When a ring rolls on a rough surface, the frictional force acts to reduce its angular velocity.
The equation for the angular deceleration \( \alpha \) due to friction is given by:
\[
f = \mu mg
\]
where \( m \) is the mass of the ring and \( g \) is the acceleration due to gravity.
The torque \( \tau \) due to the friction is:
\[
\tau = fR = \mu mgR
\]
The angular acceleration \( \alpha \) is given by:
\[
\tau = I \alpha
\]
where \( I \) is the moment of inertia of the ring.
For a ring, \( I = mR^2 \), so:
\[
\mu mgR = mR^2 \alpha
\]
Simplifying:
\[
\alpha = \frac{\mu g}{R}
\]
Now, to reduce the angular velocity to half, we use the equation:
\[
\omega_f = \omega_0 + \alpha t
\]
Substituting \( \omega_f = \frac{\omega_0}{2} \), we get:
\[
\frac{\omega_0}{2} = \omega_0 - \frac{\mu g}{R} t
\]
Solving for \( t \):
\[
t = \frac{\omega_0 R}{\mu g}
\]
Thus, the correct answer is (b).