQ} = -\hat{i} + 2\hat{j} + 3x\hat{k}$$, $$x, y \in R$$, $$x > 0$$, be such that $$|\vec{PQ}| = \sqrt{20}$$ and the vector $$\vec{OP}$$ is perpendicular to $$\vec{OQ}$$. If $$\vec{OR} = 3\hat{i} + z\hat{j} - 7\hat{k}$$, $$z \in R$$, is coplanar with $$\vec{OP}$$ and $$\vec{OQ}$$, then the value of $$x^2 + y^2 + z^2$$ is equal to:
We have $$\vec{OP} = x\hat{i} + y\hat{j} - \hat{k}$$ and $$\vec{OQ} = -\hat{i} + 2\hat{j} + 3x\hat{k}$$, with $$x > 0$$.
Condition 1: $$\vec{OP} \perp \vec{OQ}$$, so $$\vec{OP} \cdot \vec{OQ} = 0$$. This gives $$x(-1) + y(2) + (-1)(3x) = 0$$, so $$-x + 2y - 3x = 0$$, which simplifies to $$2y = 4x$$, giving $$y = 2x$$ ... (1).
Condition 2: $$|\vec{PQ}| = \sqrt{20}$$. We have $$\vec{PQ} = \vec{OQ} - \vec{OP} = (-1-x)\hat{i} + (2-y)\hat{j} + (3x+1)\hat{k}$$.
$$|\vec{PQ}|^2 = (-1-x)^2 + (2-y)^2 + (3x+1)^2 = 20$$.
Substituting $$y = 2x$$: $$(1+x)^2 + (2-2x)^2 + (3x+1)^2 = 20$$.
Expanding: $$(1 + 2x + x^2) + (4 - 8x + 4x^2) + (9x^2 + 6x + 1) = 20$$.
$$14x^2 + 0x + 6 = 20$$, so $$14x^2 = 14$$, giving $$x^2 = 1$$, so $$x = 1$$ (since $$x > 0$$).
From (1): $$y = 2$$. So $$\vec{OP} = \hat{i} + 2\hat{j} - \hat{k}$$ and $$\vec{OQ} = -\hat{i} + 2\hat{j} + 3\hat{k}$$.
Now $$\vec{OR} = 3\hat{i} + z\hat{j} - 7\hat{k}$$ is coplanar with $$\vec{OP}$$ and $$\vec{OQ}$$. Three vectors are coplanar when their scalar triple product is zero:
$$\begin{vmatrix} 1 & 2 & -1 \\ -1 & 2 & 3 \\ 3 & z & -7 \end{vmatrix} = 0$$.
Expanding along the first row: $$1(2 \cdot (-7) - 3z) - 2((-1)(-7) - 3 \cdot 3) + (-1)((-1)z - 2 \cdot 3) = 0$$.
$$1(-14 - 3z) - 2(7 - 9) + (-1)(-z - 6) = 0$$.
$$-14 - 3z - 2(-2) + z + 6 = 0$$.
$$-14 - 3z + 4 + z + 6 = 0$$, so $$-2z - 4 = 0$$, giving $$z = -2$$.
Therefore $$x^2 + y^2 + z^2 = 1 + 4 + 4 = 9$$.
The answer is $$9$$, which is Option B.
Let the vectors $$(2 + a + b)\hat{i} + (a + 2b+c)\hat{j} - (b + c)\hat{k}$$, $$(1 + b)\hat{i}+2b\hat{j}-b\hat{k}$$ and $$(2 + b)\hat{i} + 2b\hat{j} + (1 - b)\hat{k}$$, $$ a, b, c \in R$$ be co-planar. Then which of the following is true?
Let $$\vec{a} = 2\hat{i} - 3\hat{j} + 4\hat{k}$$ and $$\vec{b} = 7\hat{i} + \hat{j} - 6\hat{k}$$. If $$\vec{r} \times \vec{a} = \vec{r} \times \vec{b}$$, $$\vec{r} \cdot (\hat{i} + 2\hat{j} + \hat{k}) = -3$$, then $$\vec{r} \cdot (2\hat{i} - 3\hat{j} + \hat{k})$$ is equal to:
We are given $$\vec{a} = 2\hat{i} - 3\hat{j} + 4\hat{k}$$ and $$\vec{b} = 7\hat{i} + \hat{j} - 6\hat{k}$$, with the conditions $$\vec{r} \times \vec{a} = \vec{r} \times \vec{b}$$ and $$\vec{r} \cdot (\hat{i} + 2\hat{j} + \hat{k}) = -3$$.
From $$\vec{r} \times \vec{a} = \vec{r} \times \vec{b}$$, we get $$\vec{r} \times (\vec{a} - \vec{b}) = \vec{0}$$.
Now $$\vec{a} - \vec{b} = (2-7)\hat{i} + (-3-1)\hat{j} + (4+6)\hat{k} = -5\hat{i} - 4\hat{j} + 10\hat{k}$$.
Since $$\vec{r} \times (\vec{a} - \vec{b}) = \vec{0}$$, the vector $$\vec{r}$$ is parallel to $$\vec{a} - \vec{b}$$. So $$\vec{r} = \lambda(-5\hat{i} - 4\hat{j} + 10\hat{k})$$ for some scalar $$\lambda$$.
Using $$\vec{r} \cdot (\hat{i} + 2\hat{j} + \hat{k}) = -3$$: $$\lambda(-5 - 8 + 10) = -3$$, so $$-3\lambda = -3$$, giving $$\lambda = 1$$.
Therefore $$\vec{r} = -5\hat{i} - 4\hat{j} + 10\hat{k}$$.
Now $$\vec{r} \cdot (2\hat{i} - 3\hat{j} + \hat{k}) = (-5)(2) + (-4)(-3) + (10)(1) = -10 + 12 + 10 = 12$$.
The answer is Option A: 12.
Let $$\vec{a} = \hat{i} + \hat{j} + 2\hat{k}$$ and $$\vec{b} = -\hat{i} + 2\hat{j} + 3\hat{k}$$. Then the vector product $$\left(\vec{a} + \vec{b}\right) \times \left(\left(\vec{a} \times \left(\left(\vec{a} - \vec{b}\right) \times \vec{b}\right)\right) \times \vec{b}\right)$$ is equal to:
We have the two given vectors
$$\vec a = \hat i + \hat j + 2\hat k, \qquad \vec b = -\hat i + 2\hat j + 3\hat k.$$
The expression to be evaluated is
$$\bigl(\vec a+\vec b\bigr)\;\times\;\Bigl(\bigl(\vec a \times \bigl((\vec a-\vec b)\times \vec b\bigr)\bigr)\times\vec b\Bigr).$$
We shall build it part by part, showing every algebraic step.
1. Calculating $$\vec a+\vec b$$
$$\vec a+\vec b = (1\hat i+1\hat j+2\hat k)+(-1\hat i+2\hat j+3\hat k) = 0\hat i+3\hat j+5\hat k.$$
2. Calculating $$\vec a-\vec b$$
$$\vec a-\vec b = (1\hat i+1\hat j+2\hat k)-(-1\hat i+2\hat j+3\hat k) = 2\hat i-1\hat j-1\hat k.$$
3. Calculating the first cross product $$\bigl(\vec a-\vec b\bigr)\times\vec b$$
Using the determinant form for the cross product,
$$ \bigl(\vec a-\vec b\bigr)\times\vec b =\begin{vmatrix} \hat i & \hat j & \hat k\\ 2 & -1 & -1\\ -1 & 2 & 3 \end{vmatrix} =\hat i\bigl((-1)\cdot3-(-1)\cdot2\bigr) -\hat j\bigl(2\cdot3-(-1)\cdot(-1)\bigr) +\hat k\bigl(2\cdot2-(-1)\cdot(-1)\bigr). $$
This gives
$$ \hat i(-3+2)-\hat j(6-1)+\hat k(4-1) =-1\hat i-5\hat j+3\hat k. $$
4. Calculating the next cross product $$\vec a\times\Bigl((\vec a-\vec b)\times\vec b\Bigr)$$
Now we cross $$\vec a=(1,1,2)$$ with $$(-1,-5,3).$$ Again using the determinant,
$$ \vec a\times\bigl((\vec a-\vec b)\times\vec b\bigr) =\begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & 1 & 2\\ -1 & -5 & 3 \end{vmatrix} =\hat i\bigl(1\cdot3-2\cdot(-5)\bigr) -\hat j\bigl(1\cdot3-2\cdot(-1)\bigr) +\hat k\bigl(1\cdot(-5)-1\cdot(-1)\bigr). $$
Simplifying term by term,
$$ \hat i(3+10)-\hat j(3+2)+\hat k(-5+1) =13\hat i-5\hat j-4\hat k. $$
5. Calculating $$\Bigl(\vec a\times\bigl((\vec a-\vec b)\times\vec b\bigr)\Bigr)\times\vec b$$
We now cross $$\bigl(13,-5,-4\bigr)$$ with $$\vec b=(-1,2,3).$$ Writing the determinant,
$$ \begin{vmatrix} \hat i & \hat j & \hat k\\ 13 & -5 & -4\\ -1 & 2 & 3 \end{vmatrix} =\hat i\bigl((-5)\cdot3-(-4)\cdot2\bigr) -\hat j\bigl(13\cdot3-(-4)\cdot(-1)\bigr) +\hat k\bigl(13\cdot2-(-5)\cdot(-1)\bigr). $$
Evaluating each component,
$$ \hat i(-15+8)-\hat j(39-4)+\hat k(26-5) =-7\hat i-35\hat j+21\hat k. $$
6. Finally, computing $$\bigl(\vec a+\vec b\bigr)\times\Bigl(\dots\Bigr)$$
The last cross product is between $$\vec a+\vec b=(0,3,5)$$ and $$(-7,-35,21).$$ Using the determinant once more,
$$ \begin{vmatrix} \hat i & \hat j & \hat k\\ 0 & 3 & 5\\ -7 & -35 & 21 \end{vmatrix} =\hat i\bigl(3\cdot21-5\cdot(-35)\bigr) -\hat j\bigl(0\cdot21-5\cdot(-7)\bigr) +\hat k\bigl(0\cdot(-35)-3\cdot(-7)\bigr). $$
Simplifying,
$$ \hat i(63+175)-\hat j(0+35)+\hat k(0+21) =238\hat i-35\hat j+21\hat k. $$
7. Recognising a common factor
All three coefficients share the common factor $$7$$:
$$238\hat i-35\hat j+21\hat k =7\bigl(34\hat i-5\hat j+3\hat k\bigr).$$
Thus the required vector product equals
$$7\bigl(34\hat i-5\hat j+3\hat k\bigr).$$
Comparing with the given alternatives, this matches Option B.
Hence, the correct answer is Option 2.
Let $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$ and $$\vec{b} = \hat{j} - \hat{k}$$. If $$\vec{c}$$ is a vector such that $$\vec{a} \times \vec{c} = \vec{b}$$ and $$\vec{a} \cdot \vec{c} = 3$$, then $$\vec{a} \cdot (\vec{b} \times \vec{c})$$ is equal to:
We have the vectors
$$\vec a = \hat i + \hat j + \hat k, \qquad \vec b = \hat j - \hat k.$$
Let us assume
$$\vec c = x\,\hat i + y\,\hat j + z\,\hat k.$$
The first condition is the cross-product relation
$$\vec a \times \vec c = \vec b.$$
For two vectors
$$\vec p = (p_x,\,p_y,\,p_z),\qquad
\vec q = (q_x,\,q_y,\,q_z),$$
the formula for the cross product is
$$\vec p \times \vec q =
\bigl(p_yq_z - p_zq_y\bigr)\hat i
- \bigl(p_xq_z - p_zq_x\bigr)\hat j
+ \bigl(p_xq_y - p_yq_x\bigr)\hat k.$$
Applying this to
$$\vec p = \vec a =(1,1,1),\quad
\vec q = \vec c =(x,y,z),$$
we obtain
$$ \vec a \times \vec c = \bigl(1\cdot z - 1\cdot y\bigr)\hat i - \bigl(1\cdot z - 1\cdot x\bigr)\hat j + \bigl(1\cdot y - 1\cdot x\bigr)\hat k = (z-y)\,\hat i -(z-x)\,\hat j +(y-x)\,\hat k. $$
Since this must equal $$\vec b = 0\,\hat i + 1\,\hat j -1\,\hat k,$$ we equate the components:
$$ \begin{aligned} z-y &= 0, \\ -(z-x) &= 1, \\ y-x &= -1. \end{aligned} $$
From the first equation $$z=y.$$ Substituting $$z=y$$ in the second gives $$-(y-x)=1 \; \Longrightarrow \; y-x=-1.$$ The third equation is exactly the same, so the system is self-consistent.
Thus we can write
$$ y = x-1, \qquad z = x-1. $$
Now use the dot-product condition
$$\vec a \cdot \vec c = 3.$$
For vectors $$\vec p=(p_x,p_y,p_z)$$ and $$\vec q=(q_x,q_y,q_z)$$ the dot product is
$$\vec p \cdot \vec q = p_xq_x + p_yq_y + p_zq_z.$$
Therefore
$$ \vec a \cdot \vec c = 1\cdot x + 1\cdot y + 1\cdot z = x + y + z = x + (x-1) + (x-1) = 3x - 2. $$
Setting this equal to 3, we get
$$3x - 2 = 3 \;\Longrightarrow\; 3x = 5 \;\Longrightarrow\; x = \frac53.$$
Hence
$$ y = x-1 = \frac53 - 1 = \frac23, \qquad z = \frac23. $$
So
$$\vec c = \frac53\,\hat i + \frac23\,\hat j + \frac23\,\hat k.$$
We now find the required scalar triple product $$\vec a \cdot (\vec b \times \vec c).$$ Again using the cross-product formula, first compute $$\vec b \times \vec c.$$
Write the components explicitly: $$\vec b = (0,1,-1), \qquad \vec c = \Bigl(\frac53,\frac23,\frac23\Bigr).$$
Then
$$ \vec b \times \vec c = \Bigl(1\cdot\frac23 - (-1)\cdot\frac23\Bigr)\hat i - \Bigl(0\cdot\frac23 - (-1)\cdot\frac53\Bigr)\hat j + \Bigl(0\cdot\frac23 - 1\cdot\frac53\Bigr)\hat k = \frac43\,\hat i -\frac53\,\hat j -\frac53\,\hat k. $$
Finally take the dot product with $$\vec a = (1,1,1):$$
$$ \vec a \cdot (\vec b \times \vec c) = 1\left(\frac43\right) + 1\left(-\frac53\right) + 1\left(-\frac53\right) = \frac43 - \frac53 - \frac53 = \frac{4 - 5 - 5}{3} = \frac{-6}{3} = -2. $$
So, the value of $$\vec a \cdot (\vec b \times \vec c)$$ is $$-2.$$
Hence, the correct answer is Option B.
Let $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be three vectors such that $$\vec{a} = \vec{b} \times (\vec{b} \times \vec{c})$$. If magnitudes of the vectors $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ are $$\sqrt{2}, 1$$ and 2 respectively and the angle between $$\vec{b}$$ and $$\vec{c}$$ is $$\theta$$ $$(0 < \theta < \frac{\pi}{2})$$, then the value of $$1 + \tan \theta$$ is equal to:
We have the relation $$\vec a=\vec b\times(\vec b\times\vec c)$$.
First we recall the standard vector triple-product identity:
$$\vec p\times(\vec q\times\vec r)=\vec q(\vec p\cdot\vec r)-\vec r(\vec p\cdot\vec q).$$
Applying it with $$\vec p=\vec b,\;\vec q=\vec b,\;\vec r=\vec c$$ we get
$$\vec a=\vec b(\vec b\cdot\vec c)-\vec c(\vec b\cdot\vec b).$$
Now we substitute the given magnitudes. We know $$|\vec b|=1,\;|\vec c|=2,$$ and if the angle between $$\vec b$$ and $$\vec c$$ is $$\theta\;(0<\theta<\tfrac{\pi}{2})$$, then
$$\vec b\cdot\vec c=|\vec b||\vec c|\cos\theta=1\cdot2\cos\theta=2\cos\theta.$$
Also $$\vec b\cdot\vec b=|\vec b|^{2}=1^{2}=1.$$
Substituting these scalar products into the expression for $$\vec a$$ gives
$$\vec a=2\cos\theta\,\vec b-1\cdot\vec c=2\cos\theta\,\vec b-\vec c.$$
Next we compute the magnitude of $$\vec a$$. Let us denote
$$\vec u=2\cos\theta\,\vec b,\qquad\vec v=\vec c,$$
so that $$\vec a=\vec u-\vec v.$$
The square of the magnitude is
$$|\vec a|^{2}=|\vec u-\vec v|^{2}=|\vec u|^{2}+|\vec v|^{2}-2\,\vec u\cdot\vec v.$$
We evaluate each term separately:
$$|\vec u|^{2}=(2\cos\theta)^{2}|\vec b|^{2}=4\cos^{2}\theta\cdot1=4\cos^{2}\theta,$$
$$|\vec v|^{2}=|\vec c|^{2}=2^{2}=4,$$
$$\vec u\cdot\vec v=(2\cos\theta\,\vec b)\cdot\vec c=2\cos\theta(\vec b\cdot\vec c)=2\cos\theta(2\cos\theta)=4\cos^{2}\theta.$$
Putting these into the formula for $$|\vec a|^{2}$$ we obtain
$$|\vec a|^{2}=4\cos^{2}\theta+4-2\cdot4\cos^{2}\theta=4\cos^{2}\theta+4-8\cos^{2}\theta=4-4\cos^{2}\theta.$$
Simplifying we have
$$|\vec a|^{2}=4(1-\cos^{2}\theta)=4\sin^{2}\theta.$$
But the problem states that $$|\vec a|=\sqrt{2},$$ so $$|\vec a|^{2}=2.$$ Therefore
$$4\sin^{2}\theta=2\quad\Longrightarrow\quad\sin^{2}\theta=\frac12.$$
Since $$0<\theta<\tfrac{\pi}{2},$$ the sine and cosine are both positive, giving
$$\sin\theta=\frac1{\sqrt2},\qquad\cos\theta=\frac1{\sqrt2}.$$
Hence
$$\tan\theta=\frac{\sin\theta}{\cos\theta}=1.$$
Finally,
$$1+\tan\theta=1+1=2.$$
Hence, the correct answer is Option B.
Let $$\vec{a}$$, $$\vec{b}$$, $$\vec{c}$$ be three vectors mutually perpendicular to each other and have same magnitude. If a vector $$\vec{r}$$ satisfies $$\vec{a} \times \{\vec{r} - \vec{b} \times \vec{a}\} + \vec{b} \times \{\vec{r} - \vec{c} \times \vec{b}\} + \vec{c} \times \{\vec{r} - \vec{a} \times \vec{c}\} = \vec{0}$$, then $$\vec{r}$$ is equal to:
If $$|\vec{a}| = 2$$, $$|\vec{b}| = 5$$ and $$|\vec{a} \times \vec{b}| = 8$$, then $$|\vec{a} \cdot \vec{b}|$$ is equal to:
We start by recalling the two standard formulas that relate the magnitudes of the dot and cross products of two vectors $$\vec a$$ and $$\vec b$$ with the angle $$\theta$$ between them.
Dot-product magnitude formula: $$|\vec a \cdot \vec b| \;=\; |\vec a|\,|\vec b|\,|\cos\theta|.$$
Cross-product magnitude formula: $$|\vec a \times \vec b| \;=\; |\vec a|\,|\vec b|\,|\sin\theta|.$$
We are given $$|\vec a| = 2,\; |\vec b| = 5,\; |\vec a \times \vec b| = 8.$$ We first use the cross-product formula to determine $$\sin\theta.$$
Substituting the known magnitudes, we have
$$8 \;=\; |\vec a \times \vec b| \;=\; |\vec a|\,|\vec b|\,|\sin\theta|$$
$$8 \;=\; 2 \times 5 \times |\sin\theta|$$
$$8 \;=\; 10\,|\sin\theta|$$
Dividing both sides by 10,
$$|\sin\theta| \;=\; \frac{8}{10} \;=\; 0.8.$$
Now we find $$|\cos\theta|$$ using the fundamental trigonometric identity $$\sin^{2}\theta + \cos^{2}\theta = 1.$$ Hence,
$$|\cos\theta| \;=\; \sqrt{1 - (\sin^{2}\theta)}$$
$$|\cos\theta| \;=\; \sqrt{1 - (0.8)^{2}}$$
$$|\cos\theta| \;=\; \sqrt{1 - 0.64}$$
$$|\cos\theta| \;=\; \sqrt{0.36}$$
$$|\cos\theta| \;=\; 0.6.$$
With $$|\cos\theta|$$ known, we substitute into the dot-product magnitude formula:
$$|\vec a \cdot \vec b| \;=\; |\vec a|\,|\vec b|\,|\cos\theta|$$
$$|\vec a \cdot \vec b| \;=\; 2 \times 5 \times 0.6$$
$$|\vec a \cdot \vec b| \;=\; 10 \times 0.6$$
$$|\vec a \cdot \vec b| \;=\; 6.$$
Hence, the correct answer is Option A.
Let $$\vec{a} = 2\hat{i} + \hat{j} - 2\hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j}$$. If $$\vec{c}$$ is a vector such that $$\vec{a} \cdot \vec{c} = |\vec{c}|$$, $$|\vec{c} - \vec{a}| = 2\sqrt{2}$$ and the angle between $$(\vec{a} \times \vec{b})$$ and $$\vec{c}$$ is $$\frac{\pi}{6}$$, then the value of $$|(\vec{a} \times \vec{b}) \times \vec{c}|$$ is:
We are given $$\vec{a} = 2\hat{i} + \hat{j} - 2\hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j}$$. First, we compute $$\vec{a} \times \vec{b}$$:
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 1 & -2 \\ 1 & 1 & 0 \end{vmatrix} = \hat{i}(0 + 2) - \hat{j}(0 + 2) + \hat{k}(2 - 1) = 2\hat{i} - 2\hat{j} + \hat{k}$$
So $$|\vec{a} \times \vec{b}| = \sqrt{4 + 4 + 1} = 3$$. Also $$|\vec{a}| = \sqrt{4 + 1 + 4} = 3$$.
From the condition $$|\vec{c} - \vec{a}|^2 = (2\sqrt{2})^2 = 8$$, we expand to get $$|\vec{c}|^2 - 2\vec{a} \cdot \vec{c} + |\vec{a}|^2 = 8$$. Using $$\vec{a} \cdot \vec{c} = |\vec{c}|$$ and $$|\vec{a}|^2 = 9$$:
$$|\vec{c}|^2 - 2|\vec{c}| + 9 = 8 \implies |\vec{c}|^2 - 2|\vec{c}| + 1 = 0 \implies (|\vec{c}| - 1)^2 = 0$$
Thus $$|\vec{c}| = 1$$. Now we use the identity $$|(\vec{a} \times \vec{b}) \times \vec{c}| = |\vec{a} \times \vec{b}||\vec{c}|\sin\theta$$, where $$\theta = \frac{\pi}{6}$$ is the angle between $$\vec{a} \times \vec{b}$$ and $$\vec{c}$$:
$$|(\vec{a} \times \vec{b}) \times \vec{c}| = 3 \cdot 1 \cdot \sin\frac{\pi}{6} = 3 \cdot \frac{1}{2} = \frac{3}{2}$$
Let $$\vec{a}$$ and $$\vec{b}$$ be two non-zero vectors perpendicular to each other and $$|\vec{a}| = |\vec{b}|$$, If $$|\vec{a} \times \vec{b}| = |\vec{a}|$$, then the angle between the vectors $$\left(\vec{a} + \vec{b} + (\vec{a} \times \vec{b})\right)$$ and $$\vec{a}$$ is equal to :
We are given that $$\vec{a}$$ and $$\vec{b}$$ are non-zero, perpendicular, and equal in magnitude, so $$\vec{a} \cdot \vec{b} = 0$$ and $$|\vec{a}| = |\vec{b}|$$. Since the vectors are perpendicular, $$|\vec{a} \times \vec{b}| = |\vec{a}||\vec{b}| = |\vec{a}|^2$$. The condition $$|\vec{a} \times \vec{b}| = |\vec{a}|$$ then gives $$|\vec{a}|^2 = |\vec{a}|$$, so $$|\vec{a}| = 1$$ and hence $$|\vec{b}| = 1$$.
Because $$\vec{a} \times \vec{b}$$ is perpendicular to both $$\vec{a}$$ and $$\vec{b}$$, and $$|\vec{a} \times \vec{b}| = 1$$, the three vectors $$\vec{a}$$, $$\vec{b}$$, and $$\vec{a} \times \vec{b}$$ are mutually orthogonal unit vectors. Let $$\vec{v} = \vec{a} + \vec{b} + (\vec{a} \times \vec{b})$$. Then $$|\vec{v}|^2 = |\vec{a}|^2 + |\vec{b}|^2 + |\vec{a} \times \vec{b}|^2 = 1 + 1 + 1 = 3$$, so $$|\vec{v}| = \sqrt{3}$$.
The dot product $$\vec{v} \cdot \vec{a} = |\vec{a}|^2 + 0 + 0 = 1$$. Therefore the angle $$\theta$$ between $$\vec{v}$$ and $$\vec{a}$$ satisfies $$\cos\theta = \dfrac{\vec{v} \cdot \vec{a}}{|\vec{v}||\vec{a}|} = \dfrac{1}{\sqrt{3}}$$, giving $$\theta = \cos^{-1}\!\left(\dfrac{1}{\sqrt{3}}\right)$$.
Let $$\vec{a}$$ and $$\vec{b}$$ be two vectors such that $$|2\vec{a} + 3\vec{b}| = |3\vec{a} + \vec{b}|$$ and the angle between $$\vec{a}$$ and $$\vec{b}$$ is 60°. If $$\frac{1}{8}\vec{a}$$ is a unit vector, then $$|\vec{b}|$$ is equal to:
We are given that the magnitudes of the two vectors
$$\;2\vec a+3\vec b\quad\text{and}\quad 3\vec a+\vec b$$
are equal, that the angle between $$\vec a$$ and $$\vec b$$ is $$60^\circ,$$ and that $$\displaystyle \frac18\vec a$$ is a unit vector. Our task is to find $$|\vec b|.$$
First, from “$$\dfrac18\vec a$$ is a unit vector” we have
$$\Bigl|\dfrac18\vec a\Bigr|=1 \;\;\Longrightarrow\;\; \dfrac1{8}\,|\vec a|=1 \;\;\Longrightarrow\;\; |\vec a|=8.$$ Hence
$$|\vec a|^2 = 8^2 = 64.$$
Next we use the condition
$$|\,2\vec a+3\vec b\,| \;=\; |\,3\vec a+\vec b\,|.$$
Squaring both sides (because both magnitudes are non-negative) and applying the dot-product identity $$|\vec u|^2=\vec u\!\cdot\!\vec u,$$ we get
$$ (2\vec a+3\vec b)\cdot(2\vec a+3\vec b) \;=\; (3\vec a+\vec b)\cdot(3\vec a+\vec b). $$
Now we expand each side completely, remembering that $$\vec a\!\cdot\!\vec b=\vec b\!\cdot\!\vec a.$$ For the left-hand side:
$$ (2\vec a+3\vec b)\cdot(2\vec a+3\vec b) \;=\; (2\vec a)\cdot(2\vec a) \;+\; 2\,(2\vec a)\cdot(3\vec b) \;+\; (3\vec b)\cdot(3\vec b). $$ Evaluating term by term, we obtain
$$ 4|\vec a|^2 \;+\; 12\,\vec a\!\cdot\!\vec b \;+\; 9|\vec b|^2. $$
For the right-hand side:
$$ (3\vec a+\vec b)\cdot(3\vec a+\vec b) \;=\; (3\vec a)\cdot(3\vec a) \;+\; 2\,(3\vec a)\cdot\vec b \;+\; \vec b\cdot\vec b, $$ which evaluates to
$$ 9|\vec a|^2 \;+\; 6\,\vec a\!\cdot\!\vec b \;+\; |\vec b|^2. $$
Because the two magnitudes are equal, the two expansions themselves must be equal. Thus
$$ 4|\vec a|^2 + 12\,\vec a\!\cdot\!\vec b + 9|\vec b|^2 \;=\; 9|\vec a|^2 + 6\,\vec a\!\cdot\!\vec b + |\vec b|^2. $$
We now move every term to one side to set the entire expression to zero:
$$ 4|\vec a|^2 - 9|\vec a|^2 \;+\; 12\,\vec a\!\cdot\!\vec b - 6\,\vec a\!\cdot\!\vec b \;+\; 9|\vec b|^2 - |\vec b|^2 \;=\; 0. $$ Combining like terms gives
$$ -5|\vec a|^2 \;+\; 6\,\vec a\!\cdot\!\vec b \;+\; 8|\vec b|^2 = 0. $$
Next we write the scalar product $$\vec a\!\cdot\!\vec b$$ in terms of the magnitudes and the included angle. The standard formula is
$$ \vec a\!\cdot\!\vec b = |\vec a|\,|\vec b|\,\cos\theta, $$ where $$\theta$$ is the angle between the two vectors. Here $$\theta=60^\circ,$$ so $$\cos60^\circ=\dfrac12.$$ Therefore
$$ \vec a\!\cdot\!\vec b = |\vec a|\,|\vec b|\,\dfrac12 = 8\,|\vec b|\cdot\dfrac12 = 4\,|\vec b|. $$
Let us denote $$|\vec b|=x$$ to simplify writing. Then
$$ \vec a\!\cdot\!\vec b = 4x, \qquad |\vec b|^2 = x^2. $$
Substituting these expressions, together with $$|\vec a|^2=64,$$ into the earlier equation $$-5|\vec a|^2 + 6\,\vec a\!\cdot\!\vec b + 8|\vec b|^2 = 0,$$ we get
$$ -5(64) \;+\; 6(4x) \;+\; 8(x^2) \;=\; 0. $$ Now we evaluate each term:
$$ -320 \;+\; 24x \;+\; 8x^2 = 0. $$
For convenience we multiply the whole equation by $$-1$$ to make the leading coefficient of $$x^2$$ positive:
$$ 320 \;-\; 24x \;-\; 8x^2 = 0. $$
Next we divide every term by $$8$$ to reduce the coefficients:
$$ 40 \;-\; 3x \;-\; x^2 = 0. $$
Re-ordering the terms in the usual descending powers of $$x$$ yields the quadratic equation
$$ x^2 + 3x - 40 = 0. $$
We now solve this quadratic. The quadratic formula states that for $$ax^2+bx+c=0,$$ $$ x = \dfrac{-b \pm \sqrt{b^2-4ac}}{2a}. $$ Here $$a=1,\; b=3,\; c=-40,$$ so
$$ x = \dfrac{-3 \pm \sqrt{\,3^2 - 4(1)(-40)\,}}{2(1)} = \dfrac{-3 \pm \sqrt{9 + 160}}{2} = \dfrac{-3 \pm \sqrt{169}}{2} = \dfrac{-3 \pm 13}{2}. $$
This gives the two solutions
$$ x = \dfrac{-3 + 13}{2} = \dfrac{10}{2} = 5, \qquad x = \dfrac{-3 - 13}{2} = \dfrac{-16}{2} = -8. $$
Because a magnitude can never be negative, we discard $$x=-8$$ and keep
$$ x = 5. $$
Recalling that $$x = |\vec b|,$$ we conclude
$$ |\vec b| = 5. $$
Hence, the correct answer is Option D.
If $$\vec{a} = \alpha\hat{i} + \beta\hat{j} + 3\hat{k}$$, $$\vec{b} = -\beta\hat{i} - \alpha\hat{j} - \hat{k}$$ and $$\vec{c} = \hat{i} - 2\hat{j} - \hat{k}$$ such that $$\vec{a} \cdot \vec{b} = 1$$ and $$\vec{b} \cdot \vec{c} = -3$$, then $$\frac{1}{3}\left((\vec{a} \times \vec{b}) \cdot \vec{c}\right)$$ is equal to ________.
We have $$\vec{a} = \alpha\hat{i} + \beta\hat{j} + 3\hat{k}$$, $$\vec{b} = -\beta\hat{i} - \alpha\hat{j} - \hat{k}$$, $$\vec{c} = \hat{i} - 2\hat{j} - \hat{k}$$, with $$\vec{a} \cdot \vec{b} = 1$$ and $$\vec{b} \cdot \vec{c} = -3$$.
$$\vec{a} \cdot \vec{b} = -\alpha\beta - \alpha\beta - 3 = -2\alpha\beta - 3 = 1$$, so $$\alpha\beta = -2$$ $$-(1)$$.
$$\vec{b} \cdot \vec{c} = -\beta(1) + (-\alpha)(-2) + (-1)(-1) = -\beta + 2\alpha + 1 = -3$$, so $$2\alpha - \beta = -4$$ $$-(2)$$.
From $$(2)$$: $$\beta = 2\alpha + 4$$. Substituting into $$(1)$$: $$\alpha(2\alpha+4) = -2$$, giving $$2\alpha^2 + 4\alpha + 2 = 0$$, i.e., $$(\alpha+1)^2 = 0$$, so $$\alpha = -1$$.
Then $$\beta = 2(-1) + 4 = 2$$. So $$\vec{a} = -\hat{i} + 2\hat{j} + 3\hat{k}$$ and $$\vec{b} = -2\hat{i} + \hat{j} - \hat{k}$$.
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -1 & 2 & 3 \\ -2 & 1 & -1 \end{vmatrix} = \hat{i}(-2-3) - \hat{j}(1+6) + \hat{k}(-1+4) = -5\hat{i} - 7\hat{j} + 3\hat{k}$$.
$$(\vec{a} \times \vec{b}) \cdot \vec{c} = (-5)(1) + (-7)(-2) + (3)(-1) = -5 + 14 - 3 = 6$$.
$$\frac{1}{3}((\vec{a} \times \vec{b}) \cdot \vec{c}) = \frac{6}{3} = 2$$.
The answer is 2.
If $$\vec{a}$$ and $$\vec{b}$$ are unit vectors and $$\left(\vec{a} + 3\vec{b}\right)$$ is perpendicular to $$\left(7\vec{a} - 5\vec{b}\right)$$ and $$\left(\vec{a} - 4\vec{b}\right)$$ is perpendicular to $$\left(7\vec{a} - 2\vec{b}\right)$$, then the angle between $$\vec{a}$$ and $$\vec{b}$$ (in degrees) is _________.
Let us denote the angle between the unit vectors $$\vec a$$ and $$\vec b$$ by $$\theta$$. By definition of the dot product we have
$$\vec a\cdot\vec b \;=\; |\vec a|\,|\vec b|\cos\theta \;=\; 1\cdot1\cdot\cos\theta \;=\; \cos\theta.$$
First we use the fact that $$\bigl(\vec a+3\vec b\bigr)$$ is perpendicular to $$\bigl(7\vec a-5\vec b\bigr)$$. Two vectors are perpendicular exactly when their dot product is zero, so
$$\bigl(\vec a+3\vec b\bigr)\cdot\bigl(7\vec a-5\vec b\bigr)=0.$$
We expand this dot product term by term:
$$\begin{aligned} \bigl(\vec a+3\vec b\bigr)\cdot\bigl(7\vec a-5\vec b\bigr) &= \vec a\cdot(7\vec a) \;+\; \vec a\cdot(-5\vec b)\;+\; 3\vec b\cdot(7\vec a)\;+\; 3\vec b\cdot(-5\vec b)\\[4pt] &= 7\,\vec a\cdot\vec a \;-\; 5\,\vec a\cdot\vec b \;+\; 21\,\vec b\cdot\vec a \;-\; 15\,\vec b\cdot\vec b.\\ \end{aligned}$$
Since $$|\vec a|^2=\vec a\cdot\vec a=1$$ and $$|\vec b|^2=\vec b\cdot\vec b=1$$, and because $$\vec b\cdot\vec a=\vec a\cdot\vec b=\cos\theta,$$ this becomes
$$7(1)\;-\;5(\cos\theta)\;+\;21(\cos\theta)\;-\;15(1)=0.$$
Simplifying we get
$$7-15 \;+\; (-5+21)\cos\theta \;=\; 0 \quad\Longrightarrow\quad -8\;+\;16\cos\theta=0.$$
So
$$16\cos\theta = 8 \quad\Longrightarrow\quad \cos\theta = \frac{8}{16} = \frac12.$$
Now we use the second given perpendicularity: $$\bigl(\vec a-4\vec b\bigr)$$ is perpendicular to $$\bigl(7\vec a-2\vec b\bigr)$$, giving
$$\bigl(\vec a-4\vec b\bigr)\cdot\bigl(7\vec a-2\vec b\bigr)=0.$$
Again we expand fully:
$$\begin{aligned} \bigl(\vec a-4\vec b\bigr)\cdot\bigl(7\vec a-2\vec b\bigr) &= \vec a\cdot(7\vec a)\;+\;\vec a\cdot(-2\vec b)\;-\;4\vec b\cdot(7\vec a)\;-\;4\vec b\cdot(-2\vec b)\\[4pt] &= 7\,\vec a\cdot\vec a \;-\; 2\,\vec a\cdot\vec b \;-\; 28\,\vec b\cdot\vec a \;+\; 8\,\vec b\cdot\vec b.\\ \end{aligned}$$
Substituting $$\vec a\cdot\vec a=1$$, $$\vec b\cdot\vec b=1$$ and $$\vec a\cdot\vec b=\cos\theta$$ gives
$$7(1)\;-\;2(\cos\theta)\;-\;28(\cos\theta)\;+\;8(1)=0.$$
Combining like terms:
$$15 \;-\;30\cos\theta = 0 \quad\Longrightarrow\quad 30\cos\theta = 15 \quad\Longrightarrow\quad \cos\theta = \frac12.$$
Both independent conditions agree on $$\cos\theta=\frac12$$. For $$0^\circ\le\theta\le 180^\circ,$$ the value $$\cos\theta=\frac12$$ corresponds to
$$\theta = 60^\circ.$$
So, the answer is $$60^\circ$$.
Let $$\vec{a}, \vec{b}, \vec{c}$$ be three mutually perpendicular vectors of the same magnitude and equally inclined at an angle $$\theta$$, with the vector $$\vec{a} + \vec{b} + \vec{c}$$. Then $$36\cos^2 2\theta$$ is equal to ___.
Let $$|\vec{a}| = |\vec{b}| = |\vec{c}| = k$$. Since $$\vec{a}, \vec{b}, \vec{c}$$ are mutually perpendicular, all dot products between distinct vectors are zero. Let $$\vec{s} = \vec{a} + \vec{b} + \vec{c}$$. Then:
$$|\vec{s}|^2 = |\vec{a}|^2 + |\vec{b}|^2 + |\vec{c}|^2 = 3k^2 \implies |\vec{s}| = k\sqrt{3}$$
The angle $$\theta$$ that $$\vec{a}$$ makes with $$\vec{s}$$ satisfies:
$$\cos\theta = \frac{\vec{a} \cdot \vec{s}}{|\vec{a}||\vec{s}|} = \frac{\vec{a}\cdot(\vec{a}+\vec{b}+\vec{c})}{k \cdot k\sqrt{3}} = \frac{k^2}{k^2\sqrt{3}} = \frac{1}{\sqrt{3}}$$
By symmetry, $$\vec{b}$$ and $$\vec{c}$$ make the same angle with $$\vec{s}$$, confirming they are equally inclined. Now:
$$\cos 2\theta = 2\cos^2\theta - 1 = \frac{2}{3} - 1 = -\frac{1}{3}$$
$$36\cos^2 2\theta = 36 \cdot \frac{1}{9} = 4$$
If the projection of the vector $$\hat{i} + 2\hat{j} + \hat{k}$$ on the sum of the two vectors $$2\hat{i} + 4\hat{j} - 5\hat{k}$$ and $$-\lambda\hat{i} + 2\hat{j} + 3\hat{k}$$ is 1, then $$\lambda$$ is equal to _________
First, we identify all the vectors involved. The vector whose projection we are talking about is $$\vec{A}=\,\hat{i}+2\hat{j}+\hat{k}.$$ The two vectors that must be added are $$\vec{B}=\,2\hat{i}+4\hat{j}-5\hat{k}$$ and $$\vec{C}= -\lambda\hat{i}+2\hat{j}+3\hat{k}.$$
We form their sum: $$\vec{D}= \vec{B}+\vec{C} =\bigl(2-\lambda\bigr)\hat{i} +\bigl(4+2\bigr)\hat{j} +\bigl(-5+3\bigr)\hat{k} =(2-\lambda)\hat{i}+6\hat{j}-2\hat{k}.$$
The question tells us that the scalar projection (sometimes called the component) of $$\vec{A}$$ on $$\vec{D}$$ equals $$1$$. We state the standard formula: For any two vectors $$\vec{u}$$ and $$\vec{v}$$, the scalar projection of $$\vec{u}$$ on $$\vec{v}$$ is $$\text{proj}_{\vec{v}}\vec{u}= \dfrac{\vec{u}\cdot\vec{v}}{|\vec{v}|}\,.$$
Applying this formula, we must have $$\dfrac{\vec{A}\cdot\vec{D}}{|\vec{D}|}=1.$$
Now we compute the dot product in the numerator. Writing both vectors in component form, $$\vec{A}=(1,\,2,\,1),\qquad \vec{D}=(2-\lambda,\,6,\,-2).$$ Hence $$\vec{A}\cdot\vec{D}=1\,(2-\lambda)+2\,(6)+1\,(-2) =(2-\lambda)+12-2 =12-\lambda.$$
Next we need the magnitude of $$\vec{D}$$. Using the formula $$|\vec{v}|=\sqrt{v_x^2+v_y^2+v_z^2},$$ we have $$|\vec{D}|=\sqrt{(2-\lambda)^2+6^2+(-2)^2} =\sqrt{(2-\lambda)^2+36+4} =\sqrt{(2-\lambda)^2+40}.$$ Therefore the projection condition becomes $$\dfrac{12-\lambda}{\sqrt{(2-\lambda)^2+40}}=1.$$
We clear the square root by squaring both sides: $$(12-\lambda)^2=(2-\lambda)^2+40.$$
Now we expand each square completely. On the left, $$(12-\lambda)^2=\lambda^2-24\lambda+144.$$ On the right, $$(2-\lambda)^2+40=(\lambda-2)^2+40 =\bigl(\lambda^2-4\lambda+4\bigr)+40 =\lambda^2-4\lambda+44.$$
Equating the two expressions and cancelling the identical $$\lambda^2$$ terms on both sides, we get $$\lambda^2-24\lambda+144=\lambda^2-4\lambda+44 \;\Longrightarrow\; -24\lambda+144=-4\lambda+44.$$
Bringing all terms to one side, $$-24\lambda+144+4\lambda-44=0 \;\Longrightarrow\; -20\lambda+100=0.$$
Dividing by $$-20$$, we find $$\lambda = 5.$$
So, the answer is $$5$$.
Let three vectors $$\vec{a}$$, $$\vec{b}$$ and $$\vec{c}$$ be such that $$\vec{c}$$ is coplanar with $$\vec{a}$$ and $$\vec{b}$$, $$\vec{a} \cdot \vec{c} = 7$$ and $$\vec{b}$$ is perpendicular to $$\vec{c}$$, where $$\vec{a} = -\hat{i} + \hat{j} + \hat{k}$$ and $$\vec{b} = 2\hat{i} + \hat{k}$$, then the value of $$|2\vec{a} + \vec{b} + \vec{c}|^2$$ is ______
Let $$\vec{a} = 2\hat{i} - \hat{j} + 2\hat{k}$$ and $$\vec{b} = \hat{i} + 2\hat{j} - \hat{k}$$. Let a vector $$\vec{v}$$ be in the plane containing $$\vec{a}$$ and $$\vec{b}$$. If $$\vec{v}$$ is perpendicular to the vector $$3\hat{i} + 2\hat{j} - \hat{k}$$ and its projection on $$\vec{a}$$ is 19 units, then $$|2\vec{v}|^2$$ is equal to _________.
We have the two fixed vectors $$\vec a=2\hat i-\hat j+2\hat k$$ and $$\vec b=\hat i+2\hat j-\hat k$$. Because the required vector $$\vec v$$ lies in the plane containing $$\vec a$$ and $$\vec b$$, every such vector can be written as a linear combination of these two. So we introduce real numbers $$p$$ and $$q$$ and write
$$\vec v=p\,\vec a+q\,\vec b.$$
The statement “$$\vec v$$ is perpendicular to $$3\hat i+2\hat j-\hat k$$” means that the dot-product of these two vectors is zero. Using the bilinearity of the dot product we have
$$\vec v\cdot\left(3\hat i+2\hat j-\hat k\right)=\left(p\vec a+q\vec b\right)\cdot\left(3\hat i+2\hat j-\hat k\right) = p\bigl(\vec a\cdot(3\hat i+2\hat j-\hat k)\bigr)+q\bigl(\vec b\cdot(3\hat i+2\hat j-\hat k)\bigr)=0.$$
Let us evaluate each scalar product appearing above. First,
$$\vec a\cdot(3\hat i+2\hat j-\hat k)=2\cdot3+(-1)\cdot2+2\cdot(-1)=6-2-2=2,$$
and secondly,
$$\vec b\cdot(3\hat i+2\hat j-\hat k)=1\cdot3+2\cdot2+(-1)\cdot(-1)=3+4+1=8.$$
Substituting these values we get
$$2p+8q=0,$$
which simplifies to
$$p+4q=0\quad\Longrightarrow\quad p=-4q.$$
The next piece of information is that the projection of $$\vec v$$ on $$\vec a$$ has magnitude $$19$$. The length of the projection of a vector $$\vec u$$ on another vector $$\vec w$$ is given by the formula
$$\text{projection length}=\frac{|\vec u\cdot\vec w|}{|\vec w|}.$$
Here $$\vec u=\vec v$$ and $$\vec w=\vec a$$, so we require
$$\frac{|\vec v\cdot\vec a|}{|\vec a|}=19.$$
First we compute $$|\vec a|$$:
$$|\vec a|=\sqrt{2^{2}+(-1)^{2}+2^{2}}=\sqrt{4+1+4}=3.$$
Therefore the above condition becomes
$$|\vec v\cdot\vec a|=19\cdot3=57.$$
Now we evaluate $$\vec v\cdot\vec a$$ using $$\vec v=p\vec a+q\vec b$$:
$$\vec v\cdot\vec a=(p\vec a+q\vec b)\cdot\vec a=p(\vec a\cdot\vec a)+q(\vec b\cdot\vec a).$$
We already know $$\vec a\cdot\vec a=|\vec a|^{2}=9.$$ Next, calculate $$\vec b\cdot\vec a$$:
$$\vec b\cdot\vec a=2\cdot1+(-1)\cdot2+2\cdot(-1)=2-2-2=-2.$$
Hence
$$\vec v\cdot\vec a=9p-2q.$$
We therefore require
$$|9p-2q|=57.$$
But we already have the relation $$p=-4q$$ from the perpendicularity condition. Substituting $$p=-4q$$ gives
$$|9(-4q)-2q|=| -36q-2q |=|-38q|=38|q|=57.$$
Thus
$$|q|=\frac{57}{38}=\frac{3}{2}.$$
To proceed it is enough to take $$q=\pm\frac{3}{2}$$; whichever sign we choose, the square of the final magnitude will be the same. Correspondingly,
$$p=-4q=\mp6.$$
Now, to find $$|\vec v|^{2}$$ we use the expression
$$|\vec v|^{2}=(p\vec a+q\vec b)\cdot(p\vec a+q\vec b) = p^{2}(\vec a\cdot\vec a)+q^{2}(\vec b\cdot\vec b)+2pq(\vec a\cdot\vec b).$$
We already have $$\vec a\cdot\vec a=9$$ and $$\vec a\cdot\vec b=-2.$$ Next we compute $$\vec b\cdot\vec b$$:
$$\vec b\cdot\vec b=1^{2}+2^{2}+(-1)^{2}=1+4+1=6.$$
Substituting all these scalar products, we get
$$|\vec v|^{2}=9p^{2}+6q^{2}+2pq(-2)=9p^{2}+6q^{2}-4pq.$$
Using $$p=-4q$$, we substitute term by term:
$$p^{2}=16q^{2},\qquad pq=-4q^{2}.$$
Hence
$$|\vec v|^{2}=9(16q^{2})+6q^{2}-4(-4q^{2}) =144q^{2}+6q^{2}+16q^{2} =166q^{2}.$$
Now put $$q^{2}=\left(\frac{3}{2}\right)^{2}=\frac{9}{4},$$ obtaining
$$|\vec v|^{2}=166\cdot\frac{9}{4}=\frac{1494}{4}.$$
The question finally asks for $$|2\vec v|^{2}$$. Because multiplying a vector by the scalar $$2$$ multiplies its magnitude by $$2$$, we have
$$|2\vec v|^{2}=4|\vec v|^{2}=4\cdot\frac{1494}{4}=1494.$$
Hence, the correct answer is Option A.
Let $$\vec{a} = \hat{i} + \alpha\hat{j} + 3\hat{k}$$ and $$\vec{b} = 3\hat{i} - \alpha\hat{j} + \hat{k}$$. If the area of the parallelogram whose adjacent sides are represented by the vectors $$\vec{a}$$ and $$\vec{b}$$ is $$8\sqrt{3}$$ square units, then $$\vec{a} \cdot \vec{b}$$ is equal to ______.
We have $$\vec{a} = \hat{i} + \alpha\hat{j} + 3\hat{k}$$ and $$\vec{b} = 3\hat{i} - \alpha\hat{j} + \hat{k}$$. The area of the parallelogram is $$|\vec{a} \times \vec{b}| = 8\sqrt{3}$$.
Computing the cross product: $$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & \alpha & 3 \\ 3 & -\alpha & 1 \end{vmatrix} = \hat{i}(\alpha \cdot 1 - 3 \cdot (-\alpha)) - \hat{j}(1 \cdot 1 - 3 \cdot 3) + \hat{k}(1 \cdot (-\alpha) - \alpha \cdot 3) = (4\alpha)\hat{i} + 8\hat{j} + (-4\alpha)\hat{k}$$.
The magnitude is $$|\vec{a} \times \vec{b}| = \sqrt{16\alpha^2 + 64 + 16\alpha^2} = \sqrt{32\alpha^2 + 64}$$.
Setting this equal to $$8\sqrt{3}$$: $$32\alpha^2 + 64 = 192$$, so $$32\alpha^2 = 128$$, giving $$\alpha^2 = 4$$.
Now, $$\vec{a} \cdot \vec{b} = (1)(3) + (\alpha)(-\alpha) + (3)(1) = 3 - \alpha^2 + 3 = 6 - \alpha^2 = 6 - 4 = 2$$.
Therefore, $$\vec{a} \cdot \vec{b} = 2$$.
Let $$\vec{a} = \hat{i} - \alpha\hat{j} + \beta\hat{k}$$, $$\vec{b} = 3\hat{i} + \beta\hat{j} - \alpha\hat{k}$$ and $$\vec{c} = -\alpha\hat{i} - 2\hat{j} + \hat{k}$$, where $$\alpha$$ and $$\beta$$ are integers. If $$\vec{a} \cdot \vec{b} = -1$$ and $$\vec{b} \cdot \vec{c} = 10$$, then $$(\vec{a} \times \vec{b}) \cdot \vec{c}$$ is equal to _________.
We have the three vectors
$$\vec a = \hat i - \alpha\,\hat j + \beta\,\hat k,\qquad \vec b = 3\hat i + \beta\,\hat j - \alpha\,\hat k,\qquad \vec c = -\alpha\,\hat i - 2\hat j + \hat k.$$
The first condition is given as $$\vec a\cdot\vec b = -1.$$
Using the dot-product formula $$\vec p\cdot\vec q = p_xq_x + p_yq_y + p_zq_z,$$ we write
$$\vec a\cdot\vec b = \bigl(1\bigr)(3) + \bigl(-\alpha\bigr)(\beta) + \bigl(\beta\bigr)(-\alpha) = 3 - \alpha\beta - \alpha\beta = 3 - 2\alpha\beta.$$
Equating this to $$-1$$ gives
$$3 - 2\alpha\beta = -1 \;\Longrightarrow\; 2\alpha\beta = 4 \;\Longrightarrow\; \alpha\beta = 2. \quad -(1)$$
The second condition is $$\vec b\cdot\vec c = 10.$$
Again applying the dot-product formula,
$$\vec b\cdot\vec c = (3)(-\alpha) + (\beta)(-2) + (-\alpha)(1) = -3\alpha - 2\beta - \alpha = -4\alpha - 2\beta.$$
Setting this equal to 10 we obtain
$$-4\alpha - 2\beta = 10 \;\Longrightarrow\; 2\alpha + \beta = -5. \quad -(2)$$
We now have to solve the simultaneous integer equations (1) and (2):
$$\alpha\beta = 2$$, $$\qquad 2\alpha + \beta = -5.$$
Because the product $$\alpha\beta=2$$, the integer possibilities for $$(\alpha,\beta)$$ are $$(1,2),(2,1),(-1,-2),(-2,-1).$$
Substituting each pair into $$2\alpha+\beta$$:
For $$(1,2):\;2(1)+2 = 4\neq -5,$$
For $$(2,1):\;2(2)+1 = 5\neq -5,$$
For $$(-1,-2):\;2(-1)+(-2) = -4\neq -5,$$
For $$(-2,-1):\;2(-2)+(-1) = -5.$$
Only $$\alpha=-2,\;\beta=-1$$ satisfies both equations, so these are the required values.
Next we must find $$(\vec a\times\vec b)\cdot\vec c.$$ The scalar triple product formula is
$$ (\vec a\times\vec b)\cdot\vec c = \begin{vmatrix} a_x & a_y & a_z\\ b_x & b_y & b_z\\ c_x & c_y & c_z \end{vmatrix},$$
that is, the determinant whose rows are the components of $$\vec a,\vec b,\vec c.$$
With $$\alpha=-2,\;\beta=-1$$ the components become
$$\vec a = \langle 1$$, $$\; -\alpha$$, $$\; \beta\rangle = \langle 1$$, $$\;2$$, $$\;-1\rangle$$
$$\vec b = \langle 3$$, $$\; \beta$$, $$\; -\alpha\rangle = \langle 3$$, $$\;-1$$, $$\;2\rangle$$
$$\vec c = \langle -\alpha$$, $$\; -2$$, $$\; 1\rangle = \langle 2$$, $$\;-2$$, $$\;1\rangle.$$
Thus
$$ (\vec a\times\vec b)\cdot\vec c = \begin{vmatrix} 1 & 2 & -1\\ 3 & -1 & 2\\ 2 & -2 & 1 \end{vmatrix}. $$
Expanding along the first row:
$$\begin{aligned} &= 1\;\begin{vmatrix}-1 & 2\\ -2 & 1\end{vmatrix} \;-\;2\;\begin{vmatrix}3 & 2\\ 2 & 1\end{vmatrix} \;+\;(-1)\;\begin{vmatrix}3 & -1\\ 2 & -2\end{vmatrix}\\[4pt] &= 1\,[(-1)(1) - (2)(-2)] \;-\;2\,[3(1) - 2(2)] \;-\;1\,[3(-2) - (-1)(2)]\\[4pt] &= 1\,[-1 + 4] \;-\;2\,[3 - 4] \;-\;1\,[-6 + 2]\\[4pt] &= 1\,(3) \;-\;2\,(-1) \;-\;1\,(-4)\\[4pt] &= 3 + 2 + 4\\[4pt] &= 9. \end{aligned}$$
Therefore, $$(\vec a \times \vec b)\cdot \vec c = 9.$$
So, the answer is $$9$$.
Let $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{b}$$ and $$\vec{c} = \hat{j} - \hat{k}$$ be three vectors such that $$\vec{a} \times \vec{b} = \vec{c}$$ and $$\vec{a} \cdot \vec{b} = 1$$. If the length of projection vector of the vector $$\vec{b}$$ on the vector $$\vec{a} \times \vec{c}$$ is $$l$$, then the value of $$3l^2$$ is equal to _________.
We have the given vectors
$$\vec a = \hat i + \hat j + \hat k, \qquad \vec c = \hat j - \hat k, \qquad \vec b = x\hat i + y\hat j + z\hat k.$$
The first condition is the cross-product relation
$$\vec a \times \vec b = \vec c.$$
Using the determinant formula for a cross product,
$$\vec a \times \vec b \;=\; \begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & 1 & 1\\ x & y & z \end{vmatrix} \;=\; \hat i(1\cdot z-1\cdot y)\;-\;\hat j(1\cdot z-1\cdot x)\;+\;\hat k(1\cdot y-1\cdot x).$$
Simplifying each component we get
$$\vec a \times \vec b = (\,z-y\,)\hat i - (\,z-x\,)\hat j + (\,y-x\,)\hat k.$$
Because this must equal $$\vec c = 0\hat i + 1\hat j -1\hat k,$$ we equate the corresponding components:
$$z-y = 0,\qquad -(z-x)=1,\qquad y-x=-1.$$
From the first equation we have $$z=y.$$ Substituting $$z=y$$ into the other two equations gives
$$x-z = 1 \quad\text{and}\quad y-x = -1.$$
Since $$z=y$$, the first becomes $$x-y=1$$; the second is already $$y-x=-1$$, so both are identical, confirming consistency. Hence
$$x-y = 1 \;\Longrightarrow\; x = y+1.$$
Letting $$y=t$$ (a parameter), we now have
$$x = t+1, \qquad y = t, \qquad z = t,$$
so that
$$\vec b = (t+1)\hat i + t\hat j + t\hat k.$$
The second given condition is the dot-product relation
$$\vec a \cdot \vec b = 1.$$
Using the formula $$\vec a \cdot \vec b = a_x b_x + a_y b_y + a_z b_z$$, we obtain
$$1(t+1) + 1(t) + 1(t) \;=\; 1.$$
That is
$$(t+1) + t + t \;=\; 1 \;\Longrightarrow\; 3t + 1 = 1 \;\Longrightarrow\; 3t = 0 \;\Longrightarrow\; t = 0.$$
Putting $$t=0$$ back into $$\vec b$$ gives
$$\vec b = 1\hat i + 0\hat j + 0\hat k = \hat i.$$
Next, we need the vector $$\vec a \times \vec c$$. Again applying the cross-product determinant,
$$\vec a \times \vec c = \begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & 1 & 1\\ 0 & 1 & -1 \end{vmatrix} = \hat i(1\cdot(-1)-1\cdot1)\;-\;\hat j(1\cdot(-1)-1\cdot0)\;+\;\hat k(1\cdot1-1\cdot0).$$
This simplifies to
$$\vec a \times \vec c = (-2)\hat i + 1\hat j + 1\hat k.$$
We now wish to find the projection of $$\vec b$$ onto $$\vec a \times \vec c$$. The projection vector formula is
$$\text{proj}_{\vec v}\vec u \;=\; \frac{\vec u\cdot\vec v}{\vec v\cdot\vec v}\,\vec v.$$
Here $$\vec u=\vec b$$ and $$\vec v=\vec a \times \vec c$$. First, compute the needed dot products.
$$\vec b \cdot (\vec a \times \vec c) = (1,0,0)\cdot(-2,1,1) = 1\cdot(-2)+0\cdot1+0\cdot1 = -2.$$
Next, compute the squared magnitude of $$\vec a \times \vec c$$:
$$|\vec a \times \vec c|^2 = (-2)^2 + 1^2 + 1^2 = 4 + 1 + 1 = 6.$$
Therefore the projection vector is
$$\vec p = \frac{-2}{6}\,(\,-2,\,1,\,1) = -\frac13(\,-2,\,1,\,1) = \left(\frac23,\,-\frac13,\,-\frac13\right).$$
Its length $$l$$ is obtained from
$$l^2 = \left(\frac23\right)^2 + \left(-\frac13\right)^2 + \left(-\frac13\right)^2 = \frac49 + \frac19 + \frac19 = \frac69 = \frac23.$$
Hence
$$l^2 = \frac23 \quad\Longrightarrow\quad 3l^2 = 3\left(\frac23\right) = 2.$$
So, the answer is $$2$$.
Let $$\vec{c}$$ be a vector perpendicular to the vectors $$\vec{a} = \hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = \hat{i} + 2\hat{j} + \hat{k}$$. If $$\vec{c} \cdot (\hat{i} + \hat{j} + 3\hat{k}) = 8$$, then the value of $$\vec{c} \cdot (\vec{a} \times \vec{b})$$ is equal to ________.
We need $$\vec{c}$$ perpendicular to both $$\vec{a} = \hat{i} + \hat{j} - \hat{k}$$ and $$\vec{b} = \hat{i} + 2\hat{j} + \hat{k}$$. So $$\vec{c}$$ is parallel to $$\vec{a} \times \vec{b}$$.
Computing $$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 1 & -1 \\ 1 & 2 & 1 \end{vmatrix} = \hat{i}(1+2) - \hat{j}(1+1) + \hat{k}(2-1) = 3\hat{i} - 2\hat{j} + \hat{k}$$.
So $$\vec{c} = \lambda(3\hat{i} - 2\hat{j} + \hat{k})$$ for some scalar $$\lambda$$.
Using $$\vec{c} \cdot (\hat{i} + \hat{j} + 3\hat{k}) = 8$$: $$\lambda(3 - 2 + 3) = 8$$, so $$4\lambda = 8$$, giving $$\lambda = 2$$.
Therefore $$\vec{c} = 6\hat{i} - 4\hat{j} + 2\hat{k}$$.
Now $$\vec{c} \cdot (\vec{a} \times \vec{b}) = (6\hat{i} - 4\hat{j} + 2\hat{k}) \cdot (3\hat{i} - 2\hat{j} + \hat{k}) = 18 + 8 + 2 = 28$$.
The answer is $$28$$.
Let $$\vec{x}$$ be a vector in the plane containing vectors $$\vec{a} = 2\hat{i} - \hat{j} + \hat{k}$$ and $$\vec{b} = \hat{i} + 2\hat{j} - \hat{k}$$. If the vector $$\vec{x}$$ is perpendicular to $$(3\hat{i} + 2\hat{j} - \hat{k})$$ and its projection on $$\vec{a}$$ is $$\frac{17\sqrt{6}}{2}$$, then the value of $$|\vec{x}|^2$$ is equal to ________.
The vector $$\vec{x}$$ lies in the plane of $$\vec{a} = 2\hat{i} - \hat{j} + \hat{k}$$ and $$\vec{b} = \hat{i} + 2\hat{j} - \hat{k}$$, so we can write $$\vec{x} = \lambda\vec{a} + \mu\vec{b} = (2\lambda + \mu)\hat{i} + (-\lambda + 2\mu)\hat{j} + (\lambda - \mu)\hat{k}$$.
Since $$\vec{x}$$ is perpendicular to $$\vec{c} = 3\hat{i} + 2\hat{j} - \hat{k}$$, we have $$\vec{x} \cdot \vec{c} = 0$$: $$3(2\lambda + \mu) + 2(-\lambda + 2\mu) - (\lambda - \mu) = 0$$, giving $$6\lambda + 3\mu - 2\lambda + 4\mu - \lambda + \mu = 0$$, so $$3\lambda + 8\mu = 0$$, hence $$\lambda = -\frac{8\mu}{3}$$.
The projection of $$\vec{x}$$ on $$\vec{a}$$ is $$\frac{\vec{x} \cdot \vec{a}}{|\vec{a}|} = \frac{17\sqrt{6}}{2}$$. We compute $$|\vec{a}| = \sqrt{4+1+1} = \sqrt{6}$$.
So $$\vec{x} \cdot \vec{a} = \frac{17\sqrt{6}}{2} \cdot \sqrt{6} = \frac{17 \cdot 6}{2} = 51$$.
Now $$\vec{x} \cdot \vec{a} = \lambda|\vec{a}|^2 + \mu(\vec{a} \cdot \vec{b})$$. We compute $$\vec{a} \cdot \vec{b} = 2 - 2 - 1 = -1$$ and $$|\vec{a}|^2 = 6$$. So $$6\lambda - \mu = 51$$.
Substituting $$\lambda = -\frac{8\mu}{3}$$: $$6 \cdot (-\frac{8\mu}{3}) - \mu = 51$$, giving $$-16\mu - \mu = 51$$, so $$-17\mu = 51$$, hence $$\mu = -3$$.
Then $$\lambda = -\frac{8(-3)}{3} = 8$$. So $$\vec{x} = (16 - 3)\hat{i} + (-8 - 6)\hat{j} + (8 + 3)\hat{k} = 13\hat{i} - 14\hat{j} + 11\hat{k}$$.
Therefore $$|\vec{x}|^2 = 169 + 196 + 121 = 486$$.
For $$p > 0$$, a vector $$\vec{v_2} = 2\hat{i} + (p+1)\hat{j}$$ is obtained by rotating the vector $$\vec{v_1} = \sqrt{3}p\hat{i} + \hat{j}$$ by an angle $$\theta$$ about origin in counter clockwise direction. If $$\tan\theta = \frac{(\alpha\sqrt{3}-2)}{(4\sqrt{3}+3)}$$, then the value of $$\alpha$$ is equal to ___.
We have $$\vec{v_1} = \sqrt{3}p\hat{i} + \hat{j}$$ and $$\vec{v_2} = 2\hat{i} + (p+1)\hat{j}$$. Since $$\vec{v_2}$$ is obtained by rotating $$\vec{v_1}$$, their magnitudes must be equal: $$|\vec{v_1}|^2 = 3p^2 + 1 = |\vec{v_2}|^2 = 4 + (p+1)^2 = 4 + p^2 + 2p + 1 = p^2 + 2p + 5$$
$$3p^2 + 1 = p^2 + 2p + 5 \implies 2p^2 - 2p - 4 = 0 \implies p^2 - p - 2 = 0 \implies (p-2)(p+1) = 0$$
Since $$p > 0$$, we have $$p = 2$$. So $$\vec{v_1} = 2\sqrt{3}\hat{i} + \hat{j}$$ and $$\vec{v_2} = 2\hat{i} + 3\hat{j}$$.
The angle $$\theta$$ from $$\vec{v_1}$$ to $$\vec{v_2}$$ (counterclockwise) satisfies: $$\tan\theta = \tan(\phi_2 - \phi_1)$$ where $$\phi_1 = \arg(\vec{v_1})$$ and $$\phi_2 = \arg(\vec{v_2})$$.
Using the cross product and dot product: $$\sin\theta = \frac{v_{1x} v_{2y} - v_{1y} v_{2x}}{|\vec{v_1}||\vec{v_2}|} = \frac{2\sqrt{3} \cdot 3 - 1 \cdot 2}{|\vec{v_1}||\vec{v_2}|} = \frac{6\sqrt{3} - 2}{|\vec{v_1}||\vec{v_2}|}$$
$$\cos\theta = \frac{\vec{v_1}\cdot\vec{v_2}}{|\vec{v_1}||\vec{v_2}|} = \frac{2\sqrt{3}\cdot 2 + 1\cdot 3}{|\vec{v_1}||\vec{v_2}|} = \frac{4\sqrt{3}+3}{|\vec{v_1}||\vec{v_2}|}$$
Therefore: $$\tan\theta = \frac{\sin\theta}{\cos\theta} = \frac{6\sqrt{3}-2}{4\sqrt{3}+3}$$
Comparing with $$\tan\theta = \frac{\alpha\sqrt{3}-2}{4\sqrt{3}+3}$$, we get $$\alpha\sqrt{3} = 6\sqrt{3}$$, so $$\alpha = 6$$.
Let $$\vec{a} = \hat{i} + 2\hat{j} - \hat{k}$$, $$\vec{b} = \hat{i} - \hat{j}$$ and $$\vec{c} = \hat{i} - \hat{j} - \hat{k}$$ be three given vectors. If $$\vec{r}$$ is a vector such that $$\vec{r} \times \vec{a} = \vec{c} \times \vec{a}$$ and $$\vec{r} \cdot \vec{b} = 0$$, then $$\vec{r} \cdot \vec{a}$$ is equal to ______
We are given $$\vec{a} = \hat{i} + 2\hat{j} - \hat{k}$$, $$\vec{b} = \hat{i} - \hat{j}$$, $$\vec{c} = \hat{i} - \hat{j} - \hat{k}$$, and the conditions $$\vec{r} \times \vec{a} = \vec{c} \times \vec{a}$$ and $$\vec{r} \cdot \vec{b} = 0$$.
From $$\vec{r} \times \vec{a} = \vec{c} \times \vec{a}$$, we get $$(\vec{r} - \vec{c}) \times \vec{a} = \vec{0}$$. This means $$\vec{r} - \vec{c}$$ is parallel to $$\vec{a}$$, so $$\vec{r} = \vec{c} + \lambda\vec{a}$$ for some scalar $$\lambda$$.
Substituting: $$\vec{r} = (1 + \lambda)\hat{i} + (-1 + 2\lambda)\hat{j} + (-1 - \lambda)\hat{k}$$.
Applying the condition $$\vec{r} \cdot \vec{b} = 0$$ where $$\vec{b} = \hat{i} - \hat{j}$$: $$(1 + \lambda)(1) + (-1 + 2\lambda)(-1) + (-1 - \lambda)(0) = 0$$.
This gives $$1 + \lambda + 1 - 2\lambda = 0$$, so $$2 - \lambda = 0$$, hence $$\lambda = 2$$.
Therefore, $$\vec{r} = 3\hat{i} + 3\hat{j} - 3\hat{k}$$.
Computing $$\vec{r} \cdot \vec{a} = 3(1) + 3(2) + (-3)(-1) = 3 + 6 + 3 = 12$$.
Let $$\vec{a} = \hat{i} + 5\hat{j} + \alpha\hat{k}$$, $$\vec{b} = \hat{i} + 3\hat{j} + \beta\hat{k}$$ and $$\vec{c} = -\hat{i} + 2\hat{j} - 3\hat{k}$$ be three vectors such that, $$|\vec{b} \times \vec{c}| = 5\sqrt{3}$$ and $$\vec{a}$$ is perpendicular to $$\vec{b}$$. Then the greatest amongst the values of $$|\vec{a}|^2$$ is _________.
We have the vectors $$\vec a = \hat i + 5\hat j + \alpha \hat k,\; \vec b = \hat i + 3\hat j + \beta \hat k,\; \vec c = -\hat i + 2\hat j - 3 \hat k.$$
The magnitude of the cross-product $$\vec b \times \vec c$$ is given to be $$5\sqrt3,$$ and we also know that $$\vec a$$ is perpendicular to $$\vec b.$$ We shall translate these two statements into algebraic equations step by step.
First, recall the formula for a cross-product of two vectors expressed component-wise: if $$\vec u = (u_1,u_2,u_3)$$ and $$\vec v = (v_1,v_2,v_3),$$ then $$ \vec u \times \vec v = \bigl(u_2v_3 - u_3v_2,\; u_3v_1 - u_1v_3,\; u_1v_2 - u_2v_1\bigr). $$
Applying this to $$\vec b = (1,3,\beta)$$ and $$\vec c = (-1,2,-3),$$ we obtain
$$ \vec b \times \vec c = \Bigl(3(-3) - \beta(2),\; \beta(-1) - 1(-3),\; 1\cdot 2 - 3(-1)\Bigr). $$
Simplifying each component one by one, we get
$$ \vec b \times \vec c = \bigl(-9 - 2\beta,\; -\beta + 3,\; 2 + 3\bigr) = \bigl(-9 - 2\beta,\; 3 - \beta,\; 5\bigr). $$
The squared magnitude of any vector $$\vec v = (v_1,v_2,v_3)$$ is $$|\vec v|^2 = v_1^2 + v_2^2 + v_3^2.$$ Therefore,
$$ \bigl|\vec b \times \vec c\bigr|^2 = (-9 - 2\beta)^2 + (3 - \beta)^2 + 5^2. $$
Expanding each square carefully, we write
$$ (-9 - 2\beta)^2 = (2\beta + 9)^2 = 4\beta^2 + 36\beta + 81, $$ $$ (3 - \beta)^2 = \beta^2 - 6\beta + 9, $$ $$ 5^2 = 25. $$
Adding these three expressions, we obtain
$$ |\vec b \times \vec c|^2 = 4\beta^2 + 36\beta + 81 \;+\; \beta^2 - 6\beta + 9 \;+\; 25 = 5\beta^2 + 30\beta + 115. $$
The question states that $$|\vec b \times \vec c| = 5\sqrt3,$$ so we square both sides to match the expression we have just derived:
$$ |\vec b \times \vec c|^2 = (5\sqrt3)^2 = 25\cdot3 = 75. $$
Equating the two results,
$$ 5\beta^2 + 30\beta + 115 = 75. $$
Subtracting $$75$$ from both sides, we simplify to
$$ 5\beta^2 + 30\beta + 40 = 0. $$
Dividing by $$5$$ throughout gives the quadratic
$$ \beta^2 + 6\beta + 8 = 0. $$
This factors immediately:
$$ (\beta + 2)(\beta + 4) = 0, $$ so $$ \beta = -2 \quad\text{or}\quad \beta = -4. $$
Now we employ the fact that $$\vec a$$ is perpendicular to $$\vec b.$$ The scalar (dot) product formula is
$$ \vec a \cdot \vec b = a_1b_1 + a_2b_2 + a_3b_3. $$
Writing out each component explicitly, we get
$$ \vec a \cdot \vec b = (1)(1) + (5)(3) + (\alpha)(\beta) = 1 + 15 + \alpha\beta = 16 + \alpha\beta. $$
Because the vectors are perpendicular, their dot product must vanish, hence
$$ 16 + \alpha\beta = 0 \quad\Longrightarrow\quad \alpha\beta = -16 \quad\Longrightarrow\quad \alpha = -\frac{16}{\beta}. $$
We now examine each allowed value of $$\beta$$ separately.
Case 1: $$\beta = -2$$. Then $$ \alpha = -\frac{16}{-2} = 8. $$ The squared magnitude of $$\vec a$$ is $$ |\vec a|^2 = 1^2 + 5^2 + \alpha^2 = 1 + 25 + 8^2 = 26 + 64 = 90. $$
Case 2: $$\beta = -4$$. Then $$ \alpha = -\frac{16}{-4} = 4. $$ Now $$ |\vec a|^2 = 1 + 25 + 4^2 = 26 + 16 = 42. $$
Comparing the two possibilities, the greater value of $$|\vec a|^2$$ is clearly $$90.$$
So, the answer is $$90.$$
Let $$\vec{p} = 2\hat{i} + 3\hat{j} + \hat{k}$$ and $$\vec{q} = \hat{i} + 2\hat{j} + \hat{k}$$ be two vectors. If a vector $$\vec{r} = \alpha\hat{i} + \beta\hat{j} + \gamma\hat{k}$$ is perpendicular to each of the vectors $$(\vec{p} + \vec{q})$$ and $$(\vec{p} - \vec{q})$$, and $$|\vec{r}| = \sqrt{3}$$, then $$|\alpha| + |\beta| + |\gamma|$$ is equal to ___.
We have the vectors $$\vec{p}=2\hat{i}+3\hat{j}+\hat{k}$$ and $$\vec{q}=\hat{i}+2\hat{j}+\hat{k}$$. First we form the two combinations that are mentioned in the problem.
Adding the two given vectors, we obtain $$\vec{p}+\vec{q}=(2\hat{i}+\hat{i})+(3\hat{j}+2\hat{j})+(\hat{k}+\hat{k}) =3\hat{i}+5\hat{j}+2\hat{k}.$$
Subtracting them, we get $$\vec{p}-\vec{q}=(2\hat{i}-\hat{i})+(3\hat{j}-2\hat{j})+(\hat{k}-\hat{k}) =\hat{i}+\hat{j}+0\hat{k}.$$
The unknown vector is given as $$\vec{r}=\alpha\hat{i}+\beta\hat{j}+\gamma\hat{k}.$$ It is stated that $$\vec{r}$$ is perpendicular to each of the two vectors found above. The fundamental fact we use is: Two vectors are perpendicular if and only if their dot product is zero.
Applying this to $$\vec{r}$$ and $$\vec{p}+\vec{q}$$, we write $$\vec{r}\cdot(\vec{p}+\vec{q})=0.$$ Using the component-wise formula for the dot product, $$\vec{r}\cdot(\vec{p}+\vec{q}) =(\alpha\hat{i}+\beta\hat{j}+\gamma\hat{k})\cdot(3\hat{i}+5\hat{j}+2\hat{k}) =3\alpha+5\beta+2\gamma=0.$$ So we have our first linear equation: $$3\alpha+5\beta+2\gamma=0.\qquad(1)$$
Next we impose perpendicularity between $$\vec{r}$$ and $$\vec{p}-\vec{q}$$. Thus $$\vec{r}\cdot(\vec{p}-\vec{q})=0,$$ which gives $$(\alpha\hat{i}+\beta\hat{j}+\gamma\hat{k})\cdot(\hat{i}+\hat{j}+0\hat{k}) =\alpha+\beta+0\gamma=0.$$ Hence the second linear equation is $$\alpha+\beta=0.\qquad(2)$$
From equation (2) we can immediately express $$\beta$$ in terms of $$\alpha$$: $$\beta=-\alpha.$$
Substituting $$\beta=-\alpha$$ into equation (1), we obtain $$3\alpha+5(-\alpha)+2\gamma=0 \;\;\Longrightarrow\;\; 3\alpha-5\alpha+2\gamma=0 \;\;\Longrightarrow\;\; -2\alpha+2\gamma=0 \;\;\Longrightarrow\;\; \gamma=\alpha.$$
At this stage we have expressed every component of $$\vec{r}$$ in terms of the single parameter $$\alpha$$: $$\vec{r}=\alpha\hat{i}+(-\alpha)\hat{j}+\alpha\hat{k} =\alpha\big(\hat{i}-\hat{j}+\hat{k}\big).$$
The length of $$\vec{r}$$ is prescribed to be $$\sqrt{3}$$. The magnitude of a scalar multiple obeys $$|\lambda\vec{u}|=|\lambda|\,|\vec{u}|$$. Therefore $$|\vec{r}|=|\alpha|\,\big|\hat{i}-\hat{j}+\hat{k}\big|=\sqrt{3}.$$
We now compute the magnitude of the vector $$\hat{i}-\hat{j}+\hat{k}$$: $$\big|\hat{i}-\hat{j}+\hat{k}\big| =\sqrt{(1)^2+(-1)^2+(1)^2} =\sqrt{1+1+1} =\sqrt{3}.$$
Putting this value into the length condition, we get $$|\alpha|\,\sqrt{3}=\sqrt{3} \;\;\Longrightarrow\;\; |\alpha|=1.$$
Because $$\beta=-\alpha$$ and $$\gamma=\alpha$$, we have $$|\beta|=|\alpha|=1,\qquad|\gamma|=|\alpha|=1.$$
Finally, the required sum is $$|\alpha|+|\beta|+|\gamma|=1+1+1=3.$$
So, the answer is $$3$$.
A vector $$\vec{a} = \alpha\hat{i} + 2\hat{j} + \beta\hat{k}$$ $$(\alpha, \beta \in R)$$ lies in the plane of the vectors, $$\vec{b} = \hat{i} + \hat{j}$$ and $$\vec{c} = \hat{i} - \hat{j} + 4\hat{k}$$. If $$\vec{a}$$ bisects the angle between $$\vec{b}$$ and $$\vec{c}$$, then
We have the three vectors
$$\vec{b}=1\,\hat{i}+1\,\hat{j}+0\,\hat{k},\qquad \vec{c}=1\,\hat{i}-1\,\hat{j}+4\,\hat{k},\qquad \vec{a}=\alpha\,\hat{i}+2\,\hat{j}+\beta\,\hat{k}\;,\; (\alpha,\beta\in\mathbb R).$$
The question tells us two facts about $$\vec{a}:$$
(i) It lies in the plane spanned by $$\vec{b}$$ and $$\vec{c}$$ (this will be automatically true once we use the angle-bisector property), and
(ii) It bisects the angle between $$\vec{b}$$ and $$\vec{c}$$.
In vector geometry the direction of the internal bisector of the angle between two non-zero vectors $$\vec{p}$$ and $$\vec{q}$$ is proportional to $$\dfrac{\vec{p}}{|\vec{p}|}+\dfrac{\vec{q}}{|\vec{q}|},$$ while the direction of the external bisector is proportional to $$\dfrac{\vec{p}}{|\vec{p}|}-\dfrac{\vec{q}}{|\vec{q}|}.$$
We therefore write the two possible bisectors as
$$\vec{a}_{\text{(int)}}=\lambda\left( \frac{\vec{b}}{|\vec{b}|}+\frac{\vec{c}}{|\vec{c}|}\right), \qquad \vec{a}_{\text{(ext)}}=\mu\left( \frac{\vec{b}}{|\vec{b}|}-\frac{\vec{c}}{|\vec{c}|}\right), $$
where $$\lambda$$ and $$\mu$$ are real scalars still to be determined.
Step 1 - Find the magnitudes of $$\vec{b}$$ and $$\vec{c}$$.
$$|\vec{b}|=\sqrt{1^{2}+1^{2}+0^{2}}=\sqrt{2},$$
$$|\vec{c}|=\sqrt{1^{2}+(-1)^{2}+4^{2}} =\sqrt{1+1+16}=\sqrt{18}=3\sqrt{2}.$$
Step 2 - Write the unit vectors.
$$\frac{\vec{b}}{|\vec{b}|} =\left(\frac{1}{\sqrt2}\right)\hat{i} +\left(\frac{1}{\sqrt2}\right)\hat{j} +0\,\hat{k},$$
$$\frac{\vec{c}}{|\vec{c}|} =\left(\frac{1}{3\sqrt2}\right)\hat{i} -\left(\frac{1}{3\sqrt2}\right)\hat{j} +\left(\frac{4}{3\sqrt2}\right)\hat{k}.$$
Step 3 - Internal bisector.
Add the unit vectors:
$$\frac{\vec{b}}{|\vec{b}|}+\frac{\vec{c}}{|\vec{c}|} =\Bigl(\frac{1}{\sqrt2}+\frac{1}{3\sqrt2}\Bigr)\hat{i} +\Bigl(\frac{1}{\sqrt2}-\!\frac{1}{3\sqrt2}\Bigr)\hat{j} +\Bigl(0+\frac{4}{3\sqrt2}\Bigr)\hat{k}$$
$$=\frac{4}{3\sqrt2}\hat{i} +\frac{2}{3\sqrt2}\hat{j} +\frac{4}{3\sqrt2}\hat{k}.$$
Multiply by $$\lambda$$ and equate to $$\vec{a}:$$
$$\alpha=\lambda\frac{4}{3\sqrt2},\qquad 2=\lambda\frac{2}{3\sqrt2},\qquad \beta=\lambda\frac{4}{3\sqrt2}.$$
From the middle equation
$$\lambda=\frac{2\cdot3\sqrt2}{2}=3\sqrt2.$$
This gives $$\alpha=4$$ and $$\beta=4.$$ But none of the given options involve $$\alpha=4$$ or $$\beta=4,$$ so the internal bisector does not match the given form of $$\vec{a}.$$ Hence $$\vec{a}$$ must be the external bisector.
Step 4 - External bisector.
Subtract the unit vectors:
$$\frac{\vec{b}}{|\vec{b}|}-\frac{\vec{c}}{|\vec{c}|} =\Bigl(\frac{1}{\sqrt2}-\frac{1}{3\sqrt2}\Bigr)\hat{i} +\Bigl(\frac{1}{\sqrt2}+\frac{1}{3\sqrt2}\Bigr)\hat{j} +\Bigl(0-\frac{4}{3\sqrt2}\Bigr)\hat{k}$$
$$=\frac{2}{3\sqrt2}\hat{i} +\frac{4}{3\sqrt2}\hat{j} -\frac{4}{3\sqrt2}\hat{k}.$$
Multiply by $$\mu$$ and equate to $$\vec{a}:$$
$$\alpha=\mu\frac{2}{3\sqrt2},\qquad 2 =\mu\frac{4}{3\sqrt2},\qquad \beta=\mu\!\left(-\frac{4}{3\sqrt2}\right).$$
Use the middle equation to find $$\mu$$:
$$2=\mu\frac{4}{3\sqrt2} \;\;\Longrightarrow\;\; \mu=\frac{2\cdot3\sqrt2}{4} =\frac{3\sqrt2}{2}.$$
Substituting this $$\mu$$ back, we get
$$\alpha=\frac{3\sqrt2}{2}\cdot\frac{2}{3\sqrt2}=1,$$ $$\beta=\frac{3\sqrt2}{2}\left(-\frac{4}{3\sqrt2}\right)=-2.$$
Therefore the actual vector is
$$\vec{a}=1\,\hat{i}+2\,\hat{j}-2\,\hat{k}.$$
The coefficient of $$\hat{k}$$ in $$\vec{a}$$ is $$\beta=-2,$$ and this satisfies the simple relation
$$\vec{a}\cdot\hat{k}+\;2 =\beta+2 =-2+2 =0.$$
This relation matches Option C, which is $$\vec{a}\cdot\hat{k}+2=0.$$
Hence, the correct answer is Option C.
Let $$a, b, c \in R$$ be such that $$a^2 + b^2 + c^2 = 1$$. If $$a\cos\theta = b\cos\left(\theta + \frac{2\pi}{3}\right) = c\cos\left(\theta + \frac{4\pi}{3}\right)$$, where $$\theta = \frac{\pi}{9}$$, then the angle between the vectors $$a\hat{i} + b\hat{j} + c\hat{k}$$ and $$b\hat{i} + c\hat{j} + a\hat{k}$$ is:
We begin by denoting the two vectors
$$$\vec{u}=a\hat i+b\hat j+c\hat k,\qquad \vec{v}=b\hat i+c\hat j+a\hat k.$$$
The angle between two vectors is obtained from the well-known formula
$$\cos\phi=\frac{\vec{u}\cdot\vec{v}}{|\vec{u}|\,|\vec{v}|}.$$
Hence our first task is to evaluate the dot product $$\vec{u}\cdot\vec{v}$$.
We are told that
$$$a\cos\theta=b\cos\!\left(\theta+\frac{2\pi}{3}\right)= c\cos\!\left(\theta+\frac{4\pi}{3}\right),\qquad\theta=\frac{\pi}{9}.$$$ For convenience set
$$k=a\cos\theta=b\cos\!\left(\theta+\frac{2\pi}{3}\right)= c\cos\!\left(\theta+\frac{4\pi}{3}\right).$$
From this single constant $$k$$ we can express each coefficient:
$$$a=\frac{k}{\cos\theta},\qquad b=\frac{k}{\cos\!\left(\theta+\frac{2\pi}{3}\right)},\qquad c=\frac{k}{\cos\!\left(\theta+\frac{4\pi}{3}\right)}.$$$
Now we write the dot product explicitly:
$$\vec{u}\cdot\vec{v}=ab+bc+ca.$$ Substituting the expressions found above gives
$$$\vec{u}\cdot\vec{v}=k^{2}\!\left[ \frac{1}{\cos\theta\,\cos\!\left(\theta+\frac{2\pi}{3}\right)}+ \frac{1}{\cos\!\left(\theta+\frac{2\pi}{3}\right)\cos\!\left(\theta+\frac{4\pi}{3}\right)}+ \frac{1}{\cos\!\left(\theta+\frac{4\pi}{3}\right)\cos\theta}\right].$$$
For brevity let us introduce the three cosine values
$$$p=\cos\theta,\qquad q=\cos\!\left(\theta+\frac{2\pi}{3}\right),\qquad r=\cos\!\left(\theta+\frac{4\pi}{3}\right).$$$
In this notation we have
$$\vec{u}\cdot\vec{v}=k^{2}\!\left(\frac1{pq}+\frac1{qr}+\frac1{rp}\right).$$
The bracketed sum can be rewritten by bringing the terms to a common denominator:
$$\frac1{pq}+\frac1{qr}+\frac1{rp}=\frac{r+p+q}{pqr}.$$
Thus the dot product reduces to
$$\vec{u}\cdot\vec{v}=k^{2}\frac{p+q+r}{pqr}.$$
To proceed we need the value of the numerator $$p+q+r$$. A trigonometric identity for three angles that differ by $$120^\circ$$ (or $$\frac{2\pi}{3}$$) is
$$\cos\theta+\cos\!\left(\theta+\frac{2\pi}{3}\right)+ \cos\!\left(\theta+\frac{4\pi}{3}\right)=0.$$ This result can be checked either by the sum-to-product formulas or more elegantly by writing each cosine as the real part of an exponential and using the fact that $$1+e^{i\frac{2\pi}{3}}+e^{i\frac{4\pi}{3}}=0$$. Therefore
$$p+q+r=0.$$
Substituting this zero into the expression for the dot product gives
$$\vec{u}\cdot\vec{v}=k^{2}\frac{0}{pqr}=0.$$
Because $$a^{2}+b^{2}+c^{2}=1$$, the vector $$\vec{u}$$ is non-zero; cyclic symmetry immediately implies $$\vec{v}$$ is also non-zero. Hence $$|\vec{u}|\,|\vec{v}| \neq 0$$, and the cosine of the required angle is
$$$\cos\phi=\frac{\vec{u}\cdot\vec{v}}{|\vec{u}|\,|\vec{v}|} =\frac{0}{|\vec{u}|\,|\vec{v}|}=0.$$$
An angle whose cosine is $$0$$ is $$\displaystyle\frac{\pi}{2}$$ radians (or $$90^\circ$$).
Hence, the correct answer is Option C.
Let the volume of a parallelepiped whose coterminous edges are given by $$\vec{u} = \hat{i} + \hat{j} + \lambda\hat{k}$$, $$\vec{v} = \hat{i} + \hat{j} + 3\hat{k}$$ and $$\vec{w} = 2\hat{i} + \hat{j} + \hat{k}$$ be 1 cu. unit. If $$\theta$$ be the angle between the edges $$\vec{u}$$ and $$\vec{w}$$, then the value of $$\cos\theta$$ can be
We recall that the volume of a parallelepiped whose coterminous edges are the vectors $$\vec u,\;\vec v,\;\vec w$$ is given by the absolute value of the scalar triple product:
$$V=\left|\vec u\cdot(\vec v\times\vec w)\right|.$$
The problem states that this volume equals $$1$$. First we compute the cross-product $$\vec v\times\vec w$$, writing it as the determinant of a $$3\times3$$ matrix:
$$\vec v\times\vec w=\begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\\[2pt] 1 & 1 & 3\\[2pt] 2 & 1 & 1 \end{vmatrix}.$$
Expanding term by term, we have
$$ \vec v\times\vec w =\hat{i}(1\cdot1-3\cdot1)-\hat{j}(1\cdot1-3\cdot2)+\hat{k}(1\cdot1-1\cdot2). $$
Simplifying each bracket:
$$ 1\cdot1-3\cdot1 = -2,\qquad 1\cdot1-3\cdot2 = -5,\qquad 1\cdot1-1\cdot2 = -1. $$
So
$$ \vec v\times\vec w=-2\hat{i}+5\hat{j}-1\hat{k}. $$
Now we take the dot product with $$\vec u=\hat{i}+\hat{j}+\lambda\hat{k}$$:
$$ \vec u\cdot(\vec v\times\vec w) =(1)(-2)+(1)(5)+\lambda(-1) =-2+5-\lambda =3-\lambda. $$
Because the given volume is $$1$$, we impose
$$ |3-\lambda|=1. $$
This single equation yields two possible values of $$\lambda$$:
$$ 3-\lambda=1 \quad\Longrightarrow\quad \lambda=2, $$
or
$$ 3-\lambda=-1 \quad\Longrightarrow\quad \lambda=4. $$
Next we must find the cosine of the angle $$\theta$$ between the edges $$\vec u$$ and $$\vec w$$. Using the definition of the dot product, we state the formula:
$$ \cos\theta=\dfrac{\vec u\cdot\vec w}{\|\vec u\|\,\|\vec w\|}. $$
The vector $$\vec w$$ is fixed:
$$ \vec w = 2\hat{i}+\hat{j}+\hat{k}. $$
First we compute its magnitude:
$$ \|\vec w\| =\sqrt{2^{2}+1^{2}+1^{2}} =\sqrt{4+1+1} =\sqrt6. $$
Now we treat the two admissible values of $$\lambda$$ separately.
(i) For $$\lambda=2$$
We have $$\vec u=\hat{i}+\hat{j}+2\hat{k}$$. The dot product is
$$ \vec u\cdot\vec w =(1)(2)+(1)(1)+2(1) =2+1+2 =5. $$
The magnitude of $$\vec u$$ is
$$ \|\vec u\| =\sqrt{1^{2}+1^{2}+2^{2}} =\sqrt{1+1+4} =\sqrt6. $$
Therefore
$$ \cos\theta =\dfrac{5}{\sqrt6\,\sqrt6} =\dfrac{5}{6}. $$
This value is not present among the given options.
(ii) For $$\lambda=4$$
Now $$\vec u=\hat{i}+\hat{j}+4\hat{k}$$. The dot product is
$$ \vec u\cdot\vec w =(1)(2)+(1)(1)+4(1) =2+1+4 =7. $$
The magnitude of $$\vec u$$ becomes
$$ \|\vec u\| =\sqrt{1^{2}+1^{2}+4^{2}} =\sqrt{1+1+16} =\sqrt{18} =3\sqrt2. $$
So the cosine is
$$ \cos\theta =\frac{7}{(3\sqrt2)(\sqrt6)} =\frac{7}{3\sqrt{12}} =\frac{7}{3\cdot2\sqrt3} =\frac{7}{6\sqrt3}. $$
This value matches Option 2.
Hence, the correct answer is Option 2.
Let $$\vec{a} = \hat{i} - 2\hat{j} + \hat{k}$$ and $$\vec{b} = \hat{i} - \hat{j} + \hat{k}$$ be two vectors. If $$\vec{c}$$ is a vector such that $$\vec{b} \times \vec{c} = \vec{b} \times \vec{a}$$ and $$\vec{c} \cdot \vec{a} = 0$$, then $$\vec{c} \cdot \vec{b}$$ is equal to.
We have the two given vectors
$$\vec a = \hat i - 2\hat j + \hat k \qquad\text{and}\qquad \vec b = \hat i - \hat j + \hat k.$$
A third vector $$\vec c$$ satisfies the two simultaneous conditions
$$\vec b \times \vec c = \vec b \times \vec a \qquad\text{and}\qquad \vec c \cdot \vec a = 0.$$
First, we employ the basic property of the cross product: if two vectors have the same cross product with a non-zero vector $$\vec b,$$ then their difference must be parallel to $$\vec b.$$ Stating the property explicitly:
Formula: $$\vec p \times \vec q = \vec 0 \; \Longrightarrow \; \vec p \parallel \vec q.$$\ Applying it, we write
$$\vec b \times \left(\vec c - \vec a\right) = \vec 0 \;\; \Longrightarrow \;\; \vec c - \vec a \parallel \vec b.$$
So we can express $$\vec c$$ as
$$\vec c = \vec a + \lambda\,\vec b,$$
where $$\lambda$$ is some real scalar that we still need to determine.
Now we impose the second condition $$\vec c \cdot \vec a = 0.$$ Substituting $$\vec c = \vec a + \lambda\vec b$$ gives
$$(\vec a + \lambda\vec b)\cdot\vec a = 0.$$
Expanding the dot product:
$$\vec a\cdot\vec a + \lambda\,\vec b\cdot\vec a = 0.$$
We calculate the two scalar products individually. First, using $$\vec a = (1,\,-2,\,1),$$ we have
$$\vec a\cdot\vec a = 1^2 + (-2)^2 + 1^2 = 1 + 4 + 1 = 6.$$
Next, using $$\vec b = (1,\,-1,\,1),$$ we obtain
$$\vec b\cdot\vec a = 1\cdot1 + (-1)(-2) + 1\cdot1 = 1 + 2 + 1 = 4.$$
Substituting these numerical values into the relation $$\vec a\cdot\vec a + \lambda\,\vec b\cdot\vec a = 0$$ gives
$$6 + \lambda\,(4) = 0.$$
So,
$$4\lambda = -6 \;\;\Longrightarrow\;\; \lambda = -\frac32.$$
Having found $$\lambda,$$ we now require $$\vec c\cdot\vec b.$$ First write $$\vec c$$ explicitly:
$$\vec c = \vec a + \lambda\,\vec b = (1, -2, 1) + \left(-\frac32\right)(1, -1, 1).$$
However, to avoid component-wise arithmetic twice, it is quicker to compute the dot product directly using the linearity of the dot product:
$$\vec c\cdot\vec b = (\vec a + \lambda\,\vec b)\cdot\vec b = \vec a\cdot\vec b + \lambda\,\vec b\cdot\vec b.$$
We already know $$\vec a\cdot\vec b = 4.$$ Next, find $$\vec b\cdot\vec b$$ using $$\vec b = (1,\,-1,\,1):$$
$$\vec b\cdot\vec b = 1^2 + (-1)^2 + 1^2 = 1 + 1 + 1 = 3.$$
Therefore,
$$\vec c\cdot\vec b = 4 + \lambda\,(3).$$
Substitute $$\lambda = -\dfrac32:$$
$$\vec c\cdot\vec b = 4 + \left(-\frac32\right)(3) = 4 - \frac92 = \frac{8}{2} - \frac{9}{2} = -\frac12.$$
Thus the required scalar product is
$$\vec c\cdot\vec b = -\frac12.$$
Hence, the correct answer is Option C.
If the volume of a parallelepiped, whose coterminous edges are given by the vectors $$\vec{a} = \hat{i} + \hat{j} + n\hat{k}$$, $$\vec{b} = 2\hat{i} + 4\hat{j} - n\hat{k}$$ and $$\vec{c} = \hat{i} + n\hat{j} + 3\hat{k}$$ $$(n \geq 0)$$ is 158 cubic units, then:
For a parallelepiped whose coterminous edges are represented by the vectors $$\vec a,\;\vec b,\;\vec c,$$ the volume is given by the absolute value of the scalar triple product, that is
$$V \;=\; \bigl|\,\vec a \cdot (\vec b \times \vec c)\bigr|.$$
We have
$$\vec a = \hat i + \hat j + n\hat k \;=\; (1,\,1,\,n),$$ $$\vec b = 2\hat i + 4\hat j - n\hat k \;=\; (2,\,4,\,-n),$$ $$\vec c = \hat i + n\hat j + 3\hat k \;=\; (1,\,n,\,3).$$
First we find the cross product $$\vec b \times \vec c.$$ Using the determinant form
$$\vec b \times \vec c \;=\; \begin{vmatrix} \hat i & \hat j & \hat k\\[4pt] 2 & 4 & -n\\[4pt] 1 & n & 3 \end{vmatrix},$$
we expand:
$$$ \vec b \times \vec c = \hat i\,(4\cdot 3 - (-n)\cdot n) - \hat j\,(2\cdot 3 - (-n)\cdot 1) + \hat k\,(2\cdot n - 4\cdot 1). $$$
Evaluating each term we obtain
$$$ \vec b \times \vec c = \hat i\,(12 + n^{2}) - \hat j\,(6 + n) + \hat k\,(2n - 4) = \bigl(12 + n^{2},\, -\!(6 + n),\, 2n - 4\bigr). $$$
Now we take the dot product with $$\vec a = (1,\,1,\,n):$$
$$$ \vec a \cdot (\vec b \times \vec c) = 1\,(12 + n^{2}) + 1\,\bigl(-6 - n\bigr) + n\,(2n - 4). $$$
Carrying out the arithmetic step by step:
$$$ 1\,(12 + n^{2}) \;=\; 12 + n^{2}, \quad 1\,\bigl(-6 - n\bigr) \;=\; -6 - n, \quad n\,(2n - 4) \;=\; 2n^{2} - 4n. $$$
Adding these three results gives
$$$ 12 + n^{2} \;+\; (-6 - n) \;+\; (2n^{2} - 4n) = 3n^{2} - 5n + 6. $$$
Hence
$$\vec a \cdot (\vec b \times \vec c) = 3n^{2} - 5n + 6.$$
By the volume formula we must have
$$\bigl|3n^{2} - 5n + 6\bigr| = 158.$$
This gives two algebraic possibilities:
1. $$3n^{2} - 5n + 6 = 158,$$ 2. $$3n^{2} - 5n + 6 = -158.$$
For the first equation:
$$$ 3n^{2} - 5n + 6 = 158 \;\Longrightarrow\; 3n^{2} - 5n - 152 = 0. $$$
Using the quadratic formula $$n = \dfrac{-b \pm \sqrt{b^{2} - 4ac}}{2a}$$ with $$a=3,\; b=-5,\; c=-152,$$ we have
$$$ n = \frac{5 \pm \sqrt{(-5)^{2} - 4\cdot 3 \cdot (-152)}}{2\cdot 3} = \frac{5 \pm \sqrt{25 + 1824}}{6} = \frac{5 \pm \sqrt{1849}}{6}. $$$
Since $$\sqrt{1849} = 43,$$ this becomes
$$$ n = \frac{5 \pm 43}{6}. $$$
Thus
$$$ n = \frac{5 + 43}{6} = \frac{48}{6} = 8 \quad\text{or}\quad n = \frac{5 - 43}{6} = \frac{-38}{6} = -\frac{19}{3}. $$$
Because the problem states $$n \ge 0,$$ we retain only
$$n = 8.$$
For the second equation $$3n^{2} - 5n + 6 = -158$$ we would have
$$$ 3n^{2} - 5n + 164 = 0, $$$
whose discriminant is $$(-5)^{2} - 4\cdot 3\cdot 164 = 25 - 1968 = -1943,$$ a negative number, so this equation has no real solutions. Hence the only admissible value is
$$n = 8.$$
Now we examine the statements offered in the options. We shall substitute $$n = 8$$ into each relevant expression.
Option A: $$\vec a \cdot \vec c = (1,\,1,\,8)\cdot(1,\,8,\,3) = 1\cdot 1 + 1\cdot 8 + 8\cdot 3 = 1 + 8 + 24 = 33.$$ The option claims $$17$$, so it is false.
Option B: $$\vec b \cdot \vec c = (2,\,4,\,-8)\cdot(1,\,8,\,3) = 2\cdot 1 + 4\cdot 8 + (-8)\cdot 3 = 2 + 32 - 24 = 10.$$ This exactly matches the value given in the option, so Option B is true.
Option C: states $$n = 7$$, which contradicts $$n = 8$$; therefore it is false.
Option D: states $$n = 9$$; again this contradicts $$n = 8$$, so it is false.
Only Option B withstands all checks.
Hence, the correct answer is Option B.
Let $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be three unit vectors such that $$\vec{a} + \vec{b} + \vec{c} = 0$$. If $$\lambda = \vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{c} + \vec{c} \cdot \vec{a}$$ and $$\vec{d} = \vec{a} \times \vec{b} + \vec{b} \times \vec{c} + \vec{c} \times \vec{a}$$, then the order pair, $$\left(\lambda, \vec{d}\right)$$, is equal to
We are given three unit vectors $$\vec a ,\; \vec b,\; \vec c$$ satisfying $$\vec a+\vec b+\vec c = 0.$$
First we compute $$\lambda = \vec a\cdot\vec b + \vec b\cdot\vec c + \vec c\cdot\vec a.$$ We start by taking the dot product of the equation $$\vec a+\vec b+\vec c = 0$$ with itself. The dot-product formula $$\vec x\cdot\vec x = |\vec x|^{2}$$ gives
$$\left(\vec a+\vec b+\vec c\right)\cdot\left(\vec a+\vec b+\vec c\right)=0.$$
Expanding the left side term by term, we have
$$\vec a\cdot\vec a + \vec b\cdot\vec b + \vec c\cdot\vec c + 2\left(\vec a\cdot\vec b + \vec b\cdot\vec c + \vec c\cdot\vec a\right)=0.$$
Because each vector is a unit vector, $$\vec a\cdot\vec a=\vec b\cdot\vec b=\vec c\cdot\vec c=1.$$ Substituting these values gives
$$1+1+1 + 2\lambda = 0 \quad\Longrightarrow\quad 3 + 2\lambda = 0.$$
Solving for $$\lambda$$ yields
$$\lambda = -\dfrac{3}{2}.$$
Next we find $$\vec d = \vec a\times\vec b + \vec b\times\vec c + \vec c\times\vec a.$$ From $$\vec a+\vec b+\vec c=0$$ we get $$\vec c = -(\vec a+\vec b).$$ We substitute this expression wherever $$\vec c$$ occurs in $$\vec d$$:
$$\vec d = \vec a\times\vec b + \vec b\times\!\bigl(-(\vec a+\vec b)\bigr) + \bigl(-(\vec a+\vec b)\bigr)\times\vec a.$$
Simplifying each cross product one by one:
$$\vec b\times\!\bigl(-(\vec a+\vec b)\bigr) = -\vec b\times\vec a - \vec b\times\vec b = -\vec b\times\vec a - \vec 0 = -\vec b\times\vec a,$$ since $$\vec b\times\vec b=\vec 0.$$
Similarly,
$$( -(\vec a+\vec b) )\times\vec a = -\vec a\times\vec a - \vec b\times\vec a = -\vec 0 - \vec b\times\vec a = -\vec b\times\vec a.$$
Therefore
$$\vec d = \vec a\times\vec b -\vec b\times\vec a -\vec b\times\vec a.$$
The cross product is anti-commutative, so $$\vec b\times\vec a = -\vec a\times\vec b.$$ Using this fact, each of the last two terms becomes
$$-\vec b\times\vec a = -(-\vec a\times\vec b)= \vec a\times\vec b.$$
Thus we obtain
$$\vec d = \vec a\times\vec b + \vec a\times\vec b + \vec a\times\vec b = 3\,\vec a\times\vec b.$$
Combining both results, the ordered pair $$\left(\lambda,\;\vec d\right)$$ equals
$$\left(-\dfrac{3}{2},\; 3\,\vec a\times\vec b\right).$$
Hence, the correct answer is Option D.
Let $$x_0$$ be the point of local maxima of $$f(x) = \vec{a} \cdot (\vec{b} \times \vec{c})$$, where $$\vec{a} = x\hat{i} - 2\hat{j} + 3\hat{k}$$, $$\vec{b} = -2\hat{i} + x\hat{j} - \hat{k}$$ and $$\vec{c} = 7\hat{i} - 2\hat{j} + x\hat{k}$$. Then the value of $$\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{c} + \vec{c} \cdot \vec{a}$$ at $$x = x_0$$ is:
We have the vector-valued function $$f(x)=\vec a\cdot(\vec b\times\vec c)$$ where
$$\vec a=x\hat i-2\hat j+3\hat k,\qquad \vec b=-2\hat i+x\hat j-\hat k,\qquad \vec c=7\hat i-2\hat j+x\hat k.$$
First we evaluate the cross product $$\vec b\times\vec c$$. Using the formula for the determinant of a $$3\times3$$ matrix,
$$ \vec b\times\vec c= \begin{vmatrix} \hat i&\hat j&\hat k\\ -2&x&-1\\ 7&-2&x \end{vmatrix}. $$
Expanding this determinant:
$$ \vec b\times\vec c= \hat i\bigl(x\cdot x-(-1)(-2)\bigr) -\hat j\bigl((-2)\cdot x-(-1)\cdot7\bigr) +\hat k\bigl((-2)(-2)-x\cdot7\bigr). $$
Simplifying each component one by one:
$$ \hat i:\;x^2-2,\qquad \hat j:\;-\bigl(-2x+7\bigr)=2x-7,\qquad \hat k:\;4-7x. $$
So
$$\vec b\times\vec c=(\,x^2-2\,)\hat i+(\,2x-7\,)\hat j+(\,4-7x\,)\hat k.$$
Next we compute the dot product $$\vec a\cdot(\vec b\times\vec c)$$. Using the component-wise dot-product formula,
$$ \vec a\cdot(\vec b\times\vec c)= x\,(x^2-2)+(-2)\,(2x-7)+3\,(4-7x). $$
Multiplying out each term:
$$ x(x^2-2)=x^3-2x, \qquad (-2)(2x-7)=-4x+14, \qquad 3(4-7x)=12-21x. $$
Adding them together gives
$$ f(x)=x^3-2x-4x+14+12-21x =x^3-27x+26. $$
To find local extrema we differentiate. The derivative is
$$ f'(x)=\frac{d}{dx}(x^3-27x+26)=3x^2-27 =3(x^2-9)=3(x-3)(x+3). $$
Setting $$f'(x)=0$$ yields critical points $$x=3$$ and $$x=-3$$. We now apply the second-derivative test. The second derivative is
$$ f''(x)=\frac{d}{dx}\bigl(3x^2-27\bigr)=6x. $$
At $$x=3$$ we have $$f''(3)=18\gt 0$$ (concave up), so $$x=3$$ is a local minimum. At $$x=-3$$ we have $$f''(-3)=-18\lt 0$$ (concave down), so $$x=-3$$ is the point of local maximum. Thus $$x_0=-3.$$
Now we need the value of $$\vec a\cdot\vec b+\vec b\cdot\vec c+\vec c\cdot\vec a$$ at this $$x_0$$. We evaluate each dot product symbolically first.
Using $$\vec a=(x,-2,3),\ \vec b=(-2,x,-1),\ \vec c=(7,-2,x):$$
$$ \vec a\cdot\vec b =x(-2)+(-2)(x)+3(-1) =-2x-2x-3 =-4x-3. $$
$$ \vec b\cdot\vec c =(-2)(7)+x(-2)+(-1)(x) =-14-2x-x =-14-3x. $$
$$ \vec c\cdot\vec a =(7)(x)+(-2)(-2)+x(3) =7x+4+3x =10x+4. $$
Adding these three results:
$$ \vec a\cdot\vec b+\vec b\cdot\vec c+\vec c\cdot\vec a =(-4x-3)+(-14-3x)+(10x+4) =(-4x-3x+10x)+(-3-14+4) =3x-13. $$
Finally, substitute $$x=x_0=-3$$ obtained earlier:
$$ 3(-3)-13=-9-13=-22. $$
Hence, the correct answer is Option D.
If the vectors, $$\vec{p} = (a+1)\hat{i} + a\hat{j} + a\hat{k}$$, $$\vec{q} = a\hat{i} + (a+1)\hat{j} + a\hat{k}$$ and $$\vec{r} = a\hat{i} + a\hat{j} + (a+1)\hat{k}$$ $$(a \in R)$$ are coplanar and $$3(\vec{p} \cdot \vec{q})^2 - \lambda|\vec{r} \times \vec{q}|^2 = 0$$, then the value of $$\lambda$$ is ___________.
To ensure that the three given vectors are coplanar we recall the scalar-triple-product condition: for vectors $$\vec{p},\;\vec{q},\;\vec{r}$$ we must have $$\vec{p}\cdot(\vec{q}\times\vec{r})=0.$$
Writing each vector in component form, we obtain the determinant
$$$\vec{p}\cdot(\vec{q}\times\vec{r})= \begin{vmatrix} a+1 & a & a\\ a & a+1 & a\\ a & a & a+1 \end{vmatrix}.$$$
Expanding this determinant along the first row, we get
$$$\begin{aligned} \bigl(a+1\bigr)\Bigl[(a+1)(a+1)-a^{2}\Bigr] \;&-;; a\Bigl[a(a+1)-a^{2}\Bigr] \;+\; a\Bigl[a^{2}-a(a+1)\Bigr]. \end{aligned}$$$
Simplifying each bracket separately,
$$$\begin{aligned} (a+1)(a+1)-a^{2}&=a^{2}+2a+1-a^{2}=2a+1,\\[2mm] a(a+1)-a^{2}&=a^{2}+a-a^{2}=a,\\[2mm] a^{2}-a(a+1)&=a^{2}-a^{2}-a=-a. \end{aligned}$$$
Substituting these back,
$$$\begin{aligned} \vec{p}\cdot(\vec{q}\times\vec{r}) &=(a+1)(2a+1)-a(a)+a(-a)\\[2mm] &=2a^{2}+3a+1-a^{2}-a^{2}\\[2mm] &=3a+1. \end{aligned}$$$
The coplanarity requirement $$3a+1=0$$ therefore gives
$$a=-\dfrac13.$$
Next we evaluate $$\vec{p}\cdot\vec{q}.$$ Using the usual dot-product formula,
$$$\begin{aligned} \vec{p}\cdot\vec{q} &=(a+1)(a)+a(a+1)+a\cdot a\\[2mm] &=a(a+1)+a(a+1)+a^{2}\\[2mm] &=2a(a+1)+a^{2}\\[2mm] &=2(a^{2}+a)+a^{2}\\[2mm] &=3a^{2}+2a. \end{aligned}$$$
Putting $$a=-\dfrac13$$ we obtain
$$$\vec{p}\cdot\vec{q}=3\!\left(\dfrac{1}{9}\right)+2\!\left(-\dfrac13\right) =\dfrac13-\dfrac23=-\dfrac13.$$$
We now compute $$\vec{r}\times\vec{q}.$$ For components $$\vec{r}=(a,a,a+1)$$ and $$\vec{q}=(a,a+1,a),$$ the cross-product formula
$$$\vec{r}\times\vec{q}=\bigl(r_{2}q_{3}-r_{3}q_{2},\;r_{3}q_{1}-r_{1}q_{3},\;r_{1}q_{2}-r_{2}q_{1}\bigr)$$$
gives
$$$\begin{aligned} r_{2}q_{3}-r_{3}q_{2}&=a\cdot a-(a+1)(a+1)=a^{2}-(a+1)^{2}=-(2a+1),\\[2mm] r_{3}q_{1}-r_{1}q_{3}&=(a+1)\,a-a\cdot a=a(a+1)-a^{2}=a,\\[2mm] r_{1}q_{2}-r_{2}q_{1}&=a\,(a+1)-a\cdot a=a(a+1)-a^{2}=a. \end{aligned}$$$
Hence
$$\vec{r}\times\vec{q}=(-(2a+1),\,a,\,a).$$
The square of its magnitude is therefore
$$$\begin{aligned} \bigl|\vec{r}\times\vec{q}\bigr|^{2} &=(2a+1)^{2}+a^{2}+a^{2}\\[2mm] &=4a^{2}+4a+1+2a^{2}\\[2mm] &=6a^{2}+4a+1. \end{aligned}$$$
Substituting $$a=-\dfrac13,$$
$$$\bigl|\vec{r}\times\vec{q}\bigr|^{2}=6\!\left(\dfrac19\right)+4\!\left(-\dfrac13\right)+1 =\dfrac23-\dfrac43+1=\dfrac13.$$$
The problem states that
$$3(\vec{p}\cdot\vec{q})^{2}-\lambda\bigl|\vec{r}\times\vec{q}\bigr|^{2}=0.$$
Using $$(\vec{p}\cdot\vec{q})^{2}=\left(-\dfrac13\right)^{2}=\dfrac19$$ and $$\bigl|\vec{r}\times\vec{q}\bigr|^{2}=\dfrac13,$$ we have
$$$3\!\left(\dfrac19\right)-\lambda\!\left(\dfrac13\right)=0 \;\;\Longrightarrow\;\; \dfrac13-\dfrac{\lambda}{3}=0.$$$
Multiplying by 3 gives $$1-\lambda=0,$$ so
$$\lambda=1.$$
Hence, the correct answer is Option A.
Let the vectors $$\vec{a}$$, $$\vec{b}$$, $$\vec{c}$$ be such that $$|\vec{a}| = 2$$, $$|\vec{b}| = 4$$ and $$|\vec{c}| = 4$$. If the projection of $$\vec{b}$$ on $$\vec{a}$$ is equal to the projection of $$\vec{c}$$ on $$\vec{a}$$ and $$\vec{b}$$ is perpendicular to $$\vec{c}$$, then the value of $$|\vec{a} + \vec{b} - \vec{c}|$$ is...
We have three vectors $$\vec{a},\;\vec{b},\;\vec{c}$$ whose magnitudes are given as $$|\vec{a}| = 2,\;|\vec{b}| = 4,\;|\vec{c}| = 4.$$
The problem states that the projection of $$\vec{b}$$ on $$\vec{a}$$ is equal to the projection of $$\vec{c}$$ on $$\vec{a}$$. The scalar projection (sometimes called the component) of a vector $$\vec{u}$$ on another vector $$\vec{v}$$ is defined by the formula
$$\text{proj}_{\vec{v}}(\vec{u}) \;=\; \frac{\vec{v}\!\cdot\!\vec{u}}{|\vec{v}|}.$$
Applying this to the two given projections, we get
$$\frac{\vec{a}\!\cdot\!\vec{b}}{|\vec{a}|} \;=\; \frac{\vec{a}\!\cdot\!\vec{c}}{|\vec{a}|}.$$
Because $$|\vec{a}| \neq 0$$, we can multiply both sides by $$|\vec{a}|$$ and conclude
$$\vec{a}\!\cdot\!\vec{b} \;=\; \vec{a}\!\cdot\!\vec{c}.$$
Let us denote this common dot product by $$k$$, so that
$$\vec{a}\!\cdot\!\vec{b} = k \quad\text{and}\quad \vec{a}\!\cdot\!\vec{c} = k.$$
Next, we are told that $$\vec{b}$$ is perpendicular to $$\vec{c}$$. Two vectors are perpendicular precisely when their dot product is zero, so
$$\vec{b}\!\cdot\!\vec{c} = 0.$$
Our goal is to find the magnitude of the vector $$\vec{a} + \vec{b} - \vec{c}.$$ A convenient way is to compute its squared magnitude first. For any vector $$\vec{u}$$, we have $$|\vec{u}|^2 = \vec{u}\!\cdot\!\vec{u}.$$ Hence,
$$|\vec{a} + \vec{b} - \vec{c}|^2 \;=\; (\vec{a} + \vec{b} - \vec{c}) \!\cdot\! (\vec{a} + \vec{b} - \vec{c}).$$
We now expand this dot product term by term, remembering the distributive and commutative properties of the dot product:
$$$\begin{aligned} (\vec{a} + \vec{b} - \vec{c}) \!\cdot\! (\vec{a} + \vec{b} - \vec{c}) &= \vec{a}\!\cdot\!\vec{a} \;+\; \vec{b}\!\cdot\!\vec{b} \;+\; (-\vec{c})\!\cdot\!(-\vec{c}) \\ &\quad+ 2\bigl(\vec{a}\!\cdot\!\vec{b}\bigr) \;-\; 2\bigl(\vec{a}\!\cdot\!\vec{c}\bigr) \;-\; 2\bigl(\vec{b}\!\cdot\!\vec{c}\bigr). \end{aligned}$$$
Let us evaluate each of these terms one by one.
First, the three pure magnitude terms are simply the squares of the magnitudes already known:
$$\vec{a}\!\cdot\!\vec{a} = |\vec{a}|^2 = 2^2 = 4,$$ $$\vec{b}\!\cdot\!\vec{b} = |\vec{b}|^2 = 4^2 = 16,$$ $$(-\vec{c})\!\cdot\!(-\vec{c}) = |\vec{c}|^2 = 4^2 = 16.$$
Next, for the mixed terms we use the relations established earlier:
$$2\bigl(\vec{a}\!\cdot\!\vec{b}\bigr) = 2k,$$ $$-\,2\bigl(\vec{a}\!\cdot\!\vec{c}\bigr) = -\,2k,$$ $$-\,2\bigl(\vec{b}\!\cdot\!\vec{c}\bigr) = -\,2(0) = 0.$$
Notice that $$2k - 2k = 0,$$ so the mixed terms cancel out completely.
Putting everything together, we obtain
$$$\begin{aligned} |\vec{a} + \vec{b} - \vec{c}|^2 &= 4 + 16 + 16 + 0 \\ &= 36. \end{aligned}$$$
Finally, taking the positive square root (because magnitude is always non-negative), we get
$$|\vec{a} + \vec{b} - \vec{c}| = \sqrt{36} = 6.$$
So, the answer is $$6$$.
Let $$\vec{a}, \vec{b}$$ and $$\vec{c}$$ be three vectors such that $$|\vec{a}| = \sqrt{3}$$, $$|\vec{b}| = 5$$, $$\vec{b} \cdot \vec{c} = 10$$ and the angle between $$\vec{b}$$ and $$\vec{c}$$ is $$\frac{\pi}{3}$$. If $$\vec{a}$$ is perpendicular to the vector $$\vec{b} \times \vec{c}$$, then $$\left|\vec{a} \times (\vec{b} \times \vec{c})\right|$$ is equal to ___________.
We have the data
$$|\vec a|=\sqrt3,\qquad |\vec b|=5,\qquad \vec b\cdot\vec c=10,\qquad\text{angle between }\vec b\ \text{and}\ \vec c=\frac{\pi}{3}.$$
First we determine $$|\vec c|.$$ From the definition of the dot product,
$$\vec b\cdot\vec c=|\vec b|\,|\vec c|\cos\frac{\pi}{3}.$$
Substituting the given numbers,
$$10=5\cdot|\vec c|\cdot\frac12\;\Longrightarrow\;|\vec c|=\frac{10}{5}\cdot2=4.$$
Now we use the fact that $$\vec a\perp(\vec b\times\vec c).$$ Because $$\vec b\times\vec c$$ is perpendicular to both $$\vec b$$ and $$\vec c,$$ the condition $$\vec a\cdot(\vec b\times\vec c)=0$$ tells us that the three vectors $$\vec a,\vec b,\vec c$$ are coplanar; hence we may place them conveniently in the same plane without loss of generality.
Choose a right-handed coordinate system so that
$$\vec b=(5,0,0),$$
and let $$\vec c$$ make an angle $$\frac{\pi}{3}$$ with $$\vec b$$ inside the $$xy$$-plane. Using $$|\vec c|=4$$ and $$\cos\frac{\pi}{3}=1/2$$, we write
$$\vec c=(4\cos\tfrac{\pi}{3},\,4\sin\tfrac{\pi}{3},\,0)=(2,\,2\sqrt3,\,0).$$
Then
$$\vec b\times\vec c=\begin{vmatrix} \hat i & \hat j & \hat k\\[4pt] 5 & 0 & 0\\[4pt] 2 & 2\sqrt3 & 0 \end{vmatrix}=10\sqrt3\,\hat k=(0,0,10\sqrt3).$$
Because $$\vec a\perp(\vec b\times\vec c)$$ and the cross product is along the $$z$$-axis, $$\vec a$$ has no $$z$$-component. Write
$$\vec a=(x,y,0),\qquad x^2+y^2=|\vec a|^2=(\sqrt3)^2=3.$$
We need $$\bigl|\vec a\times(\vec b\times\vec c)\bigr|.$$ Before substituting numbers, recall the vector triple-product formula
$$\;\vec a\times(\vec b\times\vec c)=\vec b\,(\vec a\cdot\vec c)-\vec c\,(\vec a\cdot\vec b)\;. $$
Compute the two dot products:
$$\vec a\cdot\vec b=(x,y,0)\cdot(5,0,0)=5x,$$
$$\vec a\cdot\vec c=(x,y,0)\cdot(2,2\sqrt3,0)=2x+2\sqrt3\,y.$$
Hence
$$\vec a\times(\vec b\times\vec c)=\bigl[\,\vec b\,(2x+2\sqrt3\,y)\bigr]-\bigl[\,\vec c\,(5x)\bigr].$$
Substituting $$\vec b=(5,0,0)$$ and $$\vec c=(2,2\sqrt3,0)$$ gives
$$\vec a\times(\vec b\times\vec c)=\bigl(5,0,0\bigr)(2x+2\sqrt3\,y)-\bigl(2,2\sqrt3,0\bigr)(5x).$$
Multiplying out each term separately,
$$\vec b\,(2x+2\sqrt3\,y)=(10x+10\sqrt3\,y,\,0,\,0),$$
$$\vec c\,(5x)=(10x,\,10\sqrt3\,x,\,0).$$
Subtracting,
$$\vec a\times(\vec b\times\vec c)=\bigl(10\sqrt3\,y,\, -10\sqrt3\,x,\,0\bigr) =10\sqrt3\,(y,-x,0).$$
The magnitude is therefore
$$\bigl|\vec a\times(\vec b\times\vec c)\bigr| =10\sqrt3\,\sqrt{y^{2}+x^{2}} =10\sqrt3\,\sqrt{3} =10\cdot3=30,$$
because $$x^{2}+y^{2}=3.$$ Notice that the result is independent of the particular directions of $$\vec a$$ inside the plane, so the value $$30$$ is unique.
So, the answer is $$30$$.
If $$\vec{a} = 2\hat{i} + \hat{j} + 2\hat{k}$$, then the value of $$\left|\hat{i} \times (\vec{a} \times \hat{i})\right|^2 + \left|\hat{j} \times (\vec{a} \times \hat{j})\right|^2 + \left|\hat{k} \times (\vec{a} \times \hat{k})\right|^2$$, is equal to:
We have the given vector $$\vec{a}=2\hat{i}+\hat{j}+2\hat{k}.$$
The required expression is
$$\left|\hat{i}\times(\vec{a}\times\hat{i})\right|^{2}\;+\;\left|\hat{j}\times(\vec{a}\times\hat{j})\right|^{2}\;+\;\left|\hat{k}\times(\vec{a}\times\hat{k})\right|^{2}.$$
To evaluate each term quickly, we shall use the well-known vector triple product formula:
$$\vec{p}\times(\vec{q}\times\vec{r})=\vec{q}\,(\vec{p}\cdot\vec{r})-\vec{r}\,(\vec{p}\cdot\vec{q}).$$
First we take $$\vec{p}=\hat{i},\;\vec{q}=\vec{a},\;\vec{r}=\hat{i}.$$ Applying the formula, we get
$$\hat{i}\times(\vec{a}\times\hat{i})=\vec{a}\,(\hat{i}\cdot\hat{i})-\hat{i}\,(\hat{i}\cdot\vec{a}).$$
Now, $$\hat{i}\cdot\hat{i}=1$$ and $$\hat{i}\cdot\vec{a}=2.$$ Substituting these,
$$\hat{i}\times(\vec{a}\times\hat{i})=\vec{a}-2\hat{i}.$$
Explicitly,
$$\vec{a}-2\hat{i}=(2\hat{i}+\hat{j}+2\hat{k})-2\hat{i}=0\hat{i}+1\hat{j}+2\hat{k}.$$
The magnitude squared of this vector is
$$|0\hat{i}+1\hat{j}+2\hat{k}|^{2}=0^{2}+1^{2}+2^{2}=0+1+4=5.$$
Next, we take $$\vec{p}=\hat{j},\;\vec{q}=\vec{a},\;\vec{r}=\hat{j}.$$ Using the same formula,
$$\hat{j}\times(\vec{a}\times\hat{j})=\vec{a}\,(\hat{j}\cdot\hat{j})-\hat{j}\,(\hat{j}\cdot\vec{a}).$$
Here, $$\hat{j}\cdot\hat{j}=1$$ and $$\hat{j}\cdot\vec{a}=1.$$ So,
$$\hat{j}\times(\vec{a}\times\hat{j})=\vec{a}-\hat{j}.$$ That is,
$$\vec{a}-\hat{j}=(2\hat{i}+\hat{j}+2\hat{k})-\hat{j}=2\hat{i}+0\hat{j}+2\hat{k}.$$
The corresponding magnitude squared is
$$|2\hat{i}+0\hat{j}+2\hat{k}|^{2}=2^{2}+0^{2}+2^{2}=4+0+4=8.$$
Finally, we choose $$\vec{p}=\hat{k},\;\vec{q}=\vec{a},\;\vec{r}=\hat{k}.$$ Again,
$$\hat{k}\times(\vec{a}\times\hat{k})=\vec{a}\,(\hat{k}\cdot\hat{k})-\hat{k}\,(\hat{k}\cdot\vec{a}).$$
Because $$\hat{k}\cdot\hat{k}=1$$ and $$\hat{k}\cdot\vec{a}=2,$$ we have
$$\hat{k}\times(\vec{a}\times\hat{k})=\vec{a}-2\hat{k}.$$
So explicitly,
$$\vec{a}-2\hat{k}=(2\hat{i}+\hat{j}+2\hat{k})-2\hat{k}=2\hat{i}+1\hat{j}+0\hat{k}.$$
The magnitude squared of this vector equals
$$|2\hat{i}+1\hat{j}+0\hat{k}|^{2}=2^{2}+1^{2}+0^{2}=4+1+0=5.$$
Adding all three obtained values, we get
$$5+8+5=18.$$
So, the answer is $$18$$.
If $$\vec{a}$$ and $$\vec{b}$$ are unit vectors, then the greatest value of $$\sqrt{3}|\vec{a} + \vec{b}| + |\vec{a} - \vec{b}|$$ is___.
Let $$\vec a$$ and $$\vec b$$ be unit vectors. Hence we have $$|\vec a| = 1$$ and $$|\vec b| = 1$$. Let the angle between the two vectors be $$\theta$$, so that $$\vec a\cdot\vec b = |\vec a||\vec b|\cos\theta = \cos\theta$$.
First we write the standard formula for the magnitude of the sum of two vectors:
$$|\vec a+\vec b|^2 = |\vec a|^2 + |\vec b|^2 + 2\vec a\cdot\vec b.$$
Substituting $$|\vec a|=1,\;|\vec b|=1,\;\vec a\cdot\vec b=\cos\theta$$ we get
$$|\vec a+\vec b|^2 = 1 + 1 + 2\cos\theta = 2 + 2\cos\theta = 2(1+\cos\theta).$$
Taking the square root,
$$|\vec a+\vec b| = \sqrt{2(1+\cos\theta)}.$$
Exactly in the same way, for the difference we use
$$|\vec a-\vec b|^2 = |\vec a|^2 + |\vec b|^2 - 2\vec a\cdot\vec b.$$
Again substituting the same values,
$$|\vec a-\vec b|^2 = 1 + 1 - 2\cos\theta = 2 - 2\cos\theta = 2(1-\cos\theta).$$
Therefore
$$|\vec a-\vec b| = \sqrt{2(1-\cos\theta)}.$$
Now we simplify each square root by expressing $$1\pm\cos\theta$$ in half-angle form. We recall the trigonometric identities
$$1+\cos\theta = 2\cos^2\frac\theta2,\qquad 1-\cos\theta = 2\sin^2\frac\theta2.$$
Substituting these into the magnitudes we get
$$|\vec a+\vec b| = \sqrt{2\cdot 2\cos^2\frac\theta2} = \sqrt{4\cos^2\frac\theta2} = 2\left|\cos\frac\theta2\right|,$$
$$|\vec a-\vec b| = \sqrt{2\cdot 2\sin^2\frac\theta2} = \sqrt{4\sin^2\frac\theta2} = 2\left|\sin\frac\theta2\right|.$$
Because the absolute value bars already appear, we may let $$\phi=\dfrac{\theta}{2}$$ and consider $$\phi\in[0,\pi]$$. In the interval $$[0,\tfrac\pi2]$$ both sine and cosine are non-negative, and by symmetry the same maximum is obtained there, so we may drop the absolute values for maximisation. Setting
$$f(\phi)=\sqrt3\,|\vec a+\vec b|+|\vec a-\vec b| = \sqrt3\,(2\cos\phi)+2\sin\phi = 2\bigl(\sqrt3\cos\phi+\sin\phi\bigr),$$
we need to maximise
$$g(\phi)=\sqrt3\cos\phi+\sin\phi\quad\text{for }0\le\phi\le\dfrac\pi2.$$
We differentiate $$g(\phi)$$:
$$\dfrac{dg}{d\phi} = -\sqrt3\sin\phi + \cos\phi.$$
The critical point is obtained by setting the derivative equal to zero:
$$-\sqrt3\sin\phi + \cos\phi = 0 \;\Longrightarrow\; \cos\phi = \sqrt3\sin\phi \;\Longrightarrow\; \tan\phi = \dfrac1{\sqrt3}.$$
Thus
$$\phi = \tan^{-1}\!\left(\dfrac1{\sqrt3}\right) = \dfrac\pi6.$$
To confirm that this point is a maximum, we compute the second derivative:
$$\dfrac{d^2g}{d\phi^2} = -\sqrt3\cos\phi - \sin\phi,$$
and substituting $$\phi=\dfrac\pi6$$ gives
$$\dfrac{d^2g}{d\phi^2}\Big|_{\phi=\pi/6} = -\sqrt3\left(\dfrac{\sqrt3}{2}\right) - \dfrac12 = -\dfrac32 - \dfrac12 = -2 < 0,$$
so the function indeed attains a maximum there.
Evaluating $$g(\phi)$$ at $$\phi=\dfrac\pi6$$:
$$g\!\left(\dfrac\pi6\right) = \sqrt3\cos\!\left(\dfrac\pi6\right) + \sin\!\left(\dfrac\pi6\right) = \sqrt3\left(\dfrac{\sqrt3}{2}\right) + \dfrac12 = \dfrac32 + \dfrac12 = 2.$$
Therefore the maximum value of the original expression is
$$f_{\max} = 2 \times g_{\max} = 2 \times 2 = 4.$$
Hence, the correct answer is Option 4.
If $$\vec{x}$$ and $$\vec{y}$$ be two non-zero vectors such that $$|\vec{x} + \vec{y}| = |\vec{x}|$$ and $$2\vec{x} + \lambda\vec{y}$$ is perpendicular to $$\vec{y}$$, then the value of $$\lambda$$ is_____.
Let us translate the given geometric conditions into algebra. We are told that the two non-zero vectors $$\vec{x}$$ and $$\vec{y}$$ satisfy the length (magnitude) equation
$$|\vec{x}+\vec{y}| \;=\;|\vec{x}|.$$
First we square both sides, because the square of a magnitude is easier to expand by the dot product. Using the fact that, for any vector $$\vec{a},$$ we have $$|\vec{a}|^{2}=\vec{a}\cdot\vec{a},$$ we write
$$|\vec{x}+\vec{y}|^{2} \;=\; |\vec{x}|^{2}.$$
Now expand the left-hand side by the distributive property of the dot product:
$$ \begin{aligned} |\vec{x}+\vec{y}|^{2} &= (\vec{x}+\vec{y})\cdot(\vec{x}+\vec{y}) \\ &= \vec{x}\cdot\vec{x} + 2\vec{x}\cdot\vec{y} + \vec{y}\cdot\vec{y} \\ &= |\vec{x}|^{2} + 2\vec{x}\cdot\vec{y} + |\vec{y}|^{2}. \end{aligned} $$
Equating this with the right-hand side $$|\vec{x}|^{2}$$ gives
$$|\vec{x}|^{2} + 2\vec{x}\cdot\vec{y} + |\vec{y}|^{2} \;=\; |\vec{x}|^{2}.$$
The $$|\vec{x}|^{2}$$ terms on both sides cancel, leaving
$$2\vec{x}\cdot\vec{y} + |\vec{y}|^{2} \;=\;0.$$
We can solve this relation for the scalar product $$\vec{x}\cdot\vec{y}:$$
$$2\vec{x}\cdot\vec{y} \;=\; -|\vec{y}|^{2} \quad\Longrightarrow\quad \vec{x}\cdot\vec{y} \;=\; -\dfrac{|\vec{y}|^{2}}{2}.$$
Next, we use the perpendicularity condition that the vector $$2\vec{x}+\lambda\vec{y}$$ is perpendicular to $$\vec{y}.$$ Two vectors are perpendicular precisely when their dot product is zero. Therefore,
$$(2\vec{x}+\lambda\vec{y})\cdot\vec{y} \;=\;0.$$
Expand this dot product:
$$ \begin{aligned} (2\vec{x}+\lambda\vec{y})\cdot\vec{y} &= 2\vec{x}\cdot\vec{y} + \lambda\,\vec{y}\cdot\vec{y} \\ &= 2\vec{x}\cdot\vec{y} + \lambda|\vec{y}|^{2}. \end{aligned} $$
Set this equal to zero as required:
$$2\vec{x}\cdot\vec{y} + \lambda|\vec{y}|^{2} \;=\;0.$$
We already found $$2\vec{x}\cdot\vec{y} = -|\vec{y}|^{2}.$$ Substituting this value, we obtain
$$-|\vec{y}|^{2} + \lambda|\vec{y}|^{2} \;=\;0.$$
Factor out the common non-zero factor $$|\vec{y}|^{2}:$$
$$|\vec{y}|^{2}\,(\lambda - 1) \;=\;0.$$
Since $$\vec{y}$$ is non-zero, its magnitude $$|\vec{y}|^{2}$$ is strictly positive, so the only way for the product to vanish is
$$\lambda - 1 \;=\;0 \quad\Longrightarrow\quad \lambda = 1.$$
Hence, the correct answer is Option 1.
Let the position vectors of points 'A' and 'B' be $$\hat{i} + \hat{j} + \hat{k}$$ and $$2\hat{i} + \hat{j} + 3\hat{k}$$, respectively. A point 'P' divides the line segment AB internally in the ratio $$\lambda : 1$$ $$(\lambda > 0)$$. If O is the origin and $$\vec{OB} \cdot \vec{OP} - 3|\vec{OA} \times \vec{OP}|^2 = 6$$ then $$\lambda$$ is equal to ___________.
We have the position vectors of the two fixed points
$$\vec{OA}=1\hat i+1\hat j+1\hat k=(1,1,1),\qquad \vec{OB}=2\hat i+1\hat j+3\hat k=(2,1,3).$$
A point $$P$$ divides the line segment $$AB$$ internally in the ratio $$\lambda:1\;(\lambda>0).$$ For internal division, the section-formula tells us
$$\vec{OP}=\frac{\lambda\,\vec{B}+1\,\vec{A}}{\lambda+1}.$$
Substituting $$\vec{A}=(1,1,1)$$ and $$\vec{B}=(2,1,3)$$ we obtain
$$\vec{OP}= \frac{\lambda(2,1,3)+(1,1,1)}{\lambda+1} =\frac{(2\lambda+1,\;\lambda+1,\;3\lambda+1)}{\lambda+1} =\left(\frac{2\lambda+1}{\lambda+1},\;1,\;\frac{3\lambda+1}{\lambda+1}\right).$$
Now we evaluate the two vector expressions that appear in the given condition.
1. The dot product $$\vec{OB}\cdot\vec{OP}$$
$$\vec{OB}\cdot\vec{OP} =2\left(\frac{2\lambda+1}{\lambda+1}\right) +1\left(1\right) +3\left(\frac{3\lambda+1}{\lambda+1}\right) =\frac{4\lambda+2+\lambda+1+9\lambda+3}{\lambda+1} =\frac{14\lambda+6}{\lambda+1}.$$
2. The cross product $$\vec{OA}\times\vec{OP}$$
Writing $$\vec{OA}=(1,1,1)$$ and $$\vec{OP}=\left(\dfrac{2\lambda+1}{\lambda+1},\,1,\,\dfrac{3\lambda+1}{\lambda+1}\right)$$, the determinant form gives
$$\vec{OA}\times\vec{OP} =\Bigl(\,OP_z-1,\;OP_x-OP_z,\;1-OP_x\Bigr).$$
Because $$OP_x=\dfrac{2\lambda+1}{\lambda+1}$$ and $$OP_z=\dfrac{3\lambda+1}{\lambda+1},$$ we have
$$OP_z-1=\frac{3\lambda+1}{\lambda+1}-1 =\frac{2\lambda}{\lambda+1},$$ $$OP_x-OP_z=\frac{2\lambda+1}{\lambda+1}-\frac{3\lambda+1}{\lambda+1} =-\frac{\lambda}{\lambda+1},$$ $$1-OP_x=1-\frac{2\lambda+1}{\lambda+1} =-\frac{\lambda}{\lambda+1}.$$
Thus
$$\vec{OA}\times\vec{OP} =\left(\frac{2\lambda}{\lambda+1},\;-\frac{\lambda}{\lambda+1},\;-\frac{\lambda}{\lambda+1}\right).$$
The squared magnitude required is
$$\bigl|\vec{OA}\times\vec{OP}\bigr|^{2} =\left(\frac{2\lambda}{\lambda+1}\right)^{2} +\left(-\frac{\lambda}{\lambda+1}\right)^{2} +\left(-\frac{\lambda}{\lambda+1}\right)^{2} =\frac{4\lambda^{2}+\lambda^{2}+\lambda^{2}}{(\lambda+1)^{2}} =\frac{6\lambda^{2}}{(\lambda+1)^{2}}.$$
According to the problem, the vectors satisfy
$$\vec{OB}\cdot\vec{OP}-3\bigl|\vec{OA}\times\vec{OP}\bigr|^{2}=6.$$
Substituting the two expressions we just found:
$$\frac{14\lambda+6}{\lambda+1}-3\left(\frac{6\lambda^{2}}{(\lambda+1)^{2}}\right)=6.$$
To clear the denominators, multiply every term by $$(\lambda+1)^{2}$$:
$$\bigl(14\lambda+6\bigr)(\lambda+1)-18\lambda^{2}=6(\lambda+1)^{2}.$$
Expanding each side gives
$$14\lambda^{2}+20\lambda+6-18\lambda^{2}=6\lambda^{2}+12\lambda+6.$$
Combining like terms on the left:
$$-4\lambda^{2}+20\lambda+6 = 6\lambda^{2}+12\lambda+6.$$
Bringing everything to one side:
$$-4\lambda^{2}+20\lambda+6-6\lambda^{2}-12\lambda-6 = 0,$$ $$-10\lambda^{2}+8\lambda = 0.$$
Factoring out $$-2\lambda$$ we get
$$-2\lambda(5\lambda-4)=0.$$
This yields the possibilities $$\lambda=0$$ or $$5\lambda-4=0.$$ Because the ratio must be positive, we reject $$\lambda=0$$ and keep
$$\lambda=\frac{4}{5}=0.8.$$
So, the answer is $$0.8$$.
Let $$\vec{a}$$, $$\vec{b}$$ and $$\vec{c}$$ be three unit vectors such that $$|\vec{a} - \vec{b}|^2 + |\vec{a} - \vec{c}|^2 = 8$$. Then $$|\vec{a} + 2\vec{b}|^2 + |\vec{a} + 2\vec{c}|^2$$ is equal to ___________.
We are given that $$\vec{a},\;\vec{b},\;\vec{c}$$ are unit vectors, that is $$|\vec{a}| = |\vec{b}| = |\vec{c}| = 1.$$
The first relation in the question is
$$|\vec{a}-\vec{b}|^{2} + |\vec{a}-\vec{c}|^{2} = 8.$$
We begin by expanding each squared modulus with the dot‐product formula
$$|\vec{u}-\vec{v}|^{2} = (\vec{u}-\vec{v})\!\cdot\!(\vec{u}-\vec{v}) = |\vec{u}|^{2} + |\vec{v}|^{2} - 2\,\vec{u}\!\cdot\!\vec{v}.$$
Applying this to $$\vec{u}=\vec{a},\;\vec{v}=\vec{b}$$ we get
$$|\vec{a}-\vec{b}|^{2} = |\vec{a}|^{2} + |\vec{b}|^{2} - 2\,\vec{a}\!\cdot\!\vec{b}.$$
Because the vectors are unit, $$|\vec{a}|^{2}=|\vec{b}|^{2}=1,$$ so
$$|\vec{a}-\vec{b}|^{2} = 1 + 1 - 2\,\vec{a}\!\cdot\!\vec{b} = 2\bigl(1-\vec{a}\!\cdot\!\vec{b}\bigr).$$
In the same manner, for $$\vec{u}=\vec{a},\;\vec{v}=\vec{c}$$ we obtain
$$|\vec{a}-\vec{c}|^{2} = 2\bigl(1-\vec{a}\!\cdot\!\vec{c}\bigr).$$
Now we add these two results exactly as the question does:
$$|\vec{a}-\vec{b}|^{2} + |\vec{a}-\vec{c}|^{2} = 2\bigl(1-\vec{a}\!\cdot\!\vec{b}\bigr) + 2\bigl(1-\vec{a}\!\cdot\!\vec{c}\bigr).$$
Combining like terms, this is
$$2\Bigl[\,2 - (\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c})\Bigr].$$
The question tells us that this sum equals $$8,$$ so we equate:
$$2\Bigl[\,2 - (\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c})\Bigr] = 8.$$
Dividing both sides by $$2$$ gives
$$2 - (\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c}) = 4.$$
Transposing to isolate the dot‐product sum, we get
$$(\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c}) = 2 - 4 = -2.$$
So we have established the key relation
$$\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c} = -2.$$
Now we must evaluate $$|\vec{a}+2\vec{b}|^{2} + |\vec{a}+2\vec{c}|^{2}.$$
First expand $$|\vec{a}+2\vec{b}|^{2}$$ with the same dot‐product rule:
$$|\vec{a}+2\vec{b}|^{2} = (\vec{a}+2\vec{b})\!\cdot\!(\vec{a}+2\vec{b}) = |\vec{a}|^{2} + 4|\vec{b}|^{2} + 4\,\vec{a}\!\cdot\!\vec{b}.$$
Because $$|\vec{a}|^{2}=|\vec{b}|^{2}=1,$$ this simplifies to
$$|\vec{a}+2\vec{b}|^{2} = 1 + 4 + 4\,\vec{a}\!\cdot\!\vec{b} = 5 + 4\,\vec{a}\!\cdot\!\vec{b}.$$
Next, do the same for $$|\vec{a}+2\vec{c}|^{2}:$$
$$|\vec{a}+2\vec{c}|^{2} = (\vec{a}+2\vec{c})\!\cdot\!(\vec{a}+2\vec{c}) = |\vec{a}|^{2} + 4|\vec{c}|^{2} + 4\,\vec{a}\!\cdot\!\vec{c}.$$
Again inserting $$|\vec{a}|^{2}=|\vec{c}|^{2}=1,$$ we find
$$|\vec{a}+2\vec{c}|^{2} = 1 + 4 + 4\,\vec{a}\!\cdot\!\vec{c} = 5 + 4\,\vec{a}\!\cdot\!\vec{c}.$$
We now add these two expressions exactly as required:
$$|\vec{a}+2\vec{b}|^{2} + |\vec{a}+2\vec{c}|^{2} = \bigl(5 + 4\,\vec{a}\!\cdot\!\vec{b}\bigr) + \bigl(5 + 4\,\vec{a}\!\cdot\!\vec{c}\bigr).$$
Combining the constant terms and the dot‐product terms separately yields
$$10 + 4\bigl(\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c}\bigr).$$
We have already found that $$\vec{a}\!\cdot\!\vec{b} + \vec{a}\!\cdot\!\vec{c} = -2,$$ so substituting this value gives
$$10 + 4(-2) = 10 - 8 = 2.$$
Thus, the numerical value requested by the question is
$$2.$$
So, the answer is $$2$$.
Let $$\alpha \in R$$ and the three vectors $$\vec{a} = \alpha\hat{i} + \hat{j} + 3\hat{k}$$, $$\vec{b} = 2\hat{i} + \hat{j} - \alpha\hat{k}$$ and $$\vec{c} = \alpha\hat{i} - 2\hat{j} + 3\hat{k}$$. Then the set S = {$$\alpha$$: $$\vec{a}$$, $$\vec{b}$$ and $$\vec{c}$$ are coplanar}
We are asked to find all real numbers $$\alpha$$ for which the three vectors $$\vec{a}= \alpha\hat{i}+\hat{j}+3\hat{k}$$, $$\vec{b}=2\hat{i}+\hat{j}-\alpha\hat{k}$$ and $$\vec{c}= \alpha\hat{i}-2\hat{j}+3\hat{k}$$ are coplanar.
Coplanarity of three vectors is tested by the scalar triple product. The condition is: a set of three vectors is coplanar if and only if the scalar triple product vanishes, that is, we must have
$$\vec{a}\cdot\left( \vec{b}\times\vec{c}\right)=0.$$
Now we compute the cross product $$\vec{b}\times\vec{c}$$ first. Writing the two vectors in component form
$$\vec{b}=(2,\;1,\;-\alpha),\qquad \vec{c}=(\alpha,\;-2,\;3),$$
we use the determinant formula for the cross product:
$$\vec{b}\times\vec{c}= \begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\\[2pt] 2 & 1 & -\alpha\\[2pt] \alpha & -2 & 3 \end{vmatrix}.$$
Expanding this determinant along the first row we obtain
$$ \vec{b}\times\vec{c}= \hat{i}\bigl(1\cdot3-(-\alpha)(-2)\bigr) -\hat{j}\bigl(2\cdot3-(-\alpha)(\alpha)\bigr) +\hat{k}\bigl(2\cdot(-2)-1\cdot\alpha\bigr). $$
Simplifying every bracket step by step:
For the $$\hat{i}$$ component: $$1\cdot3 = 3,\qquad (-\alpha)(-2)=2\alpha,\qquad 3-2\alpha=3-2\alpha.$$
For the $$\hat{j}$$ component: $$2\cdot3 = 6,\qquad (-\alpha)(\alpha)=-\alpha^{2},\qquad 6-(-\alpha^{2})=6+\alpha^{2}.$$
For the $$\hat{k}$$ component: $$2\cdot(-2)=-4,\qquad 1\cdot\alpha=\alpha,\qquad -4-\alpha=-4-\alpha.$$
Putting these results back, we have
$$\vec{b}\times\vec{c}= \bigl(3-2\alpha\bigr)\hat{i}-\bigl(6+\alpha^{2}\bigr)\hat{j}+\bigl(-4-\alpha\bigr)\hat{k}.$$
Thus in component form $$\vec{b}\times\vec{c}=(\,3-2\alpha,\;-\bigl(6+\alpha^{2}\bigr),\;-4-\alpha\,).$$
Next we take the dot product of $$\vec{a}=(\alpha,\,1,\,3)$$ with this result. The dot-product formula is
$$\vec{a}\cdot(\vec{b}\times\vec{c}) = \alpha\,(3-2\alpha)+1\cdot\!\Bigl(-\bigl(6+\alpha^{2}\bigr)\Bigr)+3\cdot(-4-\alpha).$$
We now expand each term carefully:
First term: $$\alpha(3-2\alpha)=3\alpha-2\alpha^{2}.$$
Second term: $$1\cdot\!\Bigl(-\bigl(6+\alpha^{2}\bigr)\Bigr)=-6-\alpha^{2}.$$
Third term: $$3\cdot(-4-\alpha)=-12-3\alpha.$$
Adding all three expressions gives
$$ (3\alpha-2\alpha^{2})+(-6-\alpha^{2})+(-12-3\alpha). $$
Collecting like terms for clarity:
• $$\alpha$$ terms: $$3\alpha-3\alpha=0.$$
• $$\alpha^{2}$$ terms: $$-2\alpha^{2}-\alpha^{2}=-3\alpha^{2}.$$
• Constant terms: $$-6-12=-18.$$
Thus the scalar triple product simplifies to
$$-3\alpha^{2}-18.$$
For coplanarity we set this equal to zero:
$$-3\alpha^{2}-18 = 0.$$
Dividing both sides by $$-3$$ (so that the sign and coefficient become simpler), we get
$$\alpha^{2}+6 = 0.$$
We now solve this quadratic equation. Rearranged, it is
$$\alpha^{2} = -6.$$
But $$\alpha^{2}$$, being a square of a real number, is always non-negative, while the right-hand side $$-6$$ is strictly negative. Hence there is no real value of $$\alpha$$ satisfying this equation.
Therefore the set $$S=\{\alpha\in\mathbb{R}:\vec{a},\vec{b},\vec{c}\text{ are coplanar}\}$$ contains no elements; in other words, $$S$$ is empty.
Hence, the correct answer is Option C.
Let $$\sqrt{3}\hat{i} + \hat{j}$$, $$\hat{i} + \sqrt{3}\hat{j}$$ and $$\beta\hat{i} + (1 - \beta)\hat{j}$$ respectively be the position vectors of the points A, B and C with respect to the origin O. If the distance of C from the bisector of the acute angle between OA and OB is $$\frac{\sqrt{3}}{\sqrt{2}}$$, then the sum of all possible values of $$\beta$$ is:
We have the position vectors of the three points with respect to the origin O
$$\overrightarrow{OA}= \sqrt{3}\,\hat i+\hat j,$$ $$\overrightarrow{OB}= \hat i+\sqrt{3}\,\hat j,$$ $$\overrightarrow{OC}= \beta\,\hat i+(1-\beta)\,\hat j.$$
Writing these vectors in coordinate form, the points are
$$A\equiv(\sqrt3,\,1),$$ $$B\equiv(1,\,\sqrt3),$$ $$C\equiv(\beta,\,1-\beta).$$
First we find the bisector of the acute angle between the rays OA and OB. For two rays whose direction vectors are $$\vec a$$ and $$\vec b,$$ the internal bisector has direction $$\dfrac{\vec a}{|\vec a|}+\dfrac{\vec b}{|\vec b|}\;.$$ Therefore we begin by normalising the two direction vectors.
The magnitudes are
$$|\vec a|=\sqrt{(\sqrt3)^2+1^2}=\sqrt{3+1}=2,$$ $$|\vec b|=\sqrt{1^2+(\sqrt3)^2}=\sqrt{1+3}=2.$$
Hence the unit vectors are
$$\frac{\vec a}{|\vec a|}=\left(\frac{\sqrt3}{2},\;\frac12\right),$$ $$\frac{\vec b}{|\vec b|}=\left(\frac12,\;\frac{\sqrt3}{2}\right).$$
Adding them gives the direction of the acute-angle bisector:
$$\left(\frac{\sqrt3}{2}+\frac12,\;\frac12+\frac{\sqrt3}{2}\right) =\left(\frac{\sqrt3+1}{2},\;\frac{\sqrt3+1}{2}\right).$$
Both coordinates are equal, so the bisector is the straight line through the origin having equation
$$y=x.$$
Now we use the perpendicular-distance formula for a point $$(x_0,y_0)$$ from a straight line $$ax+by+c=0:$$
$$\text{Distance}=\frac{|ax_0+by_0+c|}{\sqrt{a^{2}+b^{2}}}\;.$$
The bisector line $$y=x$$ can be rewritten as $$x-y=0,$$ so $$a=1,\;b=-1,\;c=0.$$ For the point $$C(\beta,\,1-\beta)$$ the perpendicular distance is therefore
$$d=\frac{|1\cdot\beta+(-1)(1-\beta)+0|}{\sqrt{1^{2}+(-1)^{2}}} =\frac{|\,\beta-(1-\beta)\,|}{\sqrt2} =\frac{|\,2\beta-1\,|}{\sqrt2}\;.$$
According to the question this distance equals $$\dfrac{\sqrt3}{\sqrt2},$$ so we equate:
$$\frac{|\,2\beta-1\,|}{\sqrt2}=\frac{\sqrt3}{\sqrt2}.$$
Multiplying by $$\sqrt2$$ on both sides gives
$$|\,2\beta-1\,|=\sqrt3.$$
Removing the absolute value produces two linear equations:
$$2\beta-1=\sqrt3\quad\text{or}\quad 2\beta-1=-\sqrt3.$$
Solving each in turn,
$$\begin{aligned} 2\beta-1&=\sqrt3 &\Longrightarrow&\; 2\beta=1+\sqrt3 &\Longrightarrow&\; \beta=\dfrac{1+\sqrt3}{2},\\[4pt] 2\beta-1&=-\sqrt3 &\Longrightarrow&\; 2\beta=1-\sqrt3 &\Longrightarrow&\; \beta=\dfrac{1-\sqrt3}{2}. \end{aligned}$$
Thus the possible values of $$\beta$$ are
$$\beta_1=\frac{1+\sqrt3}{2},\qquad \beta_2=\frac{1-\sqrt3}{2}.$$
The required sum is therefore
$$\beta_1+\beta_2 =\frac{1+\sqrt3}{2}+\frac{1-\sqrt3}{2} =\frac{1+\sqrt3+1-\sqrt3}{2} =\frac{2}{2}=1.$$
Hence, the correct answer is Option D.
Let $$\vec{a}$$, $$\vec{b}$$ and $$\vec{c}$$ be three unit vectors, out of which vectors $$\vec{b}$$ and $$\vec{c}$$ are non-parallel. If $$\alpha$$ and $$\beta$$ are the angles which vector $$\vec{a}$$ makes with vectors $$\vec{b}$$ and $$\vec{c}$$ respectively and $$\vec{a} \times (\vec{b} \times \vec{c}) = \frac{1}{2}\vec{b}$$, then $$|\alpha - \beta|$$ is equal to:
We are given three unit vectors $$\vec a,\;\vec b,\;\vec c$$ with the information that $$\vec b$$ and $$\vec c$$ are not parallel. The angles that $$\vec a$$ makes with $$\vec b$$ and $$\vec c$$ are denoted by $$\alpha$$ and $$\beta$$ respectively, so by definition of the dot product for unit vectors we have
$$\vec a\cdot\vec b=\cos\alpha\qquad\text{and}\qquad\vec a\cdot\vec c=\cos\beta.$$
We are also told that
$$\vec a\times(\vec b\times\vec c)=\dfrac12\,\vec b.$$
To proceed, we recall the vector triple-product identity. For any vectors $$\vec p,\vec q,\vec r$$ the identity states
$$\vec p\times(\vec q\times\vec r)=\vec q\,(\vec p\cdot\vec r)-\vec r\,(\vec p\cdot\vec q).$$
Applying this identity with $$\vec p=\vec a,\;\vec q=\vec b,\;\vec r=\vec c$$, we obtain
$$\vec a\times(\vec b\times\vec c)=\vec b\,(\vec a\cdot\vec c)-\vec c\,(\vec a\cdot\vec b).$$
Using the shorthand $$\vec a\cdot\vec b=\cos\alpha$$ and $$\vec a\cdot\vec c=\cos\beta$$, the expression becomes
$$\vec a\times(\vec b\times\vec c)=\vec b\,\cos\beta-\vec c\,\cos\alpha.$$
But the problem statement gives the same vector as $$\dfrac12\,\vec b$$. Hence we equate the two results:
$$\vec b\,\cos\beta-\vec c\,\cos\alpha=\dfrac12\,\vec b.$$
Because $$\vec b$$ and $$\vec c$$ are non-parallel, they are linearly independent directions. Therefore the coefficients of $$\vec b$$ and $$\vec c$$ on both sides must match **individually**.
Comparing the $$\vec b$$ components:
$$\cos\beta=\dfrac12.$$
Comparing the $$\vec c$$ components (there is no $$\vec c$$ term on the right-hand side, so its coefficient is zero):
$$-\cos\alpha=0\;\;\Longrightarrow\;\;\cos\alpha=0.$$
Since all three vectors are unit vectors, the cosine values directly yield the angles:
• From $$\cos\alpha=0$$ we find $$\alpha=90^\circ.$$ • From $$\cos\beta=\dfrac12$$ we find $$\beta=60^\circ.$$
Hence the absolute difference between the two angles is
$$|\alpha-\beta|=\bigl|90^\circ-60^\circ\bigr|=30^\circ.$$
Hence, the correct answer is Option 4.
If a unit vector $$\vec{a}$$ makes angles $$\frac{\pi}{3}$$ with $$\hat{i}$$, $$\frac{\pi}{4}$$ with $$\hat{j}$$ and $$\theta \in (0, \pi)$$ with $$\hat{k}$$, then a value of $$\theta$$ is:
For any vector in three-dimensional space, if the angles made with the positive coordinate axes are $$\alpha,\;\beta,\;\gamma,$$ then (direction-cosine identity)
$$\cos^{2}\alpha+\cos^{2}\beta+\cos^{2}\gamma = 1.$$
Here the given angles are $$\alpha=\dfrac{\pi}{3},\;\beta=\dfrac{\pi}{4},\;\gamma=\theta,$$ so we substitute them into the identity.
First we evaluate each cosine:
$$\cos\dfrac{\pi}{3} = \dfrac12 \quad\Longrightarrow\quad \cos^{2}\dfrac{\pi}{3}=\left(\dfrac12\right)^{2}=\dfrac14.$$
$$\cos\dfrac{\pi}{4} = \dfrac{1}{\sqrt2}=\dfrac{\sqrt2}{2}\quad\Longrightarrow\quad \cos^{2}\dfrac{\pi}{4}=\left(\dfrac{\sqrt2}{2}\right)^{2}=\dfrac12.$$
Now we place these values in the identity and solve for $$\cos^{2}\theta$$:
$$\cos^{2}\dfrac{\pi}{3}+\cos^{2}\dfrac{\pi}{4}+\cos^{2}\theta = 1$$
$$\Longrightarrow\quad \dfrac14+\dfrac12+\cos^{2}\theta = 1.$$
We add the fractions on the left:
$$\dfrac14+\dfrac12 = \dfrac14+\dfrac24 = \dfrac34.$$
So we have
$$\dfrac34+\cos^{2}\theta = 1.$$
Subtracting $$\dfrac34$$ from both sides gives
$$\cos^{2}\theta = 1-\dfrac34 = \dfrac14.$$
Taking the square root, we obtain
$$\cos\theta = \pm\dfrac12.$$
Because $$\theta\in(0,\pi),$$ both values are possible in principle, yielding
$$\theta = \dfrac{\pi}{3}\quad\text{or}\quad\theta = \dfrac{2\pi}{3}.$$
Among the options provided, only $$\dfrac{2\pi}{3}$$ appears.
Hence, the correct answer is Option D.
If the volume of parallelepiped formed by the vectors $$\hat{i} + \lambda\hat{j} + \hat{k}$$, $$\hat{j} + \lambda\hat{k}$$ and $$\lambda\hat{i} + \hat{k}$$ is minimum, then $$\lambda$$ is
Let the three vectors forming the parallelepiped be:
$$\vec{a} = \hat{i} + \lambda\hat{j} + \hat{k}$$ $$\vec{b} = 0\hat{i} + \hat{j} + \lambda\hat{k}$$ $$\vec{c} = \lambda\hat{i} + 0\hat{j} + \hat{k}$$
The volume $$V$$ of a parallelepiped formed by three vectors $$\vec{a}, \vec{b}, \vec{c}$$ is given by the magnitude of their scalar triple product:
$$V = | [\vec{a} \cdot (\vec{b} \times \vec{c})] |$$
This can be calculated using the determinant of the matrix formed by their components:
$$V = \begin{vmatrix} 1 & \lambda & 1 \\ 0 & 1 & \lambda \\ \lambda & 0 & 1 \end{vmatrix}$$
Expanding the determinant along the first row:
$$V = 1(1 \cdot 1 - 0 \cdot \lambda) - \lambda(0 \cdot 1 - \lambda \cdot \lambda) + 1(0 \cdot 0 - \lambda \cdot 1)$$ $$V = 1(1) - \lambda(-\lambda^2) + 1(-\lambda)$$ $$V = 1 + \lambda^3 - \lambda$$
Thus, the volume function is $$f(\lambda) = \lambda^3 - \lambda + 1$$.
To find the minimum value, we differentiate $f(\lambda)$ with respect to $$\lambda$$:
$$f'(\lambda) = \frac{d}{d\lambda}(\lambda^3 - \lambda + 1) = 3\lambda^2 - 1$$
Setting the first derivative to zero for critical points:
$$3\lambda^2 - 1 = 0 \implies \lambda^2 = \frac{1}{3} \implies \lambda = \pm \frac{1}{\sqrt{3}}$$
To determine whether these points are a local minimum or maximum, we find the second derivative:
$$f''(\lambda) = 6\lambda$$
- For $$\lambda = \frac{1}{\sqrt{3}}$$:$$f''\left(\frac{1}{\sqrt{3}}\right) = \frac{6}{\sqrt{3}} > 0$$
Since the second derivative is positive, $$\lambda = \frac{1}{\sqrt{3}}$$ is a point of local minimum.
- For $$\lambda = -\frac{1}{\sqrt{3}}$$:$$f''\left(-\frac{1}{\sqrt{3}}\right) = -\frac{6}{\sqrt{3}} < 0$$
Since the second derivative is negative, $$\lambda = -\frac{1}{\sqrt{3}}$$ is a point of local maximum.
The volume is minimum when:
$$\lambda = \frac{1}{\sqrt{3}}$$
Let $$\vec{a} = 2\hat{i} + \lambda_1\hat{j} + 3\hat{k}$$, $$\vec{b} = 4\hat{i} + (3-\lambda_2)\hat{j} + 6\hat{k}$$ and $$\vec{c} = 3\hat{i} + 6\hat{j} + (\lambda_3 - 1)\hat{k}$$ be three vectors such that $$\vec{b} = 2\vec{a}$$ and $$\vec{a}$$ is perpendicular to $$\vec{c}$$. Then a possible value of $$(\lambda_1, \lambda_2, \lambda_3)$$ is:
We have three vectors given by
$$\vec a = 2\hat i + \lambda_1 \hat j + 3\hat k,$$
$$\vec b = 4\hat i + (3-\lambda_2)\hat j + 6\hat k,$$
$$\vec c = 3\hat i + 6\hat j + (\lambda_3 - 1)\hat k.$$
The first condition in the question is $$\vec b = 2\vec a.$$ We therefore equate each corresponding component of the two vectors.
First write the doubled vector $$2\vec a.$$ Multiplying every component of $$\vec a$$ by 2 gives
$$2\vec a = 2\left(2\hat i + \lambda_1 \hat j + 3\hat k\right) = 4\hat i + 2\lambda_1\hat j + 6\hat k.$$
Now set $$\vec b$$ equal to this result:
$$4\hat i + (3-\lambda_2)\hat j + 6\hat k \;=\; 4\hat i + 2\lambda_1\hat j + 6\hat k.$$
By comparing the $$\hat i$$ components we observe $$4 = 4,$$ which is automatically satisfied.
Comparing the $$\hat j$$ components gives the equation
$$3 - \lambda_2 = 2\lambda_1.$$
Solving this equation for $$\lambda_2$$ we get
$$\lambda_2 = 3 - 2\lambda_1.$$
The $$\hat k$$ components give $$6 = 6,$$ which again is always true, so no further information is obtained from that component.
The second condition is that $$\vec a$$ is perpendicular to $$\vec c.$$ Two vectors are perpendicular if and only if their dot product is zero. Using the dot-product formula $$\vec p\!\cdot\!\vec q = p_x q_x + p_y q_y + p_z q_z,$$ we compute
$$\vec a \cdot \vec c \;=\; 2\cdot3 \;+\; \lambda_1\cdot6 \;+\; 3\cdot(\lambda_3 - 1).$$
Carrying out the multiplications gives
$$6 + 6\lambda_1 + 3(\lambda_3 - 1) = 0.$$
Now expand the last term:
$$6 + 6\lambda_1 + 3\lambda_3 - 3 = 0.$$
Combine the constant terms $$6 - 3 = 3$$ to obtain
$$6\lambda_1 + 3 + 3\lambda_3 = 0.$$
Divide every term by 3 to simplify:
$$2\lambda_1 + 1 + \lambda_3 = 0.$$
Isolating $$\lambda_3$$ gives
$$\lambda_3 = -1 - 2\lambda_1.$$
We now have two relations connecting the three unknowns:
$$\lambda_2 = 3 - 2\lambda_1,$$
$$\lambda_3 = -1 - 2\lambda_1.$$
Any triple $$(\lambda_1,\lambda_2,\lambda_3)$$ that satisfies both relations will meet the required conditions. We check the answer options one by one.
Option A proposes $$\left(-\dfrac12,\;4,\;0\right).$$ Substituting $$\lambda_1 = -\dfrac12$$ into the first relation gives
$$\lambda_2 = 3 - 2\left(-\dfrac12\right) = 3 + 1 = 4,$$
which matches the listed $$\lambda_2 = 4.$$ Substituting the same $$\lambda_1$$ into the second relation gives
$$\lambda_3 = -1 - 2\left(-\dfrac12\right) = -1 + 1 = 0,$$
which also matches the listed $$\lambda_3 = 0.$$ Therefore Option A satisfies both equations.
Option B lists $$(1,\,5,\,1).$$ With $$\lambda_1 = 1,$$ the first relation requires $$\lambda_2 = 3 - 2(1) = 1,$$ but the option gives $$\lambda_2 = 5,$$ so it fails.
Option C lists $$\left(\dfrac12,\,4,\,-2\right).$$ For $$\lambda_1 = \dfrac12,$$ the first relation yields $$\lambda_2 = 3 - 2\left(\dfrac12\right) = 2,$$ whereas the option has $$\lambda_2 = 4,$$ so this also fails.
Option D lists $$(1,\,3,\,1).$$ Again setting $$\lambda_1 = 1$$ forces $$\lambda_2 = 1,$$ but the option gives $$\lambda_2 = 3,$$ so it is incorrect.
Only Option A meets both derived conditions.
Hence, the correct answer is Option A.
Let $$\vec{a} = 3\hat{i} + 2\hat{j} + x\hat{k}$$ and $$\vec{b} = \hat{i} - \hat{j} + \hat{k}$$, for some real $$x$$. Then the condition for $$\vec{a} \times \vec{b} = r$$ to follow is:
We have the two vectors
$$\vec a = 3\hat i + 2\hat j + x\hat k ,\qquad \vec b = \hat i - \hat j + \hat k ,$$
where $$x$$ is any real number. The question talks about $$\vec a \times \vec b = r$$. Because the left-hand side of this equation is a vector while $$r$$ is written as a scalar, the only way the statement can make sense is to interpret $$r$$ as the magnitude of the cross product:
$$r = \bigl\lvert\,\vec a \times \vec b\,\bigr\rvert.$$
To obtain the magnitude we must first find the cross product itself. Using the determinant form
$$ \vec a \times \vec b \;=\; \begin{vmatrix} \hat i & \hat j & \hat k\\ 3 & 2 & x\\ 1 & -1 & 1 \end{vmatrix}, $$
we expand component by component:
$$ \vec a \times \vec b = \hat i\,(2\cdot1 \;-\; x\cdot(-1)) \;-\; \hat j\,(3\cdot1 \;-\; x\cdot1) \;+\; \hat k\,(3\cdot(-1) \;-\; 2\cdot1). $$
Now we simplify each bracket:
$$ \begin{aligned} \hat i &:& 2\cdot1 - x\cdot(-1) &= 2 + x,\\[4pt] -\hat j &:& 3\cdot1 - x\cdot1 &= 3 - x,\\[4pt] \hat k &:& 3\cdot(-1) - 2\cdot1 &= -3 - 2 = -5. \end{aligned} $$
So the cross-product vector itself is
$$ \vec a \times \vec b = (\,2 + x\,)\,\hat i \;-\;(3 - x)\,\hat j \;-\;5\,\hat k. $$
We now calculate its magnitude. For any vector $$P\hat i + Q\hat j + R\hat k$$ the magnitude formula is
$$ |\vec P| = \sqrt{P^{2} + Q^{2} + R^{2}}. $$
Here $$P = 2 + x,\; Q = -(3 - x),\; R = -5$$, so
$$ \bigl\lvert\,\vec a \times \vec b\,\bigr\rvert = \sqrt{(2 + x)^{2} + \bigl(-(3 - x)\bigr)^{2} + (-5)^{2}}. $$
We expand each square one by one:
$$ \begin{aligned} (2 + x)^{2} &= x^{2} + 4x + 4,\\[4pt] \bigl(-(3 - x)\bigr)^{2} &= (3 - x)^{2} = x^{2} - 6x + 9,\\[4pt] (-5)^{2} &= 25. \end{aligned} $$
Adding these three expressions gives
$$ x^{2} + 4x + 4 \;+\; x^{2} - 6x + 9 \;+\; 25 \;=\; 2x^{2} - 2x + 38. $$
Hence
$$ r = \bigl\lvert\,\vec a \times \vec b\,\bigr\rvert = \sqrt{\,2x^{2} - 2x + 38\,}. $$
To understand what numerical values $$r$$ can take, we must analyze the quadratic inside the square root:
$$ g(x) = 2x^{2} - 2x + 38. $$
This is an upward-opening parabola whose minimum value occurs at
$$ x = -\frac{b}{2a} = -\frac{-2}{2\cdot2} = \frac12. $$
Substituting $$x = \frac12$$ into $$g(x)$$ we obtain
$$ g\!\Bigl(\frac12\Bigr) = 2\!\left(\frac12\right)^{2} - 2\!\left(\frac12\right) + 38 = 2\!\left(\frac14\right) - 1 + 38 = \frac12 - 1 + 38 = \frac{75}{2}. $$
Therefore the smallest value that $$2x^{2} - 2x + 38$$ can take is $$\dfrac{75}{2}$$, and for all other values of $$x$$ the expression is larger. Since there is no upper bound on the quadratic (it grows to $$+\infty$$ as $$x \to \pm\infty$$), the set of possible values is
$$ [\,\tfrac{75}{2},\;\infty). $$
Taking square roots gives the complete range of $$r$$:
$$ r \in \Bigl[\,\sqrt{\tfrac{75}{2}},\;\infty\Bigr). $$
We simplify the radical once more:
$$ \sqrt{\tfrac{75}{2}} = \sqrt{\tfrac{25\cdot3}{2}} = 5\sqrt{\tfrac32}. $$
Thus the necessary and sufficient condition is
$$ r \;\ge\; 5\sqrt{\tfrac32}. $$
Among the printed alternatives, only Option B expresses exactly this inequality.
Hence, the correct answer is Option B.
Let $$\vec{a} = \hat{i} + 2\hat{j} + 4\hat{k}$$, $$\vec{b} = \hat{i} + \lambda\hat{j} + 4\hat{k}$$ and $$\vec{c} = 2\hat{i} + 4\hat{j} + (\lambda^2 - 1)\hat{k}$$ be coplanar vectors. Then the non-zero vector $$\vec{a} \times \vec{c}$$ is:
We have the three vectors
$$\vec a = \hat i + 2\hat j + 4\hat k,\qquad \vec b = \hat i + \lambda\hat j + 4\hat k,\qquad \vec c = 2\hat i + 4\hat j + (\lambda^2-1)\hat k.$$
Since the vectors are given to be coplanar, their scalar triple product must be zero. The scalar triple product formula is
$$\vec a\cdot(\vec b\times\vec c)=0.$$
First we compute the cross product $$\vec b\times\vec c.$$ Using the determinant form of the cross product,
$$ \vec b\times\vec c=\begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & \lambda & 4\\ 2 & 4 & \lambda^2-1 \end{vmatrix}. $$
Expanding the determinant along the first row:
$$ \vec b\times\vec c = \hat i\bigl[\lambda(\lambda^2-1)-4\cdot4\bigr] -\hat j\bigl[1(\lambda^2-1)-4\cdot2\bigr] +\hat k\bigl[1\cdot4-\lambda\cdot2\bigr]. $$
Now we simplify each component.
$$\lambda(\lambda^2-1)-16=\lambda^3-\lambda-16,$$ $$1(\lambda^2-1)-8=\lambda^2-1-8=\lambda^2-9,$$ $$4-2\lambda.$$
Thus
$$\vec b\times\vec c=(\lambda^3-\lambda-16)\hat i-(\lambda^2-9)\hat j+(4-2\lambda)\hat k.$$
Next we take the dot product of this with $$\vec a=1\hat i+2\hat j+4\hat k.$$
$$ \vec a\cdot(\vec b\times\vec c) =1\cdot(\lambda^3-\lambda-16) +2\cdot\bigl[-(\lambda^2-9)\bigr] +4\cdot(4-2\lambda). $$
Carrying out the multiplication term by term:
$$1(\lambda^3-\lambda-16)=\lambda^3-\lambda-16,$$ $$2\bigl[-(\lambda^2-9)\bigr]=-2\lambda^2+18,$$ $$4(4-2\lambda)=16-8\lambda.$$
Adding all these contributions gives
$$\lambda^3-\lambda-16-2\lambda^2+18+16-8\lambda =\lambda^3-2\lambda^2-9\lambda+18.$$
For coplanarity this expression must be zero, so
$$\lambda^3-2\lambda^2-9\lambda+18=0.$$
We factor the cubic. Trying simple factors, $$\lambda=3$$ satisfies the equation, so we divide by $$(\lambda-3)$$:
$$\lambda^3-2\lambda^2-9\lambda+18=(\lambda-3)(\lambda^2+\lambda-6).$$
Further factoring $$\lambda^2+\lambda-6=(\lambda+3)(\lambda-2).$$
Hence
$$\lambda^3-2\lambda^2-9\lambda+18=(\lambda-3)(\lambda+3)(\lambda-2)=0,$$
giving three possible values
$$\lambda=3,\qquad\lambda=-3,\qquad\lambda=2.$$
We now turn to the required cross product $$\vec a\times\vec c.$$ Again we use the determinant:
$$ \vec a\times\vec c=\begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & 2 & 4\\ 2 & 4 & \lambda^2-1 \end{vmatrix}. $$
Expanding along the first row:
$$ \vec a\times\vec c = \hat i\bigl[2(\lambda^2-1)-4\cdot4\bigr] -\hat j\bigl[1(\lambda^2-1)-4\cdot2\bigr] +\hat k\bigl[1\cdot4-2\cdot2\bigr]. $$
We simplify each bracket:
$$2(\lambda^2-1)-16=2\lambda^2-2-16=2\lambda^2-18,$$ $$1(\lambda^2-1)-8=\lambda^2-9,$$ $$4-4=0.$$
Therefore
$$\vec a\times\vec c=(2\lambda^2-18)\hat i-(\lambda^2-9)\hat j+0\hat k.$$
Factoring out the common term $$(\lambda^2-9)$$:
$$\vec a\times\vec c=(\lambda^2-9)\bigl(2\hat i-\hat j\bigr).$$
This result shows that if $$\lambda^2-9=0$$ (i.e., $$\lambda=\pm3$$) the cross product vanishes, but the question asks for a non-zero vector. Hence we must choose the remaining admissible value $$\lambda=2.$$
Substituting $$\lambda=2$$ gives
$$\lambda^2-9=4-9=-5,$$
and hence
$$\vec a\times\vec c=-5\,(2\hat i-\hat j)=-10\hat i+5\hat j.$$
This matches the vector in Option D.
Hence, the correct answer is Option D.
Let $$\vec{a} = \hat{i} + \hat{j} + \sqrt{2}\hat{k}$$, $$\vec{b} = b_1\hat{i} + b_2\hat{j} + \sqrt{2}\hat{k}$$ and $$\vec{c} = 5\hat{i} + \hat{j} + \sqrt{2}\hat{k}$$ be three vectors such that the projection vector of $$\vec{b}$$ on $$\vec{a}$$ is $$|\vec{a}|$$. If $$\vec{a} + \vec{b}$$ is perpendicular to $$\vec{c}$$, then $$|\vec{b}|$$ is equal to:
We have the three vectors
$$\vec a=\hat i+\hat j+\sqrt2\,\hat k,\qquad \vec b=b_1\hat i+b_2\hat j+\sqrt2\,\hat k,\qquad \vec c=5\hat i+\hat j+\sqrt2\,\hat k.$$
The statement “the projection of $$\vec b$$ on $$\vec a$$ is $$|\vec a|$$” refers to the scalar projection. The scalar projection formula is
$$\text{comp}_{\vec a}\vec b=\frac{\vec a\cdot\vec b}{|\vec a|}.$$
Setting this equal to $$|\vec a|$$ we obtain
$$\frac{\vec a\cdot\vec b}{|\vec a|}=|\vec a|.$$
Multiplying by $$|\vec a|$$ gives
$$\vec a\cdot\vec b=|\vec a|^{\,2}.$$
First we compute $$|\vec a|^{\,2}$$:
$$|\vec a|^{\,2}=1^{2}+1^{2}+(\sqrt2)^{2}=1+1+2=4,$$
so $$|\vec a|=2.$$
Now we evaluate $$\vec a\cdot\vec b$$:
$$\vec a\cdot\vec b=(1)(b_1)+(1)(b_2)+(\sqrt2)(\sqrt2)=b_1+b_2+2.$$
The equality $$\vec a\cdot\vec b=4$$ therefore becomes
$$b_1+b_2+2=4\qquad\Longrightarrow\qquad b_1+b_2=2.$$
The second condition says that $$\vec a+\vec b$$ is perpendicular to $$\vec c$$. For perpendicular vectors the dot product is zero, so
$$(\vec a+\vec b)\cdot\vec c=0.$$
First compute $$\vec a+\vec b$$:
$$\vec a+\vec b=(1+b_1)\hat i+(1+b_2)\hat j+(2\sqrt2)\hat k.$$
Now take its dot product with $$\vec c$$:
$$$ (\vec a+\vec b)\cdot\vec c= (1+b_1)(5)+(1+b_2)(1)+(2\sqrt2)(\sqrt2). $$$
Since $$(2\sqrt2)(\sqrt2)=2\cdot2=4,$$ we have
$$5(1+b_1)+1(1+b_2)+4=0.$$
Expanding and collecting terms gives
$$5+5b_1+1+b_2+4=0\quad\Longrightarrow\quad5b_1+b_2+10=0.$$
Thus
$$5b_1+b_2=-10.$$
We now solve the simultaneous linear equations
$$\begin{cases} b_1+b_2=2,\\ 5b_1+b_2=-10. \end{cases}$$
Subtracting the first from the second eliminates $$b_2$$:
$$4b_1=-12\quad\Longrightarrow\quad b_1=-3.$$
Substituting $$b_1=-3$$ into $$b_1+b_2=2$$ gives
$$-3+b_2=2\quad\Longrightarrow\quad b_2=5.$$
Hence
$$\vec b=-3\hat i+5\hat j+\sqrt2\,\hat k.$$
Finally, we find $$|\vec b|$$:
$$|\vec b|^{\,2}=(-3)^{2}+5^{2}+(\sqrt2)^{2}=9+25+2=36,$$
so
$$|\vec b|=6.$$
Hence, the correct answer is Option C.
Let $$\vec{a} = \hat{i} - \hat{j}$$, $$\vec{b} = \hat{i} + \hat{j} + \hat{k}$$ and $$\vec{c}$$ be a vector such that $$\vec{a} \times \vec{c} + \vec{b} = \vec{0}$$ and $$\vec{a} \cdot \vec{c} = 4$$, then $$|\vec{c}|^2$$ is equal to:
We have the vectors $$\vec a=\hat i-\hat j$$ and $$\vec b=\hat i+\hat j+\hat k$$. Let us assume the unknown vector $$\vec c$$ to have Cartesian components, so we write $$\vec c=x\hat i+y\hat j+z\hat k$$ where $$x,\;y,\;z$$ are real numbers to be determined.
The first given condition is $$\vec a\times\vec c+\vec b=\vec0$$. Re-writing, we obtain $$\vec a\times\vec c=-\vec b$$. In order to use this relation, we must first compute the cross product $$\vec a\times\vec c$$.
By the determinant formula for a cross product, namely $$ \vec p\times\vec q= \begin{vmatrix} \hat i & \hat j & \hat k\\ p_x & p_y & p_z\\ q_x & q_y & q_z \end{vmatrix}, $$ we substitute $$\vec p=\vec a=(1,-1,0)$$ and $$\vec q=\vec c=(x,y,z)$$ to get
$$ \vec a\times\vec c= \begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & -1 & 0\\ x & y & z \end{vmatrix} =\hat i\bigl((-1)z-0\cdot y\bigr)-\hat j\bigl(1\cdot z-0\cdot x\bigr)+\hat k\bigl(1\cdot y-(-1)\cdot x\bigr). $$
Simplifying each component separately,
$$ \vec a\times\vec c=(-z)\hat i-\,z\hat j+(y+x)\hat k. $$
According to the relationship $$\vec a\times\vec c=-\vec b$$, we must have
$$ (-z)\hat i-\,z\hat j+(x+y)\hat k=(-1)\hat i-1\hat j-1\hat k. $$
Equating the coefficients of the corresponding unit vectors, we obtain three linear equations:
For the $$\hat i$$ component: $$-z=-1\;\Longrightarrow\;z=1.$$
For the $$\hat j$$ component: $$-z=-1\;\Longrightarrow\;z=1,$$ which is consistent with the previous result.
For the $$\hat k$$ component: $$x+y=-1.$$
Thus we already know $$z=1$$ and have the relation $$x+y=-1.$$(1)
The second given condition is the dot-product equation $$\vec a\cdot\vec c=4$$. Using the standard dot product formula $$\vec p\cdot\vec q=p_xq_x+p_yq_y+p_zq_z$$, we find
$$ \vec a\cdot\vec c=(1)(x)+(-1)(y)+(0)(z)=x-y. $$
Hence the dot-product condition provides
$$ x-y=4.\;(2) $$
Now we solve the simultaneous linear equations $$ \begin{cases} x+y=-1 \quad\text{(from (1))}\\ x-y=4 \quad\text{(from (2))} \end{cases} $$
Adding the two equations gives $$ 2x=3\;\Longrightarrow\;x=\dfrac{3}{2}. $$
Substituting $$x=\dfrac{3}{2}$$ into $$x+y=-1$$ yields $$ \dfrac{3}{2}+y=-1\;\Longrightarrow\;y=-1-\dfrac{3}{2}=-\dfrac{5}{2}. $$
We already have $$z=1$$, so the complete vector $$\vec c$$ is
$$ \vec c=\dfrac{3}{2}\hat i-\dfrac{5}{2}\hat j+1\hat k. $$
Finally, we must find $$|\vec c|^2$$. Using the magnitude-squared formula $$|\vec c|^2=x^2+y^2+z^2,$$ we substitute our values:
$$ |\vec c|^2=\left(\dfrac{3}{2}\right)^2+\left(-\dfrac{5}{2}\right)^2+(1)^2 =\dfrac{9}{4}+\dfrac{25}{4}+1. $$
Adding the fractions first, $$\dfrac{9}{4}+\dfrac{25}{4}=\dfrac{34}{4}.$$ Converting $$1$$ to quarters, we have $$1=\dfrac{4}{4}.$$ Therefore,
$$ |\vec c|^2=\dfrac{34}{4}+\dfrac{4}{4}=\dfrac{38}{4}=\dfrac{19}{2}. $$
Hence, the correct answer is Option A.
Let $$\vec{\alpha} = 3\hat{i} + \hat{j}$$ and $$\vec{\beta} = 2\hat{i} - \hat{j} + 3\hat{k}$$. If $$\vec{\beta} = \vec{\beta_1} - \vec{\beta_2}$$, where $$\vec{\beta_1}$$ is parallel to $$\vec{\alpha}$$ and $$\vec{\beta_2}$$ is perpendicular to $$\vec{\alpha}$$, then $$\vec{\beta_1} \times \vec{\beta_2}$$ is equal to:
We are given $$\vec{\alpha}=3\hat i+\hat j$$ and $$\vec{\beta}=2\hat i-\hat j+3\hat k$$. We have to split $$\vec{\beta}$$ into two parts in such a way that $$\vec{\beta_1}$$ is parallel to $$\vec{\alpha}$$ while $$\vec{\beta_2}$$ is perpendicular to $$\vec{\alpha}$$, and the relation between them is $$\vec{\beta}= \vec{\beta_1}-\vec{\beta_2}$$.
Because $$\vec{\beta_1}$$ is parallel to $$\vec{\alpha}$$, we can write it as a scalar multiple of $$\vec{\alpha}$$. So we set $$\vec{\beta_1}= \lambda \vec{\alpha}= \lambda(3\hat i+\hat j)= (3\lambda)\hat i+(\lambda)\hat j+0\hat k.$$ Here $$\lambda$$ is a real number that we will determine.
Re-arranging the given relation $$\vec{\beta}= \vec{\beta_1}-\vec{\beta_2}$$, we get $$\vec{\beta_2}= \vec{\beta_1}-\vec{\beta}.$$ Substituting $$\vec{\beta_1}=(3\lambda)\hat i+\lambda\hat j$$ and $$\vec{\beta}=2\hat i-\hat j+3\hat k$$, we obtain $$\vec{\beta_2}= (3\lambda-2)\hat i+(\lambda+1)\hat j-3\hat k.$$ So, in component form, $$\vec{\beta_2}=(3\lambda-2,\;\lambda+1,\;-3).$$
The vector $$\vec{\beta_2}$$ is perpendicular to $$\vec{\alpha}$$. For perpendicular vectors, the scalar (dot) product is zero. Using the dot-product formula $$\vec{u}\cdot\vec{v}=u_xv_x+u_yv_y+u_zv_z,$$ we write $$\vec{\alpha}\cdot\vec{\beta_2}=0.$$ Now $$\vec{\alpha}=(3,1,0)$$ and $$\vec{\beta_2}=(3\lambda-2,\;\lambda+1,\;-3).$$ Therefore $$3(3\lambda-2)+1(\lambda+1)+0(-3)=0.$$ Carrying out the multiplication and addition, $$9\lambda-6+\lambda+1=0,$$ $$10\lambda-5=0.$$ Solving for $$\lambda$$, we get $$\lambda=\frac{5}{10}=\frac12.$$ So $$\vec{\beta_1}= \frac12(3\hat i+\hat j)=\frac32\hat i+\frac12\hat j,$$ and $$\vec{\beta_2}= (3\cdot\frac12-2)\hat i+\Bigl(\frac12+1\Bigr)\hat j-3\hat k =\Bigl(\frac32-2\Bigr)\hat i+\frac32\hat j-3\hat k =-\frac12\hat i+\frac32\hat j-3\hat k.$
Now we compute the cross product $$\vec{\beta_1}\times\vec{\beta_2}$$. The cross product formula in components is $$\vec{a}\times\vec{b}=(a_yb_z-a_zb_y)\hat{i}+(a_zb_x-a_xb_z)\hat{j}+(a_xb_y-a_yb_x)\hat{k}.$$ Taking $$\vec{a}=\vec{\beta_1}=\bigl(\frac{3}{2},\;\frac{1}{2},\;0\bigr)$$ and $$\vec{b}=\vec{\beta_2}=\bigl(-\frac{1}{2},\;\frac{3}{2},\;-3\bigr),$$ we calculate:
$$$\begin{aligned} \vec{\beta_1}\times\vec{\beta_2}&=\Bigl(\frac{1}{2}\cdot(-3)-0\cdot\frac{3}{2}\Bigr)\hat{i} +\Bigl(0\cdot\bigl(-\frac{1}{2}\bigr)-\frac{3}{2}\cdot(-3)\Bigr)\hat{j} +\Bigl(\frac{3}{2}\cdot\frac{3}{2}-\frac{1}{2}\cdot\bigl(-\frac{1}{2}\bigr)\Bigr)\hat{k} \\ &=\Bigl(-\frac{3}{2}\Bigr)\hat{i} +\Bigl(0+\frac{9}{2}\Bigr)\hat{j} +\Bigl(\frac{9}{4}+\frac{1}{4}\Bigr)\hat{k} \\ &=-\frac{3}{2}\hat{i}+\frac{9}{2}\hat{j}+\frac{10}{4}\hat{k} \\ &=-\frac{3}{2}\hat{i}+\frac{9}{2}\hat{j}+\frac{5}{2}\hat{k}. \end{aligned}$$$ Factorising a common $$\frac{1}{2}$$, we get $$\vec{\beta_1}\times\vec{\beta_2}=\frac{1}{2}\bigl(-3\hat{i}+9\hat{j}+5\hat{k}\bigr).$$
Comparing with the given options, this matches exactly with Option A.
Hence, the correct answer is Option A.
Let $$\vec{\alpha} = (\lambda - 2)\vec{a} + \vec{b}$$ and $$\vec{\beta} = (4\lambda - 2)\vec{a} + 3\vec{b}$$, be two given vectors where vectors $$\vec{a}$$ and $$\vec{b}$$ are non-collinear. The value of $$\lambda$$ for which vectors $$\vec{\alpha}$$ and $$\vec{\beta}$$ are collinear, is:
We have two vectors defined in terms of the non-collinear base vectors $$\vec a$$ and $$\vec b$$:
$$\vec\alpha = (\lambda-2)\vec a + \vec b$$
$$\vec\beta = (4\lambda-2)\vec a + 3\vec b$$
Because $$\vec a$$ and $$\vec b$$ are not collinear, they form an independent pair. Any vector written as a linear combination of them is uniquely determined by its two scalar coefficients. Two such vectors will be collinear if and only if their respective coefficients are in the same ratio. In other words, for some real number $$k$$ we must have
$$\vec\alpha = k\,\vec\beta.$$
Equating the coefficients of $$\vec a$$ and $$\vec b$$ separately, we obtain
$$\dfrac{\text{coefficient of }\vec a\text{ in }\vec\alpha}{\text{coefficient of }\vec a\text{ in }\vec\beta} \;=\; \dfrac{\text{coefficient of }\vec b\text{ in }\vec\alpha}{\text{coefficient of }\vec b\text{ in }\vec\beta}.$$
Explicitly substituting the given coefficients, this condition becomes
$$\frac{\lambda-2}{4\lambda-2} = \frac{1}{3}.$$
Now we solve step by step. First cross-multiply:
$$3(\lambda-2) = 1\,(4\lambda-2).$$
Expand both sides:
$$3\lambda - 6 = 4\lambda - 2.$$
Bring all terms to one side to isolate $$\lambda$$:
$$3\lambda - 6 - 4\lambda + 2 = 0.$$
Combine like terms:
$$(3\lambda - 4\lambda) + (-6 + 2) = 0,$$
$$-\,\lambda - 4 = 0.$$
Multiply by $$-1$$ to make the coefficient positive:
$$\lambda + 4 = 0.$$
Therefore,
$$\lambda = -4.$$
Hence, the correct answer is Option A.
The magnitude of the projection of the vector $$2\hat{i} + 3\hat{j} + \hat{k}$$ on the vector perpendicular to the plane containing the vectors $$\hat{i} + \hat{j} + \hat{k}$$ and $$\hat{i} + 2\hat{j} + 3\hat{k}$$, is:
We have the vector whose projection is required, $$\vec{A}=2\hat{i}+3\hat{j}+\hat{k}.$$ The projection is to be taken on the vector that is perpendicular to the plane containing the two given vectors $$\vec{B}=\hat{i}+\hat{j}+\hat{k} \text{ and } \vec{C}=\hat{i}+2\hat{j}+3\hat{k}.$$
A vector perpendicular to a plane containing two non-parallel vectors is obtained through their cross product. Stating the formula first, for any vectors $$\vec{u}=(u_1,u_2,u_3)$$ and $$\vec{v}=(v_1,v_2,v_3),$$ the cross product is
$$\vec{u}\times\vec{v}= \begin{vmatrix} \hat{i}&\hat{j}&\hat{k}\\ u_1&u_2&u_3\\ v_1&v_2&v_3 \end{vmatrix}.$$
Now we compute $$\vec{N}=\vec{B}\times\vec{C}:$$
$$ \vec{N}= \begin{vmatrix} \hat{i}&\hat{j}&\hat{k}\\ 1&1&1\\ 1&2&3 \end{vmatrix} = \hat{i}(1\cdot3-1\cdot2) - \hat{j}(1\cdot3-1\cdot1) + \hat{k}(1\cdot2-1\cdot1). $$
Simplifying each component, we get
$$ \vec{N}= \hat{i}(3-2) - \hat{j}(3-1) + \hat{k}(2-1)= \hat{i} - 2\hat{j} + \hat{k}. $$
So the perpendicular (normal) vector is $$\vec{N}= \hat{i}-2\hat{j}+\hat{k}.$$
To find the magnitude of the projection of $$\vec{A}$$ on $$\vec{N},$$ we state the projection magnitude formula: for vectors $$\vec{u}$$ and $$\vec{v},$$ the magnitude of the projection of $$\vec{u}$$ on $$\vec{v}$$ is
$$ \left|\text{proj}_{\vec{v}}\vec{u}\right| = \frac{|\vec{u}\cdot\vec{v}|}{\|\vec{v}\|}. $$
We therefore need $$\vec{A}\cdot\vec{N}$$ and $$\|\vec{N}\|.$$
First, the dot product:
$$ \vec{A}\cdot\vec{N} = (2)(1) + (3)(-2) + (1)(1) = 2 - 6 + 1 = -3. $$
The absolute value is $$|\vec{A}\cdot\vec{N}| = |-3| = 3.$$
Next, the magnitude of $$\vec{N}$$ is
$$ \|\vec{N}\| = \sqrt{1^2 + (-2)^2 + 1^2} = \sqrt{1 + 4 + 1} = \sqrt{6}. $$
Substituting these results in the projection formula gives
$$ \left|\text{proj}_{\vec{N}}\vec{A}\right| = \frac{3}{\sqrt{6}}. $$
We rationalise the denominator to make comparison with the options easier:
$$ \frac{3}{\sqrt{6}} = \frac{3}{\sqrt{6}}\cdot\frac{\sqrt{6}}{\sqrt{6}} = \frac{3\sqrt{6}}{6} = \frac{\sqrt{6}}{2}. $$
An equivalent way to write $$\frac{3}{\sqrt{6}}$$ is $$\sqrt{\frac{3}{2}}$$ because
$$ \sqrt{\frac{3}{2}}=\sqrt{\frac{9}{6}}=\frac{3}{\sqrt{6}}. $$
Among the given choices, this matches option B, which is $$\sqrt{\frac{3}{2}}.$$
Hence, the correct answer is Option 2.
The sum of the distinct real values of $$\mu$$ for which the vectors $$\mu\hat{i} + \hat{j} + \hat{k}$$, $$\hat{i} + \mu\hat{j} + \hat{k}$$, $$\hat{i} + \hat{j} + \mu\hat{k}$$ are co-planar, is
Let $$\vec{a} = 3\hat{i} + 2\hat{j} + 2\hat{k}$$ and $$\vec{b} = \hat{i} + 2\hat{j} - 2\hat{k}$$ be two vectors. If a vector perpendicular to both the vectors $$\vec{a} + \vec{b}$$ and $$\vec{a} - \vec{b}$$ has the magnitude 12 then one such vector is:
Given the vectors:
$$\vec{a} = 3\hat{i} + 2\hat{j} + 2\hat{k}$$ $$\vec{b} = \hat{i} + 2\hat{j} - 2\hat{k}$$
First, we find the sum and difference of the vectors:
- Addition: $$\vec{a} + \vec{b} = (3+1)\hat{i} + (2+2)\hat{j} + (2-2)\hat{k} = 4\hat{i} + 4\hat{j} + 0\hat{k}$$
- Subtraction: $$\vec{a} - \vec{b} = (3-1)\hat{i} + (2-2)\hat{j} + (2-(-2))\hat{k} = 2\hat{i} + 0\hat{j} + 4\hat{k}$$
A vector perpendicular to both $$(\vec{a} + \vec{b})$$ and $$(\vec{a} - \vec{b})$$ is given by their cross product. Let $$\vec{u} = \vec{a} + \vec{b}$$ and $$\vec{v} = \vec{a} - \vec{b}$$:
$$\vec{u} \times \vec{v} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 4 & 4 & 0 \\ 2 & 0 & 4 \end{vmatrix}$$
Expanding the determinant:
$$\vec{u} \times \vec{v} = \hat{i}(16 - 0) - \hat{j}(16 - 0) + \hat{k}(0 - 8)$$ $$\vec{u} \times \vec{v} = 16\hat{i} - 16\hat{j} - 8\hat{k}$$
The magnitude of this cross product is:
$$|\vec{u} \times \vec{v}| = \sqrt{16^2 + (-16)^2 + (-8)^2}$$ $$|\vec{u} \times \vec{v}| = \sqrt{256 + 256 + 64} = \sqrt{576} = 24$$
The question requires a vector with a magnitude of 12. Since our current vector has a magnitude of 24, we multiply the vector by $$\frac{12}{24}$$ (or $$\frac{1}{2}$$):
$$\text{Required Vector} = \frac{1}{2}(16\hat{i} - 16\hat{j} - 8\hat{k}) = 8\hat{i} - 8\hat{j} - 4\hat{k}$$
Factoring out a 4 to match the options provided:
$$8\hat{i} - 8\hat{j} - 4\hat{k} = 4(2\hat{i} - 2\hat{j} - \hat{k})$$
This matches Option B.
Let $$\vec{a} = \hat{i} + \hat{j} + \hat{k}$$, $$\vec{c} = \hat{j} - \hat{k}$$ and a vector $$\vec{b}$$ be such that $$\vec{a} \times \vec{b} = \vec{c}$$ and $$\vec{a} \cdot \vec{b} = 3$$. Then $$|\vec{b}|$$ equals:
We have the three-dimensional vectors
$$\vec a = \hat i + \hat j + \hat k,$$
$$\vec c = \hat j - \hat k,$$
and an unknown vector $$\vec b = b_x\hat i + b_y\hat j + b_z\hat k$$ which must satisfy two simultaneous conditions:
$$\vec a \times \vec b = \vec c \qquad\text{and}\qquad \vec a \cdot \vec b = 3.$$
We attack the cross-product equation first. Using the determinant form of the vector product
$$\vec a \times \vec b = \begin{vmatrix} \hat i & \hat j & \hat k \\[4pt] 1 & 1 & 1 \\[4pt] b_x & b_y & b_z \end{vmatrix},$$
we obtain, expanding along the first row,
$$\vec a \times \vec b = (1\cdot b_z - 1\cdot b_y)\,\hat i - (1\cdot b_z - 1\cdot b_x)\,\hat j + (1\cdot b_y - 1\cdot b_x)\,\hat k.$$
Simplifying each component gives
$$\vec a \times \vec b = (\,b_z - b_y\,)\,\hat i + (\,b_x - b_z\,)\,\hat j + (\,b_y - b_x\,)\,\hat k.$$
This must equal $$\vec c = 0\,\hat i + 1\,\hat j - 1\,\hat k,$$ so by equating corresponding components we arrive at the three scalar equations
$$$b_z - b_y = 0, \tag{1}$$$
$$$b_x - b_z = 1, \tag{2}$$$
$$$b_y - b_x = -1. \tag{3}$$$
From equation (1) we have
$$$b_z = b_y. \tag{4}$$$
Substituting (4) into equation (2) yields
$$$b_x = 1 + b_z. \tag{5}$$$
Equation (3) can be rearranged to
$$$b_y = b_x - 1. \tag{6}$$$
Now insert (6) into (4) to keep everything in terms of $$b_x$$:
$$$b_z = b_y = b_x - 1. \tag{7}$$$
We next impose the dot-product condition. The scalar (dot) product formula is
$$\vec a \cdot \vec b = a_x b_x + a_y b_y + a_z b_z.$$
Because $$\vec a = (1,1,1),$$ this becomes simply the sum of the components of $$\vec b$$:
$$$\vec a \cdot \vec b = b_x + b_y + b_z = 3. \tag{8}$$$
Using (6) and (7) to replace $$b_y$$ and $$b_z$$ in (8) we get
$$b_x + (b_x - 1) + (b_x - 1) = 3.$$
Simplifying the left side gives
$$3b_x - 2 = 3,$$
so
$$3b_x = 5$$
and therefore
$$$b_x = \frac{5}{3}. \tag{9}$$$
Using (6) we find
$$b_y = b_x - 1 = \frac{5}{3} - 1 = \frac{2}{3},$$
and from (7)
$$b_z = \frac{2}{3}.$$
Thus the explicit vector is
$$\vec b = \frac{5}{3}\,\hat i + \frac{2}{3}\,\hat j + \frac{2}{3}\,\hat k.$$
Finally we compute its magnitude. The formula for the magnitude of a vector $$\vec v = (v_x, v_y, v_z)$$ is
$$|\vec v| = \sqrt{v_x^2 + v_y^2 + v_z^2}.$$
Applying this to $$\vec b$$ we have
$$|\vec b| = \sqrt{\left(\frac{5}{3}\right)^2 + \left(\frac{2}{3}\right)^2 + \left(\frac{2}{3}\right)^2} = \sqrt{\frac{25}{9} + \frac{4}{9} + \frac{4}{9}} = \sqrt{\frac{33}{9}} = \sqrt{\frac{11}{3}}.$$
Hence, the correct answer is Option C.
If the position vectors of the vertices A, B and C of a $$\triangle$$ABC are respectively $$4\hat{i} + 7\hat{j} + 8\hat{k}$$, $$2\hat{i} + 3\hat{j} + 4\hat{k}$$ and $$2\hat{i} + 5\hat{j} + 7\hat{k}$$, then the position vector of the point, where the bisector of $$\angle A$$ meets BC is:
We have the position vectors of the three vertices written as $$\vec A = 4\hat i + 7\hat j + 8\hat k,\; \vec B = 2\hat i + 3\hat j + 4\hat k,\; \vec C = 2\hat i + 5\hat j + 7\hat k.$$
To locate the point where the internal bisector of $$\angle A$$ meets the side BC, we use the well-known Angle-Bisector Theorem. It states:
$$\frac{BD}{DC} = \frac{AB}{AC},$$
where D is the required point on BC, BD is the length from B to D and DC is the length from D to C.
So we must first compute the lengths $$AB$$ and $$AC.$$
The vector $$\overrightarrow{AB}$$ is obtained by subtracting $$\vec A$$ from $$\vec B$$:
$$\overrightarrow{AB} = \vec B - \vec A = (2-4)\hat i + (3-7)\hat j + (4-8)\hat k = -2\hat i -4\hat j -4\hat k.$$
Now its magnitude is
$$|AB| = \sqrt{(-2)^2 + (-4)^2 + (-4)^2} = \sqrt{4 + 16 + 16} = \sqrt{36} = 6.$$
Next, the vector $$\overrightarrow{AC}$$ is
$$\overrightarrow{AC} = \vec C - \vec A = (2-4)\hat i + (5-7)\hat j + (7-8)\hat k = -2\hat i -2\hat j -1\hat k.$$
Its magnitude is
$$|AC| = \sqrt{(-2)^2 + (-2)^2 + (-1)^2} = \sqrt{4 + 4 + 1} = \sqrt{9} = 3.$$
So we obtain
$$\frac{AB}{AC} = \frac{6}{3} = 2,$$
which gives the ratio
$$BD : DC = 2 : 1.$$
Having the ratio, we now apply the Section Formula. If a point D divides the segment joining vectors $$\vec B$$ and $$\vec C$$ internally in the ratio $$m:n$$ (here $$m=2, n=1$$ so that $$BD:DC = 2:1$$), then
$$\vec D = \frac{n\,\vec B + m\,\vec C}{m+n}.$$
Substituting $$m = 2$$ and $$n = 1$$ we get
$$\vec D = \frac{1\cdot\vec B + 2\cdot\vec C}{2+1} = \frac{\vec B + 2\vec C}{3}.$$
First compute $$\vec B + 2\vec C$$:
$$\vec B + 2\vec C = (2\hat i + 3\hat j + 4\hat k) + 2(2\hat i + 5\hat j + 7\hat k)$$
$$= 2\hat i + 3\hat j + 4\hat k + 4\hat i + 10\hat j + 14\hat k$$
$$= (2+4)\hat i + (3+10)\hat j + (4+14)\hat k = 6\hat i + 13\hat j + 18\hat k.$$
Now divide by 3:
$$\vec D = \frac{1}{3}(6\hat i + 13\hat j + 18\hat k).$$
This expression exactly matches the second option provided.
Hence, the correct answer is Option B.
If $$\vec{a}$$, $$\vec{b}$$, and $$\vec{c}$$ are unit vectors such that $$\vec{a} + 2\vec{b} + 2\vec{c} = \vec{0}$$, then $$|\vec{a} \times \vec{c}|$$ is equal to:
We are told that $$\vec a,\;\vec b,\;\vec c$$ are unit vectors and they satisfy the vector equation
$$\vec a+2\vec b+2\vec c=\vec 0.$$
Because the right-hand side is the zero vector, its magnitude is zero. Hence, applying the definition of the square of a vector’s magnitude, we have
$$\bigl|\vec a+2\vec b+2\vec c\bigr|^{2}=0$$
and, by the dot-product expansion formula $$(\vec p+\vec q+\vec r)\cdot(\vec p+\vec q+\vec r)=\vec p\cdot\vec p+\vec q\cdot\vec q+\vec r\cdot\vec r+2\vec p\cdot\vec q+2\vec p\cdot\vec r+2\vec q\cdot\vec r,$$ we write
$$\bigl(\vec a+2\vec b+2\vec c\bigr)\cdot\bigl(\vec a+2\vec b+2\vec c\bigr)=0.$$
Carrying out the dot products term by term, we obtain
$$\vec a\cdot\vec a+4\,\vec b\cdot\vec b+4\,\vec c\cdot\vec c+2\bigl(\vec a\cdot2\vec b+\vec a\cdot2\vec c+2\vec b\cdot2\vec c\bigr)=0.$$
Because each of the three vectors is a unit vector, $$\vec a\cdot\vec a=\vec b\cdot\vec b=\vec c\cdot\vec c=1.$$ Introducing the notations
$$x=\vec a\cdot\vec b,\qquad y=\vec b\cdot\vec c,\qquad z=\vec a\cdot\vec c,$$
the above equation becomes
$$1+4+4+4x+4z+8y=0,$$
that is,
$$9+4x+4z+8y=0. \quad -(1)$$
Next, we exploit the original relation $$\vec a=-2\vec b-2\vec c.$$ Taking the dot product of this with each of the unit vectors in turn gives three more scalar equations.
First, dotting with $$\vec a:$$
$$\vec a\cdot\vec a=-2\bigl(\vec a\cdot\vec b+\vec a\cdot\vec c\bigr)\;\Longrightarrow\;1=-2(x+z),$$
so
$$x+z=-\dfrac12. \quad -(2)$$
Second, dotting with $$\vec b:$$
$$\vec b\cdot\vec a+2\,\vec b\cdot\vec b+2\,\vec b\cdot\vec c=0\;\Longrightarrow\;x+2+2y=0,$$
hence
$$x+2y=-2. \quad -(3)$$
Third, dotting with $$\vec c:$$
$$\vec c\cdot\vec a+2\,\vec c\cdot\vec b+2\,\vec c\cdot\vec c=0\;\Longrightarrow\;z+2y+2=0,$$
which simplifies to
$$z+2y=-2. \quad -(4)$$
We now solve the simultaneous linear equations (2), (3) and (4) for $$x,\;y,\;z.$$
Subtracting (4) from (3) gives
$$(x+2y)-(z+2y)=(-2)-(-2)\;\Longrightarrow\;x-z=0,$$
so
$$x=z. \quad -(5)$$
Substituting $$z=x$$ from (5) into (2) yields
$$x+x=-\dfrac12\;\Longrightarrow\;2x=-\dfrac12\;\Longrightarrow\;x=-\dfrac14.$$
Therefore, by (5),
$$z=-\dfrac14.$$
Finally, using $$x=-\dfrac14$$ in (3) gives
$$-\dfrac14+2y=-2\;\Longrightarrow\;2y=-2+\dfrac14=-\dfrac74\;\Longrightarrow\;y=-\dfrac78.$$
We now have the specific value we need:
$$\vec a\cdot\vec c=z=-\dfrac14.$$
Because both $$\vec a$$ and $$\vec c$$ are unit vectors, the magnitude of their cross product is determined by the fundamental formula
$$|\vec a\times\vec c|^{2}=|\vec a|^{2}\,|\vec c|^{2}-\bigl(\vec a\cdot\vec c\bigr)^{2}.$$
With $$|\vec a|=|\vec c|=1,$$ this gives
$$|\vec a\times\vec c|^{2}=1\cdot1-\left(-\dfrac14\right)^{2}=1-\dfrac1{16}=\dfrac{15}{16}.$$
Taking the positive square root,
$$|\vec a\times\vec c|=\sqrt{\dfrac{15}{16}}=\dfrac{\sqrt{15}}{4}.$$
Hence, the correct answer is Option B.
Let $$\vec{u}$$ be a vector coplanar with the vectors $$\vec{a} = 2\hat{i} + 3\hat{j} - \hat{k}$$ and $$\vec{b} = \hat{j} + \hat{k}$$. If $$\vec{u}$$ is perpendicular to $$\vec{a}$$ and $$\vec{u} \cdot \vec{b} = 24$$, then $$|\vec{u}|^2$$ is equal to:
We are told that the required vector $$\vec u$$ lies in the plane of the two given vectors, so the very first thing we write is that any vector coplanar with $$\vec a$$ and $$\vec b$$ can be expressed as their linear combination:
$$\vec u = p\,\vec a + q\,\vec b,$$
where $$p$$ and $$q$$ are real scalars to be determined.
The components of the given vectors are
$$\vec a = 2\hat i + 3\hat j - \hat k \; \Longrightarrow \; (2,\;3,\;-1),$$ $$\vec b = 0\hat i + 1\hat j + 1\hat k \; \Longrightarrow \; (0,\;1,\;1).$$
From these we calculate three basic scalar products that will repeatedly occur:
Magnitude‐square of $$\vec a$$: $$\vec a \cdot \vec a = 2^2 + 3^2 + (-1)^2 = 4 + 9 + 1 = 14.$$
Magnitude‐square of $$\vec b$$: $$\vec b \cdot \vec b = 0^2 + 1^2 + 1^2 = 0 + 1 + 1 = 2.$$
Mixed dot product: $$\vec a \cdot \vec b = 2\cdot 0 + 3\cdot 1 + (-1)\cdot 1 = 0 + 3 - 1 = 2.$$
Next, the condition “$$\vec u$$ is perpendicular to $$\vec a$$” translates to the dot product being zero:
$$\vec u \cdot \vec a = 0.$$
Substituting $$\vec u = p\vec a + q\vec b,$$ we get
$$\vec u \cdot \vec a = (p\vec a + q\vec b)\cdot\vec a = p(\vec a\cdot\vec a) + q(\vec b\cdot\vec a).$$
Using the already computed dot products, this becomes
$$p(14) + q(2) = 0.$$
So,
$$14p + 2q = 0 \quad\Longrightarrow\quad q = -7p.$$
The problem also tells us that
$$\vec u \cdot \vec b = 24.$$
Again substituting $$\vec u = p\vec a + q\vec b,$$ we write
$$\vec u \cdot \vec b = (p\vec a + q\vec b)\cdot\vec b = p(\vec a\cdot\vec b) + q(\vec b\cdot\vec b).$$
Putting the known numbers, we obtain
$$p(2) + q(2) = 24.$$
Dividing by 2 on both sides simplifies the expression:
$$p + q = 12.$$
Now we substitute $$q = -7p$$ (found earlier) into this linear equation:
$$p + (-7p) = 12 \quad\Longrightarrow\quad -6p = 12.$$
Hence,
$$p = -2,$$
and therefore
$$q = -7(-2) = 14.$$
With $$p$$ and $$q$$ known, we can finally work out the squared magnitude of $$\vec u$$. A general algebraic identity for a linear combination states
$$|\vec u|^2 \;=\; \vec u\cdot\vec u = (p\vec a + q\vec b)\cdot(p\vec a + q\vec b)$$ $$= p^2(\vec a\cdot\vec a) + q^2(\vec b\cdot\vec b) + 2pq(\vec a\cdot\vec b).$$
Putting the numerical values step by step:
$$p^2(\vec a\cdot\vec a) = (-2)^2 \times 14 = 4 \times 14 = 56,$$
$$q^2(\vec b\cdot\vec b) = 14^2 \times 2 = 196 \times 2 = 392,$$
$$2pq(\vec a\cdot\vec b) = 2 \times (-2) \times 14 \times 2 = -4 \times 14 \times 2 = -56 \times 2 = -112.$$
Adding these three contributions:
$$|\vec u|^2 = 56 + 392 - 112 = 336.$$
Hence, the correct answer is Option B.
Given, $$\vec{a} = 2\hat{i} + \hat{j} - 2\hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j}$$. Let $$\vec{c}$$ be a vector such that $$|\vec{c} - \vec{a}| = 3$$, $$|\vec{a} \times \vec{b} \times \vec{c}| = 3$$ and the angle between $$\vec{c}$$ and $$\vec{a} \times \vec{b}$$ be 30°. Then $$\vec{a} \cdot \vec{c}$$ is equal to:
We have $$\vec a = 2\hat i + \hat j - 2\hat k$$ and $$\vec b = \hat i + \hat j$$. Let us first evaluate the cross product $$\vec a \times \vec b$$ because it will appear again and again.
Using the determinant form of the cross product,
$$\vec a \times \vec b = \begin{vmatrix} \hat i & \hat j & \hat k\\ 2 & 1 & -2\\ 1 & 1 & 0 \end{vmatrix} = \hat i\,(1\cdot0-(-2)\cdot1)\;-\;\hat j\,(2\cdot0-(-2)\cdot1)\;+\;\hat k\,(2\cdot1-1\cdot1)$$
$$\qquad\;= \hat i\,(0+2)\;-\;\hat j\,(0+2)\;+\;\hat k\,(2-1) = 2\hat i - 2\hat j + \hat k.$$
So we denote $$\vec d = \vec a \times \vec b = 2\hat i - 2\hat j + \hat k.$$
The magnitude of $$\vec d$$ is
$$|\vec d| = \sqrt{(2)^2 + (-2)^2 + (1)^2} = \sqrt{4 + 4 + 1} = \sqrt 9 = 3.$$
According to the question, the angle between $$\vec c$$ and $$\vec d$$ is $$30^\circ$$. We also know the magnitude of the cross product of these two vectors: $$|\vec d \times \vec c| = 3.$$ For any two vectors $$\vec p$$ and $$\vec q$$ the formula for the magnitude of their cross product is
$$|\vec p \times \vec q| = |\vec p|\,|\vec q| \sin\theta,$$
where $$\theta$$ is the angle between them. Applying this with $$\vec p=\vec d$$, $$\vec q=\vec c$$ and $$\theta = 30^\circ$$ gives
$$|\vec d \times \vec c| = |\vec d|\,|\vec c| \sin 30^\circ = 3 \, |\vec c| \left(\frac12\right) = \frac{3}{2}\,|\vec c|.$$
The question states that this value equals 3, so
$$\frac{3}{2}\,|\vec c| = 3 \;\;\Longrightarrow\;\; |\vec c| = \frac{3 \times 2}{3} = 2.$$
Thus $$|\vec c| = 2.$$ Another piece of information provided is $$|\vec c - \vec a| = 3.$$ To use this we expand the square of the magnitude. The standard identity is
$$|\vec u - \vec v|^2 = |\vec u|^2 + |\vec v|^2 - 2\,\vec u\cdot\vec v.$$
Putting $$\vec u = \vec c$$ and $$\vec v = \vec a,$$ we write
$$|\vec c - \vec a|^2 = |\vec c|^2 + |\vec a|^2 - 2\,\vec a\cdot\vec c.$$
We already have $$|\vec c - \vec a| = 3,$$ so the left-hand side is $$3^2 = 9.$$ We have also just found $$|\vec c| = 2,$$ therefore $$|\vec c|^2 = 4.$$ Next we need $$|\vec a|.$$ Its magnitude is
$$|\vec a| = \sqrt{(2)^2 + (1)^2 + (-2)^2} = \sqrt{4 + 1 + 4} = \sqrt 9 = 3,$$ so $$|\vec a|^2 = 9.$$
Substituting these values into the identity,
$$9 = 4 + 9 - 2\,\vec a\cdot\vec c.$$
Simplifying the right-hand side, $$4 + 9 = 13,$$ hence
$$9 = 13 - 2\,\vec a\cdot\vec c.$$
Now shift terms to isolate the dot product:
$$-2\,\vec a\cdot\vec c = 9 - 13 = -4,$$
so
$$\vec a\cdot\vec c = \frac{-4}{-2} = 2.$$
Therefore $$\vec a \cdot \vec c = 2.$$
Hence, the correct answer is Option B.
If the vector $$\vec{b} = 3\hat{j} + 4\hat{k}$$ is written as the sum of a vector $$\vec{b_1}$$, parallel to $$\vec{a} = \hat{i} + \hat{j}$$ and a vector $$\vec{b_2}$$, perpendicular to $$\vec{a}$$, then $$\vec{b_1} \times \vec{b_2}$$ is equal to:
We first write down the two given vectors in component form
$$\vec{a}=1\,\hat{i}+1\,\hat{j}+0\,\hat{k}\;,-(1)$$
$$\vec{b}=0\,\hat{i}+3\,\hat{j}+4\,\hat{k}\;.-(2)$$
Let the part of $$\vec{b}$$ that is parallel to $$\vec{a}$$ be $$\vec{b_1}$$. Any vector parallel to $$\vec{a}$$ must be some real multiple of $$\vec{a}$$, so we set
$$\vec{b_1}=t\,\vec{a}\;,-(3)$$
where $$t$$ is a scalar to be determined. The remaining part
$$\vec{b_2}=\vec{b}-\vec{b_1}\;,-(4)$$
is by construction perpendicular to $$\vec{a}$$, i.e.
$$\vec{a}\cdot\vec{b_2}=0\;.-(5)$$
Substituting $$\vec{b_2}$$ from -(4) into the perpendicularity condition -(5) gives
$$\vec{a}\cdot(\vec{b}-\vec{b_1})=0\;.-(6)$$
Expand the dot product in -(6):
$$\vec{a}\cdot\vec{b}-\vec{a}\cdot\vec{b_1}=0\;.-(7)$$
Compute each term separately. First, using -(1) and -(2),
$$\vec{a}\cdot\vec{b}=(1)(0)+(1)(3)+(0)(4)=3\;.-(8)$$
For the second dot product we use -(3) and the distributive law:
$$\vec{a}\cdot\vec{b_1}=\vec{a}\cdot(t\vec{a})=t(\vec{a}\cdot\vec{a})=t|\vec{a}|^{2}\;.-(9)$$
The squared magnitude of $$\vec{a}$$ comes directly from -(1):
$$|\vec{a}|^{2}=(1)^{2}+(1)^{2}+(0)^{2}=2\;.-(10)$$
Insert -(8), -(9) and -(10) into equation -(7):
$$3-t(2)=0\;,-(11)$$
from which
$$t=\dfrac{3}{2}\;.-(12)$$
Now use -(3) and -(12) to obtain $$\vec{b_1}$$ explicitly:
$$\vec{b_1}=\dfrac{3}{2}(1\,\hat{i}+1\,\hat{j}+0\,\hat{k})=\dfrac{3}{2}\hat{i}+\dfrac{3}{2}\hat{j}+0\,\hat{k}\;.-(13)$$
Next, calculate $$\vec{b_2}$$ by substituting -(13) into -(4):
$$\vec{b_2}=(0\,\hat{i}+3\,\hat{j}+4\,\hat{k})-\left(\dfrac{3}{2}\hat{i}+\dfrac{3}{2}\hat{j}+0\,\hat{k}\right)\;,-(14)$$
and subtract component-wise:
$$\vec{b_2}=\Bigl(0-\dfrac{3}{2}\Bigr)\hat{i}+\Bigl(3-\dfrac{3}{2}\Bigr)\hat{j}+(4-0)\hat{k}=-\dfrac{3}{2}\hat{i}+\dfrac{3}{2}\hat{j}+4\hat{k}\;.-(15)$$
As a quick check, verify the perpendicularity using -(1) and -(15):
$$\vec{a}\cdot\vec{b_2}=1\Bigl(-\dfrac{3}{2}\Bigr)+1\Bigl(\dfrac{3}{2}\Bigr)+0(4)=0,$$
so the condition is satisfied.
The desired quantity is the cross product $$\vec{b_1}\times\vec{b_2}$$. Using -(13) and -(15) we write the 3×3 determinant form:
$$ \vec{b_1}\times\vec{b_2} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \dfrac{3}{2} & \dfrac{3}{2} & 0 \\ -\dfrac{3}{2} & \dfrac{3}{2} & 4 \end{vmatrix}\;.-(16) $$
Now expand the determinant component by component.
• $$\hat{i}$$-component:
$$ \left(\dfrac{3}{2}\right)(4)-0\left(\dfrac{3}{2}\right)=6\;.-(17) $$
• $$\hat{j}$$-component (remember the negative sign):
$$ -\Bigl[\left(\dfrac{3}{2}\right)(4)-0\Bigl(-\dfrac{3}{2}\Bigr)\Bigr]=-6\;.-(18) $$
• $$\hat{k}$$-component:
$$ \left(\dfrac{3}{2}\right)\left(\dfrac{3}{2}\right)-\left(\dfrac{3}{2}\right)\Bigl(-\dfrac{3}{2}\Bigr)=\dfrac{9}{4}+\dfrac{9}{4}=\dfrac{9}{2}\;.-(19) $$
Collecting the three components from -(17), -(18) and -(19) gives
$$\vec{b_1}\times\vec{b_2}=6\,\hat{i}-6\,\hat{j}+\dfrac{9}{2}\,\hat{k}\;.-(20)$$
This matches exactly the vector in Option A.
Hence, the correct answer is Option A.
The area (in sq. units) of the parallelogram whose diagonals are along the vectors $$8\hat{i} - 6\hat{j}$$ and $$3\hat{i} + 4\hat{j} - 12\hat{k}$$, is:
We are given the two diagonal vectors of a parallelogram as $$\vec{d_1}=8\hat{i}-6\hat{j}$$ and $$\vec{d_2}=3\hat{i}+4\hat{j}-12\hat{k}.$$
For any parallelogram whose sides are $$\vec{a}$$ and $$\vec{b},$$ the diagonals become $$\vec{d_1}=\vec{a}+\vec{b}$$ and $$\vec{d_2}=\vec{a}-\vec{b}.$$
Using these, the vector cross-product of the diagonals is
$$\vec{d_1}\times\vec{d_2}=(\vec{a}+\vec{b})\times(\vec{a}-\vec{b}).$$
Expanding with the distributive property of the cross product, we have
$$\vec{d_1}\times\vec{d_2}=\vec{a}\times\vec{a}-\vec{a}\times\vec{b}+\vec{b}\times\vec{a}-\vec{b}\times\vec{b}.$$
Because any vector crossed with itself is the zero vector, $$\vec{a}\times\vec{a}=0$$ and $$\vec{b}\times\vec{b}=0.$$ Also, the cross product is anti-commutative, so $$\vec{b}\times\vec{a}=-(\vec{a}\times\vec{b}).$$ Substituting these facts, we get
$$\vec{d_1}\times\vec{d_2}=-\vec{a}\times\vec{b}-\vec{a}\times\vec{b}=-2\,\vec{a}\times\vec{b}.$$
Taking magnitudes on both sides gives
$$\lvert\vec{d_1}\times\vec{d_2}\rvert=2\,\lvert\vec{a}\times\vec{b}\rvert.$$
The magnitude $$\lvert\vec{a}\times\vec{b}\rvert$$ is precisely the area of the parallelogram. Therefore the required area is obtained from the diagonals by the formula
$$A=\frac{1}{2}\,\lvert\vec{d_1}\times\vec{d_2}\rvert.$$
Now we compute the cross product of the given diagonals. Writing the determinant,
$$ \vec{d_1}\times\vec{d_2}= \begin{vmatrix} \hat{i} & \hat{j} & \hat{k}\\ 8 & -6 & 0\\ 3 & 4 & -12 \end{vmatrix}. $$
Expanding along the first row, we have
$$ \vec{d_1}\times\vec{d_2}= \hat{i}\Bigl((-6)(-12)-0\cdot4\Bigr) - \hat{j}\Bigl(8(-12)-0\cdot3\Bigr) + \hat{k}\Bigl(8\cdot4-(-6)\cdot3\Bigr). $$
Simplifying each component step by step:
For $$\hat{i}$$ component: $$(-6)(-12)-0\cdot4=72-0=72.$$
For $$\hat{j}$$ component: $$8(-12)-0\cdot3=-96-0=-96,$$ and the overall sign in front of $$\hat{j}$$ makes it $$-\,-96=+96.$$
For $$\hat{k}$$ component: $$8\cdot4-(-6)\cdot3=32+18=50.$$
So we obtain
$$\vec{d_1}\times\vec{d_2}=72\hat{i}+96\hat{j}+50\hat{k}.$$
Next, we find its magnitude:
$$ \lvert\vec{d_1}\times\vec{d_2}\rvert =\sqrt{72^{2}+96^{2}+50^{2}} =\sqrt{5184+9216+2500} =\sqrt{16900} =130. $$
Finally, substituting into the area formula,
$$ A=\frac{1}{2}\times130=65\text{ square units}. $$
Hence, the correct answer is Option B.
In a triangle $$ABC$$, right angle at vertex $$A$$, if the position vectors of $$A$$, $$B$$ and $$C$$ are respectively $$3\hat{i} + \hat{j} - \hat{k}$$, $$-\hat{i} + 3\hat{j} + p\hat{k}$$ and $$5\hat{i} + q\hat{j} - 4\hat{k}$$, then the point $$(p, q)$$ lies on a line:
In triangle $$ABC$$, the right angle is at vertex $$A$$. The position vectors are given as:
Position vector of $$A$$: $$3\hat{i} + \hat{j} - \hat{k}$$
Position vector of $$B$$: $$-\hat{i} + 3\hat{j} + p\hat{k}$$
Position vector of $$C$$: $$5\hat{i} + q\hat{j} - 4\hat{k}$$
Since the angle at $$A$$ is right-angled, the vectors $$\overrightarrow{AB}$$ and $$\overrightarrow{AC}$$ are perpendicular. Therefore, their dot product is zero.
First, compute $$\overrightarrow{AB}$$:
$$\overrightarrow{AB} = \text{Position vector of } B - \text{Position vector of } A$$
$$\overrightarrow{AB} = (-\hat{i} + 3\hat{j} + p\hat{k}) - (3\hat{i} + \hat{j} - \hat{k})$$
$$\overrightarrow{AB} = -\hat{i} + 3\hat{j} + p\hat{k} - 3\hat{i} - \hat{j} + \hat{k}$$
$$\overrightarrow{AB} = (-\hat{i} - 3\hat{i}) + (3\hat{j} - \hat{j}) + (p\hat{k} + \hat{k})$$
$$\overrightarrow{AB} = -4\hat{i} + 2\hat{j} + (p + 1)\hat{k}$$
Next, compute $$\overrightarrow{AC}$$:
$$\overrightarrow{AC} = \text{Position vector of } C - \text{Position vector of } A$$
$$\overrightarrow{AC} = (5\hat{i} + q\hat{j} - 4\hat{k}) - (3\hat{i} + \hat{j} - \hat{k})$$
$$\overrightarrow{AC} = 5\hat{i} + q\hat{j} - 4\hat{k} - 3\hat{i} - \hat{j} + \hat{k}$$
$$\overrightarrow{AC} = (5\hat{i} - 3\hat{i}) + (q\hat{j} - \hat{j}) + (-4\hat{k} + \hat{k})$$
$$\overrightarrow{AC} = 2\hat{i} + (q - 1)\hat{j} - 3\hat{k}$$
Since $$\overrightarrow{AB}$$ and $$\overrightarrow{AC}$$ are perpendicular, their dot product is zero:
$$\overrightarrow{AB} \cdot \overrightarrow{AC} = 0$$
Substitute the vectors:
$$[-4\hat{i} + 2\hat{j} + (p + 1)\hat{k}] \cdot [2\hat{i} + (q - 1)\hat{j} - 3\hat{k}] = 0$$
Compute the dot product component-wise:
$$(-4) \times 2 + 2 \times (q - 1) + (p + 1) \times (-3) = 0$$
Simplify:
$$-8 + 2(q - 1) - 3(p + 1) = 0$$
Expand the terms:
$$-8 + 2q - 2 - 3p - 3 = 0$$
Combine like terms:
$$-8 - 2 - 3 + 2q - 3p = 0$$
$$-13 + 2q - 3p = 0$$
Rearrange to:
$$2q - 3p = 13$$
This equation represents a straight line in the $$pq$$-plane. Rewrite it in slope-intercept form:
$$2q = 3p + 13$$
$$q = \frac{3}{2}p + \frac{13}{2}$$
The slope of this line is $$\frac{3}{2}$$, which is positive.
A positive slope indicates that the line makes an acute angle with the positive direction of the $$x$$-axis.
Now, evaluate the options:
A. Making an obtuse angle with the positive direction of $$x$$-axis: This requires a negative slope, but the slope is positive, so false.
B. Parallel to $$x$$-axis: This requires a slope of zero, but the slope is $$\frac{3}{2} \neq 0$$, so false.
C. Parallel to $$y$$-axis: This requires an undefined slope (vertical line), but the slope is defined, so false.
D. Making an acute angle with the positive direction of $$x$$-axis: Since the slope is positive, this is true.
Hence, the correct answer is Option D.
Let $$\vec{a}$$, $$\vec{b}$$ and $$\vec{c}$$ be three unit vectors such that $$\vec{a} \times (\vec{b} \times \vec{c}) = \frac{\sqrt{3}}{2}(\vec{b} + \vec{c})$$. If $$\vec{b}$$ is not parallel to $$\vec{c}$$, then the angle between $$\vec{a}$$ and $$\vec{b}$$ is
We are told that $$\vec a,\;\vec b,\;\vec c$$ are unit vectors (that is, each has magnitude 1) and that they satisfy the vector equation
$$\vec a \times (\vec b \times \vec c)=\frac{\sqrt3}{2}\,(\vec b+\vec c).$$Because $$\vec b$$ is not parallel to $$\vec c$$, we may treat $$\vec b$$ and $$\vec c$$ as independent directions. The key tool here is the standard vector triple-product formula:
$$\boxed{\;\vec p \times (\vec q \times \vec r)=\vec q(\vec p\cdot\vec r)\;-\;\vec r(\vec p\cdot\vec q)\;}.$$We apply this identity with $$\vec p=\vec a,\;\vec q=\vec b,\;\vec r=\vec c$$. Hence
$$\vec a \times (\vec b \times \vec c) =\vec b\,(\vec a\cdot\vec c)\;-\;\vec c\,(\vec a\cdot\vec b).$$To keep the algebra transparent, we introduce the scalar symbols
$$x=\vec a\cdot\vec c,\qquad y=\vec a\cdot\vec b.$$Both $$x$$ and $$y$$ are simply cosines of the respective angles, because each pair of vectors involved has unit length. Substituting these into the expression for the triple product gives
$$\vec a \times (\vec b \times \vec c)=x\,\vec b\;-\;y\,\vec c.$$But the problem statement tells us that the very same vector equals $$\tfrac{\sqrt3}{2}\,(\vec b+\vec c)$$. Therefore we equate the two expressions:
$$x\,\vec b\;-\;y\,\vec c=\frac{\sqrt3}{2}\,\vec b+\frac{\sqrt3}{2}\,\vec c.$$Since $$\vec b$$ and $$\vec c$$ are not parallel, the only way two linear combinations of them can be equal is for the coefficients of $$\vec b$$ to match and, independently, the coefficients of $$\vec c$$ to match. Thus we obtain the pair of equations
$$x=\frac{\sqrt3}{2},\qquad -y=\frac{\sqrt3}{2}.$$From the second equation we get
$$y=-\,\frac{\sqrt3}{2}.$$Recall now that $$y=\vec a\cdot\vec b$$, and for unit vectors the dot product equals the cosine of the angle $$\theta$$ between them: $$\vec a\cdot\vec b=\cos\theta$$. Hence
$$\cos\theta=-\,\frac{\sqrt3}{2}.$$The cosine value $$-\frac{\sqrt3}{2}$$ corresponds to an angle of $$150^\circ$$ (or $$5\pi/6$$ radians) in the principal range $$0\le\theta\le\pi$$.
Therefore, the angle between $$\vec a$$ and $$\vec b$$ is
$$\theta=\frac{5\pi}{6}.$$Hence, the correct answer is Option B.
$$ABC$$ is a triangle in a plane with vertices $$A(2, 3, 5)$$, $$B(-1, 3, 2)$$ and $$C(\lambda, 5, \mu)$$. If the median through $$A$$ is equally inclined to the coordinate axes, then the value of $$(\lambda^3 + \mu^3 + 5)$$ is
We have the triangle $$ABC$$ with
$$A(2,\,3,\,5), \qquad B(-1,\,3,\,2), \qquad C(\lambda,\,5,\,\mu).$$
The median through $$A$$ meets the midpoint of the side $$BC$$. Let us first find this midpoint. Using the midpoint formula
Midpoint $$M\Bigl(x_M,\,y_M,\,z_M\Bigr)=\left(\dfrac{x_B+x_C}{2},\,\dfrac{y_B+y_C}{2},\,\dfrac{z_B+z_C}{2}\right),$$
we substitute the coordinates of $$B$$ and $$C$$:
$$x_M=\dfrac{-1+\lambda}{2},\qquad y_M=\dfrac{3+5}{2}=4,\qquad z_M=\dfrac{2+\mu}{2}.$$
Now we write the vector $$\overrightarrow{AM}$$ by subtracting the coordinates of $$A$$ from those of $$M$$:
$$\overrightarrow{AM}=\Bigl(x_M-2,\,y_M-3,\,z_M-5\Bigr).$$
Carrying out the subtraction term by term,
$$\begin{aligned} x\text{-component}&=\dfrac{-1+\lambda}{2}-2 =\dfrac{-1+\lambda-4}{2} =\dfrac{\lambda-5}{2},\\[4pt] y\text{-component}&=4-3=1,\\[4pt] z\text{-component}&=\dfrac{2+\mu}{2}-5 =\dfrac{2+\mu-10}{2} =\dfrac{\mu-8}{2}. \end{aligned}$$
Thus
$$\overrightarrow{AM}=\left(\dfrac{\lambda-5}{2},\;1,\;\dfrac{\mu-8}{2}\right).$$
The condition given is that this median is equally inclined to the three coordinate axes. For a vector $$\bigl(l,\,m,\,n\bigr)$$ the cosines of the angles it makes with the $$x-,y-,z-$$axes are, respectively,
$$\cos\alpha=\dfrac{l}{\sqrt{l^{2}+m^{2}+n^{2}}},\qquad \cos\beta=\dfrac{m}{\sqrt{l^{2}+m^{2}+n^{2}}},\qquad \cos\gamma=\dfrac{n}{\sqrt{l^{2}+m^{2}+n^{2}}}.$$
If the vector is equally inclined to all three axes, then $$\alpha=\beta=\gamma$$, and hence
$$\cos\alpha=\cos\beta=\cos\gamma.$$
This equality forces the numerators to be equal, so we must have
$$l=m=n \quad\text{or}\quad l=m=n=-k,$$
i.e. the three components are equal in magnitude and have the same sign. Applying this to $$\overrightarrow{AM}$$, we set
$$\dfrac{\lambda-5}{2}=1=\dfrac{\mu-8}{2}\quad$$ or $$\quad \dfrac{\lambda-5}{2}=-1=\dfrac{\mu-8}{2}.$$
We examine each possibility.
First possibility:
$$\dfrac{\lambda-5}{2}=1 \;\Longrightarrow\; \lambda-5=2 \;\Longrightarrow\; \lambda=7,$$
$$\dfrac{\mu-8}{2}=1 \;\Longrightarrow\; \mu-8=2 \;\Longrightarrow\; \mu=10.$$
Second possibility:
$$\dfrac{\lambda-5}{2}=-1 \;\Longrightarrow\; \lambda-5=-2 \;\Longrightarrow\; \lambda=3,$$
$$\dfrac{\mu-8}{2}=-1 \;\Longrightarrow\; \mu-8=-2 \;\Longrightarrow\; \mu=6.$$
Next, the problem asks for the value of $$\lambda^{3}+\mu^{3}+5$$. We compute this expression for both sets of values and see which one appears in the options.
For $$\lambda=7,\;\mu=10$$:
$$\begin{aligned} \lambda^{3}+\mu^{3}+5 &=7^{3}+10^{3}+5\\ &=343+1000+5\\ &=1348. \end{aligned}$$
For $$\lambda=3,\;\mu=6$$:
$$\begin{aligned} \lambda^{3}+\mu^{3}+5 &=3^{3}+6^{3}+5\\ &=27+216+5\\ &=248. \end{aligned}$$
The value $$248$$ does not appear among the given options, whereas $$1348$$ does. Therefore the admissible solution is $$\lambda=7,\;\mu=10$$, giving
$$\lambda^{3}+\mu^{3}+5=1348.$$
Hence, the correct answer is Option 2.
Let $$ABC$$ be a triangle whose circumcentre is at $$P$$. If the position vectors of $$A$$, $$B$$, $$C$$ and $$P$$ are $$\vec{a}$$, $$\vec{b}$$, $$\vec{c}$$ and $$\frac{\vec{a}+\vec{b}+\vec{c}}{4}$$ respectively, then the position vector of the orthocentre of this triangle, is:
We are given that the position vectors of the vertices of the triangle are $$\vec{a},\; \vec{b},\; \vec{c}$$ and the position vector of its circum-centre is
$$\vec{P}= \frac{\vec{a}+\vec{b}+\vec{c}}{4}\;.$$
First recall the standard results concerning a triangle whose circum-centre is taken as the origin.
1. If we shift the origin to the circum-centre, the position vectors of the vertices become $$\vec{a}\,'=\vec{a}-\vec{P},\; \vec{b}\,'=\vec{b}-\vec{P},\; \vec{c}\,'=\vec{c}-\vec{P}.$$
2. In that coordinate system (origin at circum-centre) the orthocentre has the well-known vector form
$$\vec{H}\,'=\vec{a}\,'+\vec{b}\,'+\vec{c}\,'$$
because each altitude is perpendicular to a side chord through the centre of the circle.
3. Also, in any triangle the centroid is the average of the vertex vectors. Hence, with origin at the circum-centre, the centroid vector is
$$\vec{G}\,'=\frac{\vec{a}\,'+\vec{b}\,'+\vec{c}\,'}{3}\;.$$
From point 2 we immediately have the Euler line relation in that system:
$$\vec{H}\,'=3\vec{G}\,'\;.$$
Now we translate every quantity back to the original origin, where the circum-centre has the (non-zero) vector $$\vec{P}.$$
• The centroid in the original system is obtained by adding $$\vec{P}$$ to $$\vec{G}\,'.$$ Hence
$$\vec{G}= \vec{P}+ \vec{G}\,'= \vec{P}+ \frac{\vec{a}\,'+\vec{b}\,'+\vec{c}\,'}{3}.$$
Since $$\vec{a}\,'+\vec{b}\,'+\vec{c}\,' = (\vec{a}-\vec{P})+(\vec{b}-\vec{P})+(\vec{c}-\vec{P}) = \vec{a}+\vec{b}+\vec{c}-3\vec{P},$$ we have
$$\vec{G}= \vec{P}+ \frac{\vec{a}+\vec{b}+\vec{c}-3\vec{P}}{3}
= \frac{\vec{a}+\vec{b}+\vec{c}}{3}.$$
(This is just the familiar centroid formula, so the translation checks out.)
• The orthocentre vector in the original system is obtained by adding $$\vec{P}$$ to $$\vec{H}\,'.$$ Using $$\vec{H}\,'= \vec{a}\,'+\vec{b}\,'+\vec{c}\,'$$ gives
$$\vec{H}= \vec{P}+ (\vec{a}\,'+\vec{b}\,'+\vec{c}\,')
= \vec{P}+ \bigl(\vec{a}+\vec{b}+\vec{c}-3\vec{P}\bigr)
= \bigl(\vec{a}+\vec{b}+\vec{c}\bigr)-2\vec{P}.$$
But $$\vec{P}= \dfrac{\vec{a}+\vec{b}+\vec{c}}{4},$$ so substituting this value yields
$$\vec{H}= \bigl(\vec{a}+\vec{b}+\vec{c}\bigr)-2\left(\frac{\vec{a}+\vec{b}+\vec{c}}{4}\right)
= \bigl(\vec{a}+\vec{b}+\vec{c}\bigr)-\frac{\vec{a}+\vec{b}+\vec{c}}{2}
= \frac{\vec{a}+\vec{b}+\vec{c}}{2}\;.$$
Thus the position vector of the orthocentre of the triangle is
$$\boxed{\dfrac{\vec{a}+\vec{b}+\vec{c}}{2}}.$$
Hence, the correct answer is Option C.
In a parallelogram $$ABCD$$, $$\left|\overrightarrow{AB}\right| = a$$, $$\left|\overrightarrow{AD}\right| = b$$ and $$\left|\overrightarrow{AC}\right| = c$$. $$\overrightarrow{DB} \cdot \overrightarrow{AB}$$ has the value:
$$\vec{AC} = \vec{AB} + \vec{AD} = \mathbf{a} + \mathbf{b}$$
$$\vec{DB} = \vec{AB} - \vec{AD} = \mathbf{a} - \mathbf{b}$$
$$c^2 = |\vec{AC}|^2 = |\mathbf{a} + \mathbf{b}|^2$$
$$c^2 = \mathbf{a} \cdot \mathbf{a} + \mathbf{b} \cdot \mathbf{b} + 2(\mathbf{a} \cdot \mathbf{b})$$
$$c^2 = a^2 + b^2 + 2(\mathbf{a} \cdot \mathbf{b})$$
$$\mathbf{a} \cdot \mathbf{b} = \frac{c^2 - a^2 - b^2}{2}$$
$$\vec{DB} \cdot \vec{AB} = (\mathbf{a} - \mathbf{b}) \cdot \mathbf{a}$$
$$\vec{DB} \cdot \vec{AB} = (\mathbf{a} \cdot \mathbf{a}) - (\mathbf{b} \cdot \mathbf{a})$$
$$\vec{DB} \cdot \vec{AB} = a^2 - (\mathbf{a} \cdot \mathbf{b})$$
$$\vec{DB} \cdot \vec{AB} = a^2 - \left( \frac{c^2 - a^2 - b^2}{2} \right)$$
$$\vec{DB} \cdot \vec{AB} = \frac{3a^2 + b^2 - c^2}{2}$$
Let $$\vec{a}$$ and $$\vec{b}$$ be two unit vectors such that $$|\vec{a} + \vec{b}| = \sqrt{3}$$. If $$\vec{c} = \vec{a} + 2\vec{b} + (\vec{a} \times \vec{b})$$, then $$2|\vec{c}|$$ is equal to:
Since $$\vec{a}$$ and $$\vec{b}$$ are unit vectors, $$|\vec{a}| = |\vec{b}| = 1$$. Expanding $$|\vec{a} + \vec{b}|^2 = |\vec{a}|^2 + 2\vec{a}\cdot\vec{b} + |\vec{b}|^2 = 2 + 2\vec{a}\cdot\vec{b} = 3$$, which gives $$\vec{a}\cdot\vec{b} = \dfrac{1}{2}$$.
Now, $$\vec{c} = \vec{a} + 2\vec{b} + 3(\vec{a} \times \vec{b})$$. Since the cross product $$\vec{a} \times \vec{b}$$ is perpendicular to both $$\vec{a}$$ and $$\vec{b}$$, it is also perpendicular to every linear combination of $$\vec{a}$$ and $$\vec{b}$$. In particular, $$(\vec{a} + 2\vec{b}) \cdot (\vec{a} \times \vec{b}) = 0$$. Therefore $$|\vec{c}|^2 = |\vec{a} + 2\vec{b}|^2 + 9|\vec{a} \times \vec{b}|^2$$.
Computing the first term: $$|\vec{a} + 2\vec{b}|^2 = |\vec{a}|^2 + 4\vec{a}\cdot\vec{b} + 4|\vec{b}|^2 = 1 + 4 \cdot \dfrac{1}{2} + 4 = 7$$.
For the cross product magnitude: $$|\vec{a} \times \vec{b}|^2 = |\vec{a}|^2|\vec{b}|^2 - (\vec{a}\cdot\vec{b})^2 = 1 - \dfrac{1}{4} = \dfrac{3}{4}$$.
So $$|\vec{c}|^2 = 7 + 9 \cdot \dfrac{3}{4} = 7 + \dfrac{27}{4} = \dfrac{55}{4}$$, giving $$|\vec{c}| = \dfrac{\sqrt{55}}{2}$$. Therefore $$2|\vec{c}| = \sqrt{55}$$.
Let $$\vec{a}$$, $$\vec{b}$$ and $$\vec{c}$$ be three non-zero vectors such that no two of them are collinear and $$(\vec{a} \times \vec{b}) \times \vec{c} = \frac{1}{3}|\vec{b}||\vec{c}|\vec{a}$$. If $$\theta$$ is the angle between vectors $$\vec{b}$$ and $$\vec{c}$$, then a value of $$\sin \theta$$ is
We are given three non-zero vectors $$\vec{a}$$, $$\vec{b}$$, and $$\vec{c}$$ such that no two are collinear, and the equation $$(\vec{a} \times \vec{b}) \times \vec{c} = \frac{1}{3}|\vec{b}||\vec{c}|\vec{a}$$. We need to find $$\sin \theta$$ where $$\theta$$ is the angle between $$\vec{b}$$ and $$\vec{c}$$.
First, recall the vector triple product identity: $$(\vec{u} \times \vec{v}) \times \vec{w} = (\vec{u} \cdot \vec{w}) \vec{v} - (\vec{v} \cdot \vec{w}) \vec{u}$$. Applying this to the left-hand side with $$\vec{u} = \vec{a}$$, $$\vec{v} = \vec{b}$$, and $$\vec{w} = \vec{c}$$, we get:
$$(\vec{a} \times \vec{b}) \times \vec{c} = (\vec{a} \cdot \vec{c}) \vec{b} - (\vec{b} \cdot \vec{c}) \vec{a}$$
So the given equation becomes:
$$(\vec{a} \cdot \vec{c}) \vec{b} - (\vec{b} \cdot \vec{c}) \vec{a} = \frac{1}{3}|\vec{b}||\vec{c}|\vec{a}$$
Rearrange all terms to one side:
$$(\vec{a} \cdot \vec{c}) \vec{b} - (\vec{b} \cdot \vec{c}) \vec{a} - \frac{1}{3}|\vec{b}||\vec{c}|\vec{a} = 0$$
Combine the terms with $$\vec{a}$$:
$$(\vec{a} \cdot \vec{c}) \vec{b} - \left[ (\vec{b} \cdot \vec{c}) + \frac{1}{3}|\vec{b}||\vec{c}| \right] \vec{a} = 0$$
This can be written as:
$$(\vec{a} \cdot \vec{c}) \vec{b} = \left[ (\vec{b} \cdot \vec{c}) + \frac{1}{3}|\vec{b}||\vec{c}| \right] \vec{a}$$
Since $$\vec{a}$$ and $$\vec{b}$$ are not collinear (as given), they are linearly independent. For this equality to hold, the coefficients must both be zero. Otherwise, if the coefficient of $$\vec{b}$$ is non-zero, $$\vec{b}$$ would be a scalar multiple of $$\vec{a}$$, making them collinear, which contradicts the condition. Similarly, if the coefficient of $$\vec{a}$$ is non-zero, $$\vec{a}$$ would be a scalar multiple of $$\vec{b}$$. Therefore:
$$\vec{a} \cdot \vec{c} = 0 \quad \text{and} \quad (\vec{b} \cdot \vec{c}) + \frac{1}{3}|\vec{b}||\vec{c}| = 0$$
The first equation $$\vec{a} \cdot \vec{c} = 0$$ implies that $$\vec{a}$$ is perpendicular to $$\vec{c}$$.
From the second equation:
$$\vec{b} \cdot \vec{c} = - \frac{1}{3}|\vec{b}||\vec{c}|$$
The dot product $$\vec{b} \cdot \vec{c}$$ is also given by $$|\vec{b}| |\vec{c}| \cos \theta$$, where $$\theta$$ is the angle between $$\vec{b}$$ and $$\vec{c}$$. So:
$$|\vec{b}| |\vec{c}| \cos \theta = - \frac{1}{3}|\vec{b}||\vec{c}|$$
Since $$\vec{b}$$ and $$\vec{c}$$ are non-zero, $$|\vec{b}| \neq 0$$ and $$|\vec{c}| \neq 0$$, so we can divide both sides by $$|\vec{b}| |\vec{c}|$$:
$$\cos \theta = - \frac{1}{3}$$
Now, use the identity $$\sin^2 \theta + \cos^2 \theta = 1$$ to find $$\sin \theta$$:
$$\sin^2 \theta = 1 - \cos^2 \theta = 1 - \left(-\frac{1}{3}\right)^2 = 1 - \frac{1}{9} = \frac{8}{9}$$
Thus:
$$\sin \theta = \pm \sqrt{\frac{8}{9}} = \pm \frac{\sqrt{8}}{3} = \pm \frac{2\sqrt{2}}{3}$$
The angle $$\theta$$ between two vectors ranges from 0 to $$\pi$$ radians (0° to 180°). In this interval, $$\sin \theta$$ is non-negative because sine is positive in the first and second quadrants. Since $$\cos \theta = -1/3 < 0$$, $$\theta$$ is in the second quadrant where sine is positive. Therefore, we take the positive value:
$$\sin \theta = \frac{2\sqrt{2}}{3}$$
Comparing with the options:
A. $$\frac{-2\sqrt{3}}{3}$$
B. $$\frac{2\sqrt{2}}{3}$$
C. $$\frac{-\sqrt{2}}{3}$$
D. $$\frac{2}{3}$$
The value $$\frac{2\sqrt{2}}{3}$$ matches option B.
Hence, the correct answer is Option B.
If $$\begin{bmatrix} \vec{a} \times \vec{b} & \vec{b} \times \vec{c} & \vec{c} \times \vec{a} \end{bmatrix} = \lambda \begin{bmatrix} \vec{a} & \vec{b} & \vec{c} \end{bmatrix}^2$$, then $$\lambda$$ is equal to:
Let us agree on the usual shorthand $$[\,\vec{u}\;\vec{v}\;\vec{w}\,]=\vec{u}\cdot(\vec{v}\times\vec{w})$$; this is the scalar triple product (a single number).
The statement in the question can therefore be rewritten as
$$[\ \vec{a}\times\vec{b}\;\;\vec{b}\times\vec{c}\;\;\vec{c}\times\vec{a}\,]=\lambda\,[\,\vec{a}\;\vec{b}\;\vec{c}\,]^2.$$
We shall evaluate the left-hand scalar triple product step by step.
First put
$$\vec{p}=\vec{a}\times\vec{b},\qquad \vec{q}=\vec{b}\times\vec{c},\qquad \vec{r}=\vec{c}\times\vec{a}.$$
Then the required quantity is simply $$[\,\vec{p}\;\vec{q}\;\vec{r}\,]= \vec{p}\cdot(\vec{q}\times\vec{r}).$$
We begin by finding $$\vec{q}\times\vec{r}=(\vec{b}\times\vec{c})\times(\vec{c}\times\vec{a}).$$
The vector identity for the cross‐product of two cross‐products is
$$(\vec{u}\times\vec{v})\times(\vec{w}\times\vec{x}) =[\,\vec{u}\;\vec{v}\;\vec{x}\,]\,\vec{w}-[\,\vec{u}\;\vec{v}\;\vec{w}\,]\,\vec{x}.$$
Choosing $$\vec{u}=\vec{b},\;\vec{v}=\vec{c},\;\vec{w}=\vec{c},\;\vec{x}=\vec{a},$$ we obtain
$$ (\vec{b}\times\vec{c})\times(\vec{c}\times\vec{a}) =[\,\vec{b}\;\vec{c}\;\vec{a}\,]\,\vec{c}-[\,\vec{b}\;\vec{c}\;\vec{c}\,]\,\vec{a}. $$
Because any scalar triple product containing two identical vectors is zero, the second term vanishes:
$$[\,\vec{b}\;\vec{c}\;\vec{c}\,]=0.$$ Hence
$$\vec{q}\times\vec{r}=(\vec{b}\times\vec{c})\times(\vec{c}\times\vec{a}) =[\,\vec{b}\;\vec{c}\;\vec{a}\,]\,\vec{c}.$$
The scalar triple product is cyclic, so $$[\,\vec{b}\;\vec{c}\;\vec{a}\,]=[\,\vec{a}\;\vec{b}\;\vec{c}\,].$$ Denote this common value by
$$S=[\,\vec{a}\;\vec{b}\;\vec{c}\,].$$
Consequently
$$\vec{q}\times\vec{r}=S\,\vec{c}.$$
Now compute $$\vec{p}\cdot(\vec{q}\times\vec{r}).$$ We have
$$\vec{p}=\vec{a}\times\vec{b},\quad \vec{q}\times\vec{r}=S\,\vec{c},$$ so
$$ \vec{p}\cdot(\vec{q}\times\vec{r}) =(\vec{a}\times\vec{b})\cdot(S\,\vec{c}) =S\,(\vec{a}\times\vec{b})\cdot\vec{c}. $$
The dot product in the last expression is again the scalar triple product of $$\vec{a},\vec{b},\vec{c}$$, namely
$$ (\vec{a}\times\vec{b})\cdot\vec{c}=[\,\vec{a}\;\vec{b}\;\vec{c}\,]=S.$$ Therefore
$$[\,\vec{p}\;\vec{q}\;\vec{r}\,]=S\cdot S=S^{2}=[\,\vec{a}\;\vec{b}\;\vec{c}\,]^{2}.$$
Returning to the original notation, the relation becomes
$$[\,\vec{a}\times\vec{b}\;\;\vec{b}\times\vec{c}\;\;\vec{c}\times\vec{a}\,] =[\,\vec{a}\;\vec{b}\;\vec{c}\,]^{2}.$$
Comparing this with the given equation $$[\,\vec{a}\times\vec{b}\;\;\vec{b}\times\vec{c}\;\;\vec{c}\times\vec{a}\,] =\lambda\,[\,\vec{a}\;\vec{b}\;\vec{c}\,]^{2},$$ we see that
$$\lambda=1.$$
Hence, the correct answer is Option B.
If $$\hat{x}$$, $$\hat{y}$$ and $$\hat{z}$$ are three unit vectors in threedimensional space, then the minimum value of $$|\hat{x} + \hat{y}|^2 + |\hat{y} + \hat{z}|^2 + |\hat{z} + \hat{x}|^2$$
We are given three unit vectors $$\hat{x}$$, $$\hat{y}$$, and $$\hat{z}$$ in three-dimensional space and need to find the minimum value of the expression $$|\hat{x} + \hat{y}|^2 + |\hat{y} + \hat{z}|^2 + |\hat{z} + \hat{x}|^2$$.
First, recall that for any vector $$\vec{a}$$, $$|\vec{a}|^2 = \vec{a} \cdot \vec{a}$$. Using this, expand each term in the expression.
Start with $$|\hat{x} + \hat{y}|^2$$:
$$ |\hat{x} + \hat{y}|^2 = (\hat{x} + \hat{y}) \cdot (\hat{x} + \hat{y}) = \hat{x} \cdot \hat{x} + 2 \hat{x} \cdot \hat{y} + \hat{y} \cdot \hat{y} $$
Since $$\hat{x}$$ and $$\hat{y}$$ are unit vectors, $$\hat{x} \cdot \hat{x} = 1$$ and $$\hat{y} \cdot \hat{y} = 1$$, so:
$$ |\hat{x} + \hat{y}|^2 = 1 + 2 \hat{x} \cdot \hat{y} + 1 = 2 + 2 \hat{x} \cdot \hat{y} $$
Similarly, for $$|\hat{y} + \hat{z}|^2$$:
$$ |\hat{y} + \hat{z}|^2 = (\hat{y} + \hat{z}) \cdot (\hat{y} \cdot \hat{z}) = \hat{y} \cdot \hat{y} + 2 \hat{y} \cdot \hat{z} + \hat{z} \cdot \hat{z} = 1 + 2 \hat{y} \cdot \hat{z} + 1 = 2 + 2 \hat{y} \cdot \hat{z} $$
And for $$|\hat{z} + \hat{x}|^2$$:
$$ |\hat{z} + \hat{x}|^2 = (\hat{z} + \hat{x}) \cdot (\hat{z} + \hat{x}) = \hat{z} \cdot \hat{z} + 2 \hat{z} \cdot \hat{x} + \hat{x} \cdot \hat{x} = 1 + 2 \hat{z} \cdot \hat{x} + 1 = 2 + 2 \hat{z} \cdot \hat{x} $$
Now, sum these expressions:
$$ |\hat{x} + \hat{y}|^2 + |\hat{y} + \hat{z}|^2 + |\hat{z} + \hat{x}|^2 = (2 + 2 \hat{x} \cdot \hat{y}) + (2 + 2 \hat{y} \cdot \hat{z}) + (2 + 2 \hat{z} \cdot \hat{x}) = 6 + 2(\hat{x} \cdot \hat{y} + \hat{y} \cdot \hat{z} + \hat{z} \cdot \hat{x}) $$
Let $$s = \hat{x} \cdot \hat{y} + \hat{y} \cdot \hat{z} + \hat{z} \cdot \hat{x}$$. The expression becomes:
$$ 6 + 2s $$
To minimize the entire expression, minimize $$s$$. Since $$\hat{x}$$, $$\hat{y}$$, and $$\hat{z}$$ are unit vectors, the dot products equal the cosines of the angles between them:
$$ \hat{x} \cdot \hat{y} = \cos \theta_{xy}, \quad \hat{y} \cdot \hat{z} = \cos \theta_{yz}, \quad \hat{z} \cdot \hat{x} = \cos \theta_{zx} $$
So, $$s = \cos \theta_{xy} + \cos \theta_{yz} + \cos \theta_{zx}$$.
Consider the magnitude of the sum $$\hat{x} + \hat{y} + \hat{z}$$:
$$ |\hat{x} + \hat{y} + \hat{z}|^2 = (\hat{x} + \hat{y} + \hat{z}) \cdot (\hat{x} + \hat{y} + \hat{z}) = \hat{x} \cdot \hat{x} + \hat{y} \cdot \hat{y} + \hat{z} \cdot \hat{z} + 2(\hat{x} \cdot \hat{y} + \hat{y} \cdot \hat{z} + \hat{z} \cdot \hat{x}) = 3 + 2s $$
Since $$|\hat{x} + \hat{y} + \hat{z}|^2 \geq 0$$, we have:
$$ 3 + 2s \geq 0 \quad \Rightarrow \quad s \geq -\frac{3}{2} $$
The minimum value of $$s$$ is $$-\frac{3}{2}$$, achieved when $$|\hat{x} + \hat{y} + \hat{z}|^2 = 0$$, meaning $$\hat{x} + \hat{y} + \hat{z} = \vec{0}$$. This occurs when the vectors are coplanar and equally spaced at 120 degrees to each other.
For example, take:
$$ \hat{x} = (1, 0, 0), \quad \hat{y} = \left(-\frac{1}{2}, \frac{\sqrt{3}}{2}, 0\right), \quad \hat{z} = \left(-\frac{1}{2}, -\frac{\sqrt{3}}{2}, 0\right) $$
Verify these are unit vectors:
Magnitude of $$\hat{y}$$: $$\sqrt{\left(-\frac{1}{2}\right)^2 + \left(\frac{\sqrt{3}}{2}\right)^2} = \sqrt{\frac{1}{4} + \frac{3}{4}} = \sqrt{1} = 1$$, similarly for $$\hat{z}$$.
