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Two blocks ($$m = 0.5$$ kg and $$M = 4.5$$ kg) are arranged on a horizontal frictionless table as shown in the figure. The coefficient of static friction between the two blocks is $$\frac{3}{7}$$. Then the maximum horizontal force that can be applied on the larger block so that the blocks move together is $$N$$. (Round off to the Nearest Integer) [Take $$g$$ as 9.8 m s$$^{-2}$$]
Correct Answer: 21
We need to determine the maximum horizontal force $$F$$ that can be applied to the larger block so that both blocks continue to move together without relative slipping.
From the layout shown on page, we have:
When the horizontal force $$F$$ is applied to the bottom block $$M$$, the top block $$m$$ moves forward solely due to the static frictional force ($$f_s$$) acting between the two contact surfaces.
The maximum possible static frictional force that can act on block $$m$$ is:
$$f_{\text{max}} = \mu_s \cdot N = \mu_s \cdot mg$$
According to Newton's second law, this maximum frictional force dictates the maximum acceleration ($$a_{\text{max}}$$) the top block can experience without slipping:
$$m \cdot a_{\text{max}} = \mu_s \cdot mg$$
$$a_{\text{max}} = \mu_s \cdot g$$
Substitute the given values into the acceleration equation:
$$a_{\text{max}} = \frac{3}{7} \times 9.8 = 3 \times 1.4 = 4.2\text{ m s}^{-2}$$
For both blocks to move together as a single combined system without relative motion, the entire system of mass ($M + m$) must accelerate at this maximum rate ($a_{\text{max}}$):
$$F = (M + m) \cdot a_{\text{max}}$$
Substitute the masses and the calculated acceleration into the formula:
$$F = (4.5 + 0.5) \times 4.2$$
$$F = 5.0 \times 4.2 = 21\text{ N}$$
The maximum horizontal force that can be applied so that the blocks move together is 21 N.
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