Concept:
Moment of inertia of a solid sphere about diameter:
\[
I = \frac{2}{5}MR^2
\]
Torque relation:
\[
\tau = I\alpha
\]
Rotational kinematics:
\[
\omega_f = \omega_i + \alpha t
\]
Step 1: Convert angular speed to rad/s.}
\[
\omega_i = 1200\,rpm
\]
\[
\omega_i = 1200 \times \frac{2\pi}{60}
\]
\[
\omega_i = 40\pi \,rad/s
\]
Step 2: Find angular acceleration.}
Final angular velocity
\[
\omega_f = 0
\]
\[
0 = 40\pi + \alpha(10)
\]
\[
\alpha = -4\pi \,rad/s^2
\]
Step 3: Find moment of inertia.}
\[
R = 4\,cm = 0.04\,m
\]
\[
I = \frac{2}{5}(5)(0.04)^2
\]
\[
I = 2 \times 0.0016
\]
\[
I = 0.0032\,kg\,m^2
\]
Step 4: Calculate torque.}
\[
\tau = I\alpha
\]
\[
\tau = 0.0032 \times 4\pi
\]
\[
\tau \approx 0.04\,N-m
\]
Step 5: Find angular displacement.}
\[
\omega_f^2 = \omega_i^2 + 2\alpha\theta
\]
\[
0 = (40\pi)^2 + 2(-4\pi)\theta
\]
\[
\theta = 200\pi
\]
Number of revolutions:
\[
n = \frac{\theta}{2\pi}
\]
\[
n = \frac{200\pi}{2\pi}
\]
\[
n = 100
\]
Final Result
\[
\tau = 0.04\,N-m, \quad n = 100
\]