
Given that the velocity of the center of mass (VCM) is:
\( V_{\text{CM}} = 2R \omega \)
At the point of contact, we have:
\( V_{\text{CM}} = \omega_0 R \Rightarrow \omega_0 = 2 \omega \)
Now, the angular momentum of disk B with respect to the center of disk A is calculated as:
\( L = \left( \frac{MR^2}{2} \right) (\omega_0) + M (2R \omega) (2R) \)
Substitute the values of \( \omega_0 \) and simplify:
\( L = \left( \frac{MR^2}{2} \right) (2\omega) + 4MR^2 \omega \)
\( L = 5MR^2 \omega \) and hence, \( n = 5 \).


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: