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At some instant, a radioactive sample S$$_1$$ having an activity 5$$\mu$$Ci has twice the number of nuclei as another sample S$$_2$$ which has an activity of 10$$\mu$$Ci. The half lives of S$$_1$$ and S$$_2$$ are:
We begin with the basic law of radioactivity which says that the activity $$A$$ of a sample is directly proportional to the decay constant $$\lambda$$ and to the number of undecayed nuclei $$N$$ present at that instant. Symbolically, the relation is written as
$$A = \lambda N.$$
For the two samples we have:
$$A_1 = \lambda_1 N_1,$$
$$A_2 = \lambda_2 N_2.$$
According to the statement of the problem, the first sample S1 has an activity of $$5\ \mu\text{Ci}$$ and contains twice as many nuclei as the second sample S2, which itself has an activity of $$10\ \mu\text{Ci}.$$ Translating this wording into equations we write
$$A_1 = 5\ \mu\text{Ci}, \qquad A_2 = 10\ \mu\text{Ci},$$
$$N_1 = 2\,N_2.$$
Substituting the values of the activities into the activity formula for each sample we get
$$5 = \lambda_1 N_1,$$
$$10 = \lambda_2 N_2.$$
Next we use the given relation $$N_1 = 2N_2$$ in the first equation. Replacing $$N_1$$ by $$2N_2$$ yields
$$5 = \lambda_1 (2N_2).$$
Simplifying, this becomes
$$5 = 2\lambda_1 N_2.$$
Now we have two simultaneous equations containing the common factor $$N_2$$:
$$5 = 2\lambda_1 N_2,$$
$$10 = \lambda_2 N_2.$$
To eliminate $$N_2$$ we divide the first equation by the second equation term by term:
$$\frac{5}{10} = \frac{2\lambda_1 N_2}{\lambda_2 N_2}.$$
The quantities $$N_2$$ cancel out immediately, giving
$$\frac{1}{2} = \frac{2\lambda_1}{\lambda_2}.$$
Multiplying both sides by $$\lambda_2$$ and then by $$2$$, we obtain
$$\lambda_1 = \frac{1}{4}\,\lambda_2.$$
Thus the ratio of the decay constants is
$$\lambda_1 : \lambda_2 = 1 : 4.$$
We now connect decay constant to half-life. The standard formula relating the two is
$$T_{1/2} = \frac{\ln 2}{\lambda},$$
where $$T_{1/2}$$ is the half-life and $$\ln 2$$ is a constant. Because $$\ln 2$$ is the same for both samples, the half-life is inversely proportional to the decay constant. Therefore
$$\frac{T_{1/2,1}}{T_{1/2,2}} = \frac{\lambda_2}{\lambda_1}.$$
Substituting the ratio $$\lambda_1 : \lambda_2 = 1 : 4$$ into this inverse relation we get
$$\frac{T_{1/2,1}}{T_{1/2,2}} = \frac{4}{1}.$$
Hence the half-life of S1 is four times the half-life of S2, giving the required ratio
$$T_{1/2,1} : T_{1/2,2} = 4 : 1.$$
Hence, the correct answer is Option A.
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