Let us suppose that at a certain instant, the wheel is in one of the positions such that its centre of mass is above a rod, and its velocity is v. At the moment of the impact against the next rod (Fig. 171), the centre of mass of the wheel has a
certain velocity v' perpendicular to the line