To solve this problem, we first analyze the forces acting on the body sliding down each incline.
1. Smooth Surface:
Since the surface is smooth, there is no friction. The only forces are the gravitational force parallel to the incline and the normal force.
Gravitational acceleration parallel to the incline: \( g\sin\theta \) where \( \theta= 45^\circ \)
Thus, the acceleration is:
\( a_1 = g\sin\theta = \frac{g}{\sqrt{2}} \)
The formula for time of descent \( t \) on an incline of length \( l \) under constant acceleration \( a \) is given by:
\( t = \sqrt{\frac{2l}{a}} \)
Time taken on smooth surface \( t_1 = \sqrt{\frac{2l}{a_1}} = \sqrt{\frac{2l\sqrt{2}}{g}} \)
2. Rough Surface:
The forces include gravitational force, normal force, and frictional force.
The frictional force \( f_k = \mu_k N = \mu_k mg\cos\theta \)
Net force down the incline: \( mg\sin\theta - f_k = mg\sin\theta - \mu_k mg\cos\theta \)
Net acceleration:
\( a_2 = g(\sin\theta - \mu_k \cos\theta) = g\left(\frac{1}{\sqrt{2}} - \mu_k \frac{1}{\sqrt{2}}\right) \)
\( a_2 = \frac{g}{\sqrt{2}}(1 - \mu_k) \)
Time taken on the rough surface \( t_2 = \sqrt{\frac{2l}{a_2}} = \sqrt{\frac{2l\sqrt{2}}{g(1-\mu_k)}} \)
Condition Given:
Time on rough surface is twice time on smooth surface:
\( t_2 = 2t_1 \)
\( \sqrt{\frac{2l\sqrt{2}}{g(1-\mu_k)}} = 2\sqrt{\frac{2l\sqrt{2}}{g}} \)
Squaring both sides:
\( \frac{2l\sqrt{2}}{g(1-\mu_k)} = 4 \cdot \frac{2l\sqrt{2}}{g} \)
Canceling common terms and simplifying:
\( \frac{1}{1-\mu_k} = 4 \)
\( 1 = 4(1-\mu_k) \)
\( 1 = 4 - 4\mu_k \)
\( 4\mu_k = 3 \)
\( \mu_k = \frac{3}{4} = 0.75 \)
Thus, the coefficient of kinetic friction is approximately \( \mu_k = 0.75 \).