Compute dot products:
$$ \hat{x} \cdot \hat{y} = (1)\left(-\frac{1}{2}\right) + (0)\left(\frac{\sqrt{3}}{2}\right) = -\frac{1}{2} $$
$$ \hat{y} \cdot \hat{z} = \left(-\frac{1}{2}\right)\left(-\frac{1}{2}\right) + \left(\frac{\sqrt{3}}{2}\right)\left(-\frac{\sqrt{3}}{2}\right) = \frac{1}{4} - \frac{3}{4} = -\frac{1}{2} $$
$$ \hat{z} \cdot \hat{x} = \left(-\frac{1}{2}\right)(1) + \left(-\frac{\sqrt{3}}{2}\right)(0) = -\frac{1}{2} $$
So, $$s = -\frac{1}{2} + (-\frac{1}{2}) + (-\frac{1}{2}) = -\frac{3}{2}$$.
Substitute $$s = -\frac{3}{2}$$ into the expression:
$$ 6 + 2s = 6 + 2\left(-\frac{3}{2}\right) = 6 - 3 = 3 $$
Verify with the example vectors:
$$ \hat{x} + \hat{y} = \left(1 - \frac{1}{2}, 0 + \frac{\sqrt{3}}{2}, 0\right) = \left(\frac{1}{2}, \frac{\sqrt{3}}{2}, 0\right), \quad |\hat{x} + \hat{y}|^2 = \left(\frac{1}{2}\right)^2 + \left(\frac{\sqrt{3}}{2}\right)^2 = \frac{1}{4} + \frac{3}{4} = 1 $$
$$ \hat{y} + \hat{z} = \left(-\frac{1}{2} - \frac{1}{2}, \frac{\sqrt{3}}{2} - \frac{\sqrt{3}}{2}, 0\right) = (-1, 0, 0), \quad |\hat{y} + \hat{z}|^2 = (-1)^2 = 1 $$
$$ \hat{z} + \hat{x} = \left(-\frac{1}{2} + 1, -\frac{\sqrt{3}}{2} + 0, 0\right) = \left(\frac{1}{2}, -\frac{\sqrt{3}}{2}, 0\right), \quad |\hat{z} + \hat{x}|^2 = \left(\frac{1}{2}\right)^2 + \left(-\frac{\sqrt{3}}{2}\right)^2 = \frac{1}{4} + \frac{3}{4} = 1 $$
Sum: $$1 + 1 + 1 = 3$$.
Since $$s \geq -\frac{3}{2}$$, the expression $$6 + 2s \geq 6 + 2(-\frac{3}{2}) = 3$$, and we achieved 3, it is the minimum.
Hence, the correct answer is Option B.
If $$|\vec{a}| = 2$$, $$|\vec{b}| = 3$$ and $$|2\vec{a} - \vec{b}| = 5$$, then $$|2\vec{a} + \vec{b}|$$ equals:
We are given the magnitudes of vectors $$\vec{a}$$ and $$\vec{b}$$: $$|\vec{a}| = 2$$ and $$|\vec{b}| = 3$$. Also, the magnitude of $$2\vec{a} - \vec{b}$$ is given as $$|2\vec{a} - \vec{b}| = 5$$. We need to find the magnitude of $$|2\vec{a} + \vec{b}|$$.
Recall that for any vector $$\vec{v}$$, the square of its magnitude is equal to the dot product of the vector with itself: $$|\vec{v}|^2 = \vec{v} \cdot \vec{v}$$. We can use this property to solve the problem.
First, consider the given $$|2\vec{a} - \vec{b}| = 5$$. Squaring both sides gives: $$|2\vec{a} - \vec{b}|^2 = 5^2 = 25.$$
Now, expand the left side using the dot product: $$(2\vec{a} - \vec{b}) \cdot (2\vec{a} - \vec{b}) = (2\vec{a}) \cdot (2\vec{a}) - (2\vec{a}) \cdot \vec{b} - \vec{b} \cdot (2\vec{a}) + (-\vec{b}) \cdot (-\vec{b}).$$
Simplify this expression. Since the dot product is commutative and distributive, we have: $$(2\vec{a}) \cdot (2\vec{a}) = 4 (\vec{a} \cdot \vec{a}) = 4 |\vec{a}|^2,$$ $$(-\vec{b}) \cdot (-\vec{b}) = \vec{b} \cdot \vec{b} = |\vec{b}|^2,$$ and the cross terms: $$-(2\vec{a}) \cdot \vec{b} - \vec{b} \cdot (2\vec{a}) = -2(\vec{a} \cdot \vec{b}) - 2(\vec{b} \cdot \vec{a}).$$
Since the dot product is commutative, $$\vec{a} \cdot \vec{b} = \vec{b} \cdot \vec{a}$$, so the cross terms become: $$-2(\vec{a} \cdot \vec{b}) - 2(\vec{a} \cdot \vec{b}) = -4(\vec{a} \cdot \vec{b}).$$
Therefore, the expansion is: $$|2\vec{a} - \vec{b}|^2 = 4 |\vec{a}|^2 - 4 (\vec{a} \cdot \vec{b}) + |\vec{b}|^2.$$
Substitute the known magnitudes $$|\vec{a}| = 2$$ and $$|\vec{b}| = 3$$, so $$|\vec{a}|^2 = 4$$ and $$|\vec{b}|^2 = 9$$: $$4 \times 4 - 4 (\vec{a} \cdot \vec{b}) + 9 = 25.$$
Simplify the left side: $$16 - 4 (\vec{a} \cdot \vec{b}) + 9 = 25,$$ $$25 - 4 (\vec{a} \cdot \vec{b}) = 25.$$
Subtract 25 from both sides: $$-4 (\vec{a} \cdot \vec{b}) = 0,$$ so $$\vec{a} \cdot \vec{b} = 0.$$
This means the dot product of $$\vec{a}$$ and $$\vec{b}$$ is zero, indicating that the vectors are perpendicular.
Now, we need to find $$|2\vec{a} + \vec{b}|$$. Square this expression: $$|2\vec{a} + \vec{b}|^2 = (2\vec{a} + \vec{b}) \cdot (2\vec{a} + \vec{b}).$$
Expand the dot product: $$(2\vec{a}) \cdot (2\vec{a}) + (2\vec{a}) \cdot \vec{b} + \vec{b} \cdot (2\vec{a}) + \vec{b} \cdot \vec{b}.$$
Simplify each term: $$(2\vec{a}) \cdot (2\vec{a}) = 4 (\vec{a} \cdot \vec{a}) = 4 |\vec{a}|^2,$$ $$\vec{b} \cdot \vec{b} = |\vec{b}|^2,$$ and the cross terms: $$(2\vec{a}) \cdot \vec{b} + \vec{b} \cdot (2\vec{a}) = 2(\vec{a} \cdot \vec{b}) + 2(\vec{a} \cdot \vec{b}) = 4(\vec{a} \cdot \vec{b}),$$ since the dot product is commutative.
So, $$|2\vec{a} + \vec{b}|^2 = 4 |\vec{a}|^2 + 4 (\vec{a} \cdot \vec{b}) + |\vec{b}|^2.$$
Substitute the values $$|\vec{a}|^2 = 4$$, $$|\vec{b}|^2 = 9$$, and $$\vec{a} \cdot \vec{b} = 0$$: $$4 \times 4 + 4 \times 0 + 9 = 16 + 0 + 9 = 25.$$
Therefore, $$|2\vec{a} + \vec{b}| = \sqrt{25} = 5.$$
Hence, the correct answer is Option A.
If $$|\vec{c}|^2 = 60$$ and $$\vec{c} \times (\hat{i} + 2\hat{j} + 5\hat{k}) = \vec{0}$$, then a value of $$\vec{c} \cdot (-7\hat{i} + 2\hat{j} + 3\hat{k})$$ is:
We are given two conditions: $$|\vec{c}|^2 = 60$$ and $$\vec{c} \times (\hat{i} + 2\hat{j} + 5\hat{k}) = \vec{0}$$. We need to find $$\vec{c} \cdot (-7\hat{i} + 2\hat{j} + 3\hat{k})$$.
First, since the cross product $$\vec{c} \times (\hat{i} + 2\hat{j} + 5\hat{k}) = \vec{0}$$, the vectors $$\vec{c}$$ and $$\hat{i} + 2\hat{j} + 5\hat{k}$$ are parallel. Therefore, $$\vec{c}$$ is a scalar multiple of $$\hat{i} + 2\hat{j} + 5\hat{k}$$. Let $$\vec{c} = k (\hat{i} + 2\hat{j} + 5\hat{k})$$, where $$k$$ is a scalar. So, $$\vec{c} = k\hat{i} + 2k\hat{j} + 5k\hat{k}$$.
Now, we know $$|\vec{c}|^2 = 60$$. The magnitude squared is the dot product of $$\vec{c}$$ with itself:
$$|\vec{c}|^2 = \vec{c} \cdot \vec{c} = (k\hat{i} + 2k\hat{j} + 5k\hat{k}) \cdot (k\hat{i} + 2k\hat{j} + 5k\hat{k}) = k \cdot k + (2k) \cdot (2k) + (5k) \cdot (5k) = k^2 + 4k^2 + 25k^2 = 30k^2.$$
Given $$|\vec{c}|^2 = 60$$, we have:
$$30k^2 = 60.$$
Dividing both sides by 30:
$$k^2 = 2.$$
So, $$k = \sqrt{2}$$ or $$k = -\sqrt{2}$$.
Next, we compute $$\vec{c} \cdot (-7\hat{i} + 2\hat{j} + 3\hat{k})$$. Let $$\vec{d} = -7\hat{i} + 2\hat{j} + 3\hat{k}$$. Then:
$$\vec{c} \cdot \vec{d} = (k\hat{i} + 2k\hat{j} + 5k\hat{k}) \cdot (-7\hat{i} + 2\hat{j} + 3\hat{k}).$$
The dot product is:
$$(k) \cdot (-7) + (2k) \cdot (2) + (5k) \cdot (3) = -7k + 4k + 15k.$$
Combining like terms:
$$-7k + 4k = -3k,$$
$$-3k + 15k = 12k.$$
So, $$\vec{c} \cdot \vec{d} = 12k$$.
Substituting the values of $$k$$:
If $$k = \sqrt{2}$$, then $$\vec{c} \cdot \vec{d} = 12 \cdot \sqrt{2} = 12\sqrt{2}$$.
If $$k = -\sqrt{2}$$, then $$\vec{c} \cdot \vec{d} = 12 \cdot (-\sqrt{2}) = -12\sqrt{2}$$.
The problem asks for "a value" of the dot product. The options provided are:
A. $$4\sqrt{2}$$
B. 12
C. 24
D. $$12\sqrt{2}$$
Among the possible values, $$12\sqrt{2}$$ is present in the options as choice D. The value $$-12\sqrt{2}$$ is not listed. Therefore, we select $$12\sqrt{2}$$.
Hence, the correct answer is Option D.
If $$\vec{x} = 3\hat{i} - 6\hat{j} - \hat{k}$$, $$\vec{y} = \hat{i} + 4\hat{j} - 3\hat{k}$$ and $$\vec{z} = 3\hat{i} - 4\hat{j} - 12\hat{k}$$, then the magnitude of the projection of $$\vec{x} \times \vec{y}$$ on $$\vec{z}$$ is:
We are given three vectors:
$$\vec{x} = 3\hat{i} - 6\hat{j} - \hat{k}$$
$$\vec{y} = \hat{i} + 4\hat{j} - 3\hat{k}$$
$$\vec{z} = 3\hat{i} - 4\hat{j} - 12\hat{k}$$
We need to find the magnitude of the projection of $$\vec{x} \times \vec{y}$$ onto $$\vec{z}$$. The magnitude of the projection of a vector $$\vec{a}$$ onto a vector $$\vec{b}$$ is given by $$\frac{| \vec{a} \cdot \vec{b} |}{|\vec{b}|}$$. Here, $$\vec{a} = \vec{x} \times \vec{y}$$ and $$\vec{b} = \vec{z}$$, so the magnitude is $$\frac{| (\vec{x} \times \vec{y}) \cdot \vec{z} |}{|\vec{z}|}$$.
First, compute the cross product $$\vec{x} \times \vec{y}$$. The cross product is found using the determinant formula:
$$\vec{x} \times \vec{y} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 3 & -6 & -1 \\ 1 & 4 & -3 \end{vmatrix}$$
Expanding along the first row:
$$\hat{i} \begin{vmatrix} -6 & -1 \\ 4 & -3 \end{vmatrix} - \hat{j} \begin{vmatrix} 3 & -1 \\ 1 & -3 \end{vmatrix} + \hat{k} \begin{vmatrix} 3 & -6 \\ 1 & 4 \end{vmatrix}$$
Compute each 2x2 determinant:
- For $$\hat{i}$$: $$(-6)(-3) - (-1)(4) = 18 - (-4) = 18 + 4 = 22$$
- For $$\hat{j}$$: $$(3)(-3) - (-1)(1) = -9 - (-1) = -9 + 1 = -8$$, and with the negative sign from expansion, it becomes $$-(-8) = 8$$
- For $$\hat{k}$$: $$(3)(4) - (-6)(1) = 12 - (-6) = 12 + 6 = 18$$
So, $$\vec{x} \times \vec{y} = 22\hat{i} + 8\hat{j} + 18\hat{k}$$
Next, compute the dot product of $$\vec{x} \times \vec{y}$$ and $$\vec{z}$$:
$$(\vec{x} \times \vec{y}) \cdot \vec{z} = (22)(3) + (8)(-4) + (18)(-12)$$
Calculate step by step:
$$22 \times 3 = 66$$
$$8 \times (-4) = -32$$
$$18 \times (-12) = -216$$
Adding these: $$66 + (-32) + (-216) = 66 - 32 - 216 = 34 - 216 = -182$$
So, $$(\vec{x} \times \vec{y}) \cdot \vec{z} = -182$$
Now, find the magnitude of $$\vec{z}$$:
$$|\vec{z}| = \sqrt{(3)^2 + (-4)^2 + (-12)^2} = \sqrt{9 + 16 + 144} = \sqrt{169} = 13$$
The magnitude of the projection is:
$$\frac{| (\vec{x} \times \vec{y}) \cdot \vec{z} |}{|\vec{z}|} = \frac{|-182|}{13} = \frac{182}{13}$$
Dividing: $$182 \div 13 = 14$$, since $$13 \times 14 = 182$$.
Therefore, the magnitude is 14.
Hence, the correct answer is Option A.
Let $$\vec{a} = 2\hat{i} + \hat{j} - 2\hat{k}$$, $$\vec{b} = \hat{i} + \hat{j}$$. If $$\vec{c}$$ is a vector such that $$\vec{a} \cdot \vec{c} = |\vec{c}|$$, $$|\vec{c} - \vec{a}| = 2\sqrt{2}$$ and the angle between $$\vec{a} \times \vec{b}$$ and $$\vec{c}$$ is 30°, then $$|(\vec{a} \times \vec{b}) \times \vec{c}|$$ equals:
Given vectors are $$\vec{a} = 2\hat{i} + \hat{j} - 2\hat{k}$$ and $$\vec{b} = \hat{i} + \hat{j}$$. We need to find $$|(\vec{a} \times \vec{b}) \times \vec{c}|$$ where $$\vec{c}$$ satisfies three conditions: $$\vec{a} \cdot \vec{c} = |\vec{c}|$$, $$|\vec{c} - \vec{a}| = 2\sqrt{2}$$, and the angle between $$\vec{a} \times \vec{b}$$ and $$\vec{c}$$ is 30°.
First, compute $$\vec{a} \times \vec{b}$$. The cross product is found using the determinant formula:
$$\vec{a} \times \vec{b} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 1 & -2 \\ 1 & 1 & 0 \\ \end{vmatrix}$$
Expanding along the first row:
$$\hat{i} \left( (1)(0) - (-2)(1) \right) - \hat{j} \left( (2)(0) - (-2)(1) \right) + \hat{k} \left( (2)(1) - (1)(1) \right)$$
Calculate each component:
For $$\hat{i}$$: $$1 \cdot 0 - (-2) \cdot 1 = 0 + 2 = 2$$, so $$2\hat{i}$$.
For $$\hat{j}$$: minus sign, then $$2 \cdot 0 - (-2) \cdot 1 = 0 + 2 = 2$$, so $$-2\hat{j}$$.
For $$\hat{k}$$: $$2 \cdot 1 - 1 \cdot 1 = 2 - 1 = 1$$, so $$1\hat{k}$$.
Thus, $$\vec{a} \times \vec{b} = 2\hat{i} - 2\hat{j} + \hat{k}$$.
Now, find its magnitude:
$$|\vec{a} \times \vec{b}| = \sqrt{(2)^2 + (-2)^2 + (1)^2} = \sqrt{4 + 4 + 1} = \sqrt{9} = 3.$$
Denote $$\vec{d} = \vec{a} \times \vec{b}$$, so $$|\vec{d}| = 3$$.
The magnitude $$|(\vec{a} \times \vec{b}) \times \vec{c}| = |\vec{d} \times \vec{c}|$$. The magnitude of the cross product is given by $$|\vec{d} \times \vec{c}| = |\vec{d}| |\vec{c}| \sin \theta$$, where $$\theta$$ is the angle between $$\vec{d}$$ and $$\vec{c}$$. Given $$\theta = 30^\circ$$, $$\sin 30^\circ = \frac{1}{2}$$, so:
$$|\vec{d} \times \vec{c}| = 3 \cdot |\vec{c}| \cdot \frac{1}{2} = \frac{3}{2} |\vec{c}|.$$
To find $$|(\vec{a} \times \vec{b}) \times \vec{c}|$$, we need $$|\vec{c}|$$. Use the conditions $$\vec{a} \cdot \vec{c} = |\vec{c}|$$ and $$|\vec{c} - \vec{a}| = 2\sqrt{2}$$.
Let $$|\vec{c}| = c$$, so $$\vec{a} \cdot \vec{c} = c$$.
Compute $$|\vec{a}|^2$$:
$$|\vec{a}|^2 = (2)^2 + (1)^2 + (-2)^2 = 4 + 1 + 4 = 9.$$
Now, $$|\vec{c} - \vec{a}| = 2\sqrt{2}$$, so $$|\vec{c} - \vec{a}|^2 = (2\sqrt{2})^2 = 8$$.
Expand the magnitude squared:
$$|\vec{c} - \vec{a}|^2 = (\vec{c} - \vec{a}) \cdot (\vec{c} - \vec{a}) = \vec{c} \cdot \vec{c} - 2 \vec{a} \cdot \vec{c} + \vec{a} \cdot \vec{a} = |\vec{c}|^2 - 2 (\vec{a} \cdot \vec{c}) + |\vec{a}|^2.$$
Substitute known values:
$$c^2 - 2(c) + 9 = 8.$$
Simplify:
$$c^2 - 2c + 9 - 8 = 0 \implies c^2 - 2c + 1 = 0.$$
Factor:
$$(c - 1)^2 = 0 \implies c = 1.$$
Thus, $$|\vec{c}| = 1$$.
Now substitute back:
$$|\vec{d} \times \vec{c}| = \frac{3}{2} \cdot 1 = \frac{3}{2}.$$
Therefore, $$|(\vec{a} \times \vec{b}) \times \vec{c}| = \frac{3}{2}$$.
Hence, the correct answer is Option D.
Let $$\vec{a} = 2\hat{i} - \hat{j} + \hat{k}$$, $$\vec{b} = \hat{i} + 2\hat{j} - \hat{k}$$ and $$\vec{c} = \hat{i} + \hat{j} - 2\hat{k}$$ be three vectors. A vector of the type $$\vec{b} + \lambda\vec{c}$$ for some scalar $$\lambda$$, whose projection on $$\vec{a}$$ is of magnitude $$\sqrt{\frac{2}{3}}$$ is :
We are given three vectors: $$\vec{a} = 2\hat{i} - \hat{j} + \hat{k}$$, $$\vec{b} = \hat{i} + 2\hat{j} - \hat{k}$$, and $$\vec{c} = \hat{i} + \hat{j} - 2\hat{k}$$. We need to find a vector of the form $$\vec{b} + \lambda\vec{c}$$ for some scalar $$\lambda$$ such that the magnitude of its projection on $$\vec{a}$$ is $$\sqrt{\frac{2}{3}}$$.
The projection of a vector $$\vec{u}$$ onto $$\vec{a}$$ is given by $$\frac{\vec{u} \cdot \vec{a}}{|\vec{a}|}$$, and its magnitude is $$\left| \frac{\vec{u} \cdot \vec{a}}{|\vec{a}|} \right|$$. Here, $$\vec{u} = \vec{b} + \lambda\vec{c}$$, so we set up the equation:
$$\left| \frac{(\vec{b} + \lambda\vec{c}) \cdot \vec{a}}{|\vec{a}|} \right| = \sqrt{\frac{2}{3}}$$
Expanding the dot product:
$$\left| \frac{\vec{b} \cdot \vec{a} + \lambda (\vec{c} \cdot \vec{a})}{|\vec{a}|} \right| = \sqrt{\frac{2}{3}}$$
First, compute the dot products and the magnitude of $$\vec{a}$$.
Calculate $$\vec{a} \cdot \vec{b}$$:
$$\vec{a} \cdot \vec{b} = (2)(1) + (-1)(2) + (1)(-1) = 2 - 2 - 1 = -1$$
Calculate $$\vec{a} \cdot \vec{c}$$:
$$\vec{a} \cdot \vec{c} = (2)(1) + (-1)(1) + (1)(-2) = 2 - 1 - 2 = -1$$
Calculate $$|\vec{a}|$$:
$$|\vec{a}| = \sqrt{(2)^2 + (-1)^2 + (1)^2} = \sqrt{4 + 1 + 1} = \sqrt{6}$$
Substitute these values into the equation:
$$\left| \frac{-1 + \lambda (-1)}{\sqrt{6}} \right| = \sqrt{\frac{2}{3}}$$
Simplify the numerator:
$$\left| \frac{-1 - \lambda}{\sqrt{6}} \right| = \sqrt{\frac{2}{3}}$$
Since the absolute value, we can write:
$$\frac{| -1 - \lambda |}{\sqrt{6}} = \sqrt{\frac{2}{3}}$$
Note that $$| -1 - \lambda | = | -(1 + \lambda) | = |1 + \lambda|$$, so:
$$\frac{|1 + \lambda|}{\sqrt{6}} = \sqrt{\frac{2}{3}}$$
Multiply both sides by $$\sqrt{6}$$:
$$|1 + \lambda| = \sqrt{6} \cdot \sqrt{\frac{2}{3}}$$
Simplify the right side:
$$\sqrt{6} \cdot \sqrt{\frac{2}{3}} = \sqrt{6 \cdot \frac{2}{3}} = \sqrt{4} = 2$$
So:
$$|1 + \lambda| = 2$$
This gives two cases:
Case 1: $$1 + \lambda = 2$$, so $$\lambda = 2 - 1 = 1$$
Case 2: $$1 + \lambda = -2$$, so $$\lambda = -2 - 1 = -3$$
Now, form the vector $$\vec{b} + \lambda\vec{c}$$ for each $$\lambda$$.
For $$\lambda = 1$$:
$$\vec{b} + \lambda\vec{c} = (\hat{i} + 2\hat{j} - \hat{k}) + 1 \cdot (\hat{i} + \hat{j} - 2\hat{k}) = \hat{i} + 2\hat{j} - \hat{k} + \hat{i} + \hat{j} - 2\hat{k} = (1 + 1)\hat{i} + (2 + 1)\hat{j} + (-1 - 2)\hat{k} = 2\hat{i} + 3\hat{j} - 3\hat{k}$$
For $$\lambda = -3$$:
$$\vec{b} + \lambda\vec{c} = (\hat{i} + 2\hat{j} - \hat{k}) + (-3) \cdot (\hat{i} + \hat{j} - 2\hat{k}) = \hat{i} + 2\hat{j} - \hat{k} - 3\hat{i} - 3\hat{j} + 6\hat{k} = (1 - 3)\hat{i} + (2 - 3)\hat{j} + (-1 + 6)\hat{k} = -2\hat{i} - \hat{j} + 5\hat{k}$$
Now, compare these vectors with the given options:
A. $$2\hat{i} + \hat{j} + 5\hat{k}$$
B. $$2\hat{i} + 3\hat{j} - 3\hat{k}$$
C. $$2\hat{i} - \hat{j} + 5\hat{k}$$
D. $$2\hat{i} + 3\hat{j} + 3\hat{k}$$
The vector for $$\lambda = 1$$ is $$2\hat{i} + 3\hat{j} - 3\hat{k}$$, which matches option B.
The vector for $$\lambda = -3$$ is $$-2\hat{i} - \hat{j} + 5\hat{k}$$, which does not match any option.
Verify that the vector for $$\lambda = 1$$ satisfies the projection magnitude condition:
Vector: $$\vec{u} = 2\hat{i} + 3\hat{j} - 3\hat{k}$$
Dot product with $$\vec{a}$$: $$\vec{u} \cdot \vec{a} = (2)(2) + (3)(-1) + (-3)(1) = 4 - 3 - 3 = -2$$
Magnitude of $$\vec{a}$$: $$|\vec{a}| = \sqrt{6}$$
Projection magnitude: $$\left| \frac{-2}{\sqrt{6}} \right| = \frac{2}{\sqrt{6}} = \sqrt{\frac{4}{6}} = \sqrt{\frac{2}{3}}$$, which matches.
Although the vector for $$\lambda = -3$$ also satisfies the condition, it is not listed in the options. Only option B matches one of the solutions and is present in the choices.
Hence, the correct answer is Option B.
If the vectors $$\vec{AB} = 3\hat{i} + 4\hat{k}$$ and $$\vec{AC} = 5\hat{i} - 2\hat{j} + 4\hat{k}$$ are the sides of a triangle $$ABC$$, then the length of the median through $$A$$ is:
We have the two side vectors of the triangle taken from vertex $$A$$:
$$\vec{AB} = 3\hat{i} + 4\hat{k}, \qquad \vec{AC} = 5\hat{i} - 2\hat{j} + 4\hat{k}.$$
The median from a vertex goes to the midpoint of the opposite side. In vector language, the midpoint $$M$$ of the side $$BC$$ is reached by taking the average of the position vectors of $$B$$ and $$C$$ with respect to $$A$$. Hence the vector along the median $$\vec{AM}$$ is one-half of the sum of the two side vectors. Stating the formula,
$$\vec{AM} = \dfrac{1}{2}\left(\vec{AB} + \vec{AC}\right).$$
Now we add the two given vectors term by term:
$$\vec{AB} + \vec{AC} = \bigl(3\hat{i} + 4\hat{k}\bigr) + \bigl(5\hat{i} - 2\hat{j} + 4\hat{k}\bigr) = (3+5)\hat{i} + (0-2)\hat{j} + (4+4)\hat{k}.$$
Simplifying each component we get
$$\vec{AB} + \vec{AC} = 8\hat{i} - 2\hat{j} + 8\hat{k}.$$
Substituting this result in the formula for the median,
$$\vec{AM} = \dfrac{1}{2}\left(8\hat{i} - 2\hat{j} + 8\hat{k}\right) = 4\hat{i} - \hat{j} + 4\hat{k}.$$
To find the length of the median, we need the magnitude of $$\vec{AM}$$. For any vector $$\vec{v}=a\hat{i}+b\hat{j}+c\hat{k}$$, the magnitude formula is
$$|\vec{v}| = \sqrt{a^{2}+b^{2}+c^{2}}.$$
Applying this to $$\vec{AM}=4\hat{i}-\hat{j}+4\hat{k}$$, we calculate
$$|\vec{AM}| = \sqrt{4^{2} + (-1)^{2} + 4^{2}} = \sqrt{16 + 1 + 16} = \sqrt{33}.$$
Thus the length of the median through vertex $$A$$ is $$\sqrt{33}$$.
Hence, the correct answer is Option A.
The vector $$(\hat{i} \times \vec{a} \cdot \vec{b})\hat{i} + (\hat{j} \times \vec{a} \cdot \vec{b})\hat{j} + (\hat{k} \times \vec{a} \cdot \vec{b})\hat{k}$$ is equal to:
The given vector expression is $$ (\hat{i} \times \vec{a} \cdot \vec{b})\hat{i} + (\hat{j} \times \vec{a} \cdot \vec{b})\hat{j} + (\hat{k} \times \vec{a} \cdot \vec{b})\hat{k} $$. Each term involves a cross product followed by a dot product, which is a scalar triple product. Specifically, $$ \hat{i} \times \vec{a} \cdot \vec{b} $$ means $$ (\hat{i} \times \vec{a}) \cdot \vec{b} $$, and by the properties of the scalar triple product, this is equal to $$ \hat{i} \cdot (\vec{a} \times \vec{b}) $$. Similarly, $$ \hat{j} \times \vec{a} \cdot \vec{b} = \hat{j} \cdot (\vec{a} \times \vec{b}) $$ and $$ \hat{k} \times \vec{a} \cdot \vec{b} = \hat{k} \cdot (\vec{a} \times \vec{b}) $$.
Let $$ \vec{c} = \vec{a} \times \vec{b} $$. Then the expression becomes:
$$ (\hat{i} \cdot \vec{c}) \hat{i} + (\hat{j} \cdot \vec{c}) \hat{j} + (\hat{k} \cdot \vec{c}) \hat{k} $$
This is the standard way to express the vector $$ \vec{c} $$ in terms of its components along the Cartesian unit vectors. The component of $$ \vec{c} $$ along $$ \hat{i} $$ is $$ \hat{i} \cdot \vec{c} $$, along $$ \hat{j} $$ is $$ \hat{j} \cdot \vec{c} $$, and along $$ \hat{k} $$ is $$ \hat{k} \cdot \vec{c} $$. Therefore, the entire expression simplifies to $$ \vec{c} $$, which is $$ \vec{a} \times \vec{b} $$.
Now, comparing with the options:
- Option A: $$ \vec{b} \times \vec{a} $$ is the negative of $$ \vec{a} \times \vec{b} $$, so it is not equal.
- Option B: $$ \vec{a} $$ is not necessarily equal to $$ \vec{a} \times \vec{b} $$.
- Option C: $$ \vec{a} \times \vec{b} $$ matches our result.
- Option D: $$ \vec{b} $$ is not necessarily equal to $$ \vec{a} \times \vec{b} $$.
Hence, the correct answer is Option C.
If $$\hat{a}$$, $$\hat{b}$$ and $$\hat{c}$$ are unit vectors satisfying $$\hat{a} - \sqrt{3}\hat{b} + \hat{c} = \vec{0}$$, then the angle between the vectors $$\hat{a}$$ and $$\hat{c}$$ is :
We are given that $$\hat{a}$$, $$\hat{b}$$, and $$\hat{c}$$ are unit vectors, so their magnitudes are all 1. The equation provided is:
$$\hat{a} - \sqrt{3}\hat{b} + \hat{c} = \vec{0}$$
Rearranging this equation, we get:
$$\hat{a} + \hat{c} = \sqrt{3}\hat{b}$$
Since $$\hat{b}$$ is a unit vector, $$|\hat{b}| = 1$$. Therefore, the magnitude of the right side is:
$$|\sqrt{3}\hat{b}| = \sqrt{3} |\hat{b}| = \sqrt{3} \times 1 = \sqrt{3}$$
Thus, the magnitude of the left side must also be $$\sqrt{3}$$:
$$|\hat{a} + \hat{c}| = \sqrt{3}$$
Now, we compute the square of the magnitude of $$\hat{a} + \hat{c}$$:
$$|\hat{a} + \hat{c}|^2 = (\hat{a} + \hat{c}) \cdot (\hat{a} + \hat{c})$$
Expanding the dot product:
$$|\hat{a} + \hat{c}|^2 = \hat{a} \cdot \hat{a} + 2(\hat{a} \cdot \hat{c}) + \hat{c} \cdot \hat{c}$$
Since $$\hat{a}$$ and $$\hat{c}$$ are unit vectors, $$\hat{a} \cdot \hat{a} = |\hat{a}|^2 = 1^2 = 1$$ and $$\hat{c} \cdot \hat{c} = |\hat{c}|^2 = 1^2 = 1$$. Substituting these values:
$$|\hat{a} + \hat{c}|^2 = 1 + 2(\hat{a} \cdot \hat{c}) + 1 = 2 + 2(\hat{a} \cdot \hat{c})$$
But we know that $$|\hat{a} + \hat{c}| = \sqrt{3}$$, so:
$$|\hat{a} + \hat{c}|^2 = (\sqrt{3})^2 = 3$$
Setting the expressions equal:
$$2 + 2(\hat{a} \cdot \hat{c}) = 3$$
Subtracting 2 from both sides:
$$2(\hat{a} \cdot \hat{c}) = 1$$
Dividing both sides by 2:
$$\hat{a} \cdot \hat{c} = \frac{1}{2}$$
The dot product of two vectors is given by the product of their magnitudes and the cosine of the angle between them. Since both are unit vectors:
$$\hat{a} \cdot \hat{c} = |\hat{a}| |\hat{c}| \cos \theta = 1 \times 1 \times \cos \theta = \cos \theta$$
So:
$$\cos \theta = \frac{1}{2}$$
The angle $$\theta$$ between $$\hat{a}$$ and $$\hat{c}$$ that satisfies this in the range $$[0, \pi]$$ is $$\theta = \frac{\pi}{3}$$.
Hence, the angle between the vectors $$\hat{a}$$ and $$\hat{c}$$ is $$\frac{\pi}{3}$$.
Comparing with the options:
A. $$\frac{\pi}{4}$$
B. $$\frac{\pi}{3}$$
C. $$\frac{\pi}{6}$$
D. $$\frac{\pi}{2}$$
So, the correct answer is Option B.
If $$\vec{a}$$ and $$\vec{b}$$ are non-collinear vectors, then the value of $$\alpha$$ for which the vectors $$\vec{u} = (\alpha - 2)\vec{a} + \vec{b}$$ and $$\vec{v} = (2 + 3\alpha)\vec{a} - 3\vec{b}$$ are collinear is :
We are given that $$\vec{a}$$ and $$\vec{b}$$ are non-collinear vectors, meaning they are linearly independent. The vectors are defined as $$\vec{u} = (\alpha - 2)\vec{a} + \vec{b}$$ and $$\vec{v} = (2 + 3\alpha)\vec{a} - 3\vec{b}$$. We need to find the value of $$\alpha$$ such that $$\vec{u}$$ and $$\vec{v}$$ are collinear.
Since $$\vec{u}$$ and $$\vec{v}$$ are collinear, one must be a scalar multiple of the other. Therefore, we can write $$\vec{u} = k \vec{v}$$ for some scalar $$k$$. Substituting the expressions, we get:
$$(\alpha - 2)\vec{a} + \vec{b} = k \left[ (2 + 3\alpha)\vec{a} - 3\vec{b} \right]$$
Expanding the right-hand side:
$$(\alpha - 2)\vec{a} + \vec{b} = k(2 + 3\alpha)\vec{a} - 3k\vec{b}$$
Because $$\vec{a}$$ and $$\vec{b}$$ are linearly independent, the coefficients of $$\vec{a}$$ and $$\vec{b}$$ on both sides must be equal. This gives us two equations:
1. For $$\vec{a}$$: $$\alpha - 2 = k(2 + 3\alpha)$$
2. For $$\vec{b}$$: $$1 = -3k$$
Solving the second equation for $$k$$:
$$1 = -3k \implies k = -\frac{1}{3}$$
Substitute $$k = -\frac{1}{3}$$ into the first equation:
$$\alpha - 2 = \left(-\frac{1}{3}\right)(2 + 3\alpha)$$
Simplify the right-hand side:
$$\alpha - 2 = -\frac{1}{3} \times (2 + 3\alpha) = -\frac{2}{3} - \alpha$$
Now, solve for $$\alpha$$. Add $$\alpha$$ to both sides:
$$\alpha + \alpha - 2 = -\frac{2}{3}$$
$$2\alpha - 2 = -\frac{2}{3}$$
Add 2 to both sides:
$$2\alpha = -\frac{2}{3} + 2$$
$$2\alpha = -\frac{2}{3} + \frac{6}{3} = \frac{4}{3}$$
Divide both sides by 2:
$$\alpha = \frac{4}{3} \times \frac{1}{2} = \frac{4}{6} = \frac{2}{3}$$
Thus, $$\alpha = \frac{2}{3}$$. Now, verifying with the options:
A. $$\frac{3}{2}$$
B. $$\frac{2}{3}$$
C. $$-\frac{3}{2}$$
D. $$-\frac{2}{3}$$
The value $$\alpha = \frac{2}{3}$$ corresponds to option B. To confirm, substitute $$\alpha = \frac{2}{3}$$ into $$\vec{u}$$ and $$\vec{v}$$:
$$\vec{u} = \left(\frac{2}{3} - 2\right)\vec{a} + \vec{b} = \left(-\frac{4}{3}\right)\vec{a} + \vec{b}$$
$$\vec{v} = \left(2 + 3 \times \frac{2}{3}\right)\vec{a} - 3\vec{b} = (2 + 2)\vec{a} - 3\vec{b} = 4\vec{a} - 3\vec{b}$$
Check if $$\vec{u} = k \vec{v}$$ with $$k = -\frac{1}{3}$$:
$$k \vec{v} = -\frac{1}{3} (4\vec{a} - 3\vec{b}) = -\frac{4}{3}\vec{a} + \vec{b} = \vec{u}$$
This holds true, confirming that $$\vec{u}$$ and $$\vec{v}$$ are collinear when $$\alpha = \frac{2}{3}$$.
Hence, the correct answer is Option B.
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