We first introduce the coordinates x1 and x2 describing the motion of the blocks. The inertial forces −mixi point in the negative xi-directions (see the freebody diagram). In addition, we have to consider the pseudo moment −ΘAϕ¨ which acts in the negative ϕdirection. Moment equilibrium about point A then yields


Using the kinematic relations

we obtain the angular acceleration of the drum:

In order to determine the force in rope ① we cut the rope. Force equilibrium (see the free-body diagram) yields
↑ : S1 − m1g − m1x1 = 0
or

Note: For r2m2 > r1m1 the drum rotates clockwise, for r2m2 < r1m1 it rotates counterclockwise. In the special case r2m2 = r1m1 the system is in static equilibrium ( ¨ϕ = 0).