For the smooth inclined plane, the acceleration is:
\[a_{\text{smooth}} = g \sin 45^\circ = \frac{g}{\sqrt{2}}.\]
For the rough inclined plane, the acceleration is:
\[a_{\text{rough}} = g (\sin 45^\circ - \mu_k \cos 45^\circ) = \frac{g}{\sqrt{2}} (1 - \mu_k).\]
The time taken is inversely proportional to the square root of acceleration:
\[t_{\text{rough}} = n \cdot t_{\text{smooth}} \implies \sqrt{\frac{a_{\text{smooth}}}{a_{\text{rough}}}} = n.\]
Substituting:
\[\sqrt{\frac{\frac{g}{\sqrt{2}}}{\frac{g}{\sqrt{2}} (1 - \mu_k)}} = n.\]
Simplify:
\[\sqrt{\frac{1}{1 - \mu_k}} = n \implies 1 - \mu_k = \frac{1}{n^2}.\]
Solving for \(\mu_k\):
\[\mu_k = 1 - \frac{1}{n^2}.\]
Thus, the coefficient of kinetic friction is:
\[\mu_k = 1 - \frac{1}{n^2}.\]
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: