The centripetal force is given by $F_c = m\omega^2r$, where:
The maximum static friction is given by $F_f = \mu_s mg$, where:
For the coin to just slip, the centripetal force must equal the maximum static friction:
$m\omega^2r = \mu_s mg$
$\omega^2r = \mu_s g$
Since $\mu_s$ and $g$ are constant, we can say that $\omega^2r$ is constant.
Initially, the coin slips at $r_1 = 4$ cm with angular velocity $\omega_1$. When the angular velocity is doubled ($\omega_2 = 2\omega_1$), let the distance at which it slips be $r_2$. Since $\omega^2r$ is constant, we have:
$\omega_1^2 r_1 = \omega_2^2 r_2$
$\omega_1^2 (4\,\text{cm}) = (2\omega_1)^2 r_2$
$4\omega_1^2 = 4\omega_1^2 r_2$
$r_2 = 1$ cm
The correct answer is (A) 1 cm.
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.