The problem asks for the coefficient of friction ($\mu_s$) required to keep a coin stationary on a horizontally rotating disc. The coin experiences a centripetal force due to the rotation, which must be balanced by the static friction force between the coin and the disc.
For the coin to remain at rest, the static friction force ($f_s$) must provide the necessary centripetal force ($F_c$).
The condition for the coin to remain at rest is $F_c \le f_{s,max}$. For the minimum required coefficient of friction, we consider the case where $F_c = f_{s,max}$.
$ m a_c = \mu_s N $ $ m (\omega^2 r) = \mu_s (mg) $ $ \mu_s = \frac{\omega^2 r}{g} $A thin uniform rod ($X$) of mass $M$ and length $L$ is pivoted at a height $\left(\frac{L}{3}\right)$ as shown in the figure. The rod is allowed to fall from a vertical position and lie horizontally on the table. The angular velocity of this rod when it hits the table top, is __________.
($g = \text{gravitational acceleration}$)

The pulley shown in figure is made using a thin rim and two rods of length equal to diameter of the rim. The rim and each rod have a mass of $M$. Two blocks of mass of $M$ and $m$ are attached to two ends of a light string passing over the pulley, which is hinged to rotate freely in vertical plane about its center. The magnitudes of the acceleration experienced by the blocks is __________
(assume no slipping of string on pulley).
A thin uniform rod ($X$) of mass $M$ and length $L$ is pivoted at a height $\left(\frac{L}{3}\right)$ as shown in the figure. The rod is allowed to fall from a vertical position and lie horizontally on the table. The angular velocity of this rod when it hits the table top, is __________.
($g = \text{gravitational acceleration}$)
