
By impulse – momentum theorem: \( J = M V_{CM} \)
Therefore, the center of mass velocity \( V_{CM} \) is: \[ V_{CM} = \frac{J}{M} = \frac{\frac{\pi}{2}}{100 \times \frac{5}{1000}} = \sqrt{2\pi} \]
The total time of the journey is: \[ \Delta t = \frac{\sqrt{2\pi}}{5} \]
By the angular impulse-momentum theorem: \[ J \times \frac{R}{2} = \left[\frac{M R^2}{4}\right] w \]
Solving for the angular velocity \( w \): \[ w = \frac{J \times \frac{R}{2}}{\frac{M R^2}{4}} = \frac{J}{M R} \times 2 \]
Substituting the known values: \[ w = \frac{\frac{\frac{\sqrt{\pi}}{2}}{100} \times 2}{\frac{5}{1000} \times \frac{4}{3} \times \frac{1}{100}} = 2 \times 75 \sqrt{2\pi} \, \text{rad/s} \]
The number of rotations is: \[ n = \frac{w \times \Delta t}{2\pi} = 30 \]
Therefore, the final result is: \[ n = 30 \]


Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: