(D) The figure shows the situation given in the question. At the point of contact,the velocity of the smaller drum is $v_1 = R\omega$ (upwards) and the velocity of the larger drum is $v_2 = 2R\omega$ (downwards). Due to this relative velocity,a frictional force $f$ acts on the smaller drum in the downward direction and on the larger drum in the upward direction.
$(b)$ The external forces acting on the system are the normal forces at the contact point and the reaction forces at the fixed axes. Let $F$ be the normal force at the contact point. The reaction forces at the axes are $F'$ and $F$. The net external force on the system is zero. The external torque about the center of the smaller drum is $\tau = F \times 3R$ (anti-clockwise).
$(c)$ Let $\omega_1$ and $\omega_2$ be the final angular velocities of the smaller and larger drum respectively. When friction ceases,there is no relative motion at the point of contact.
Hence,the tangential speeds must be equal: $R\omega_1 = 2R\omega_2$.
Therefore,the ratio of the final angular velocities is $\frac{\omega_1}{\omega_2} = 2$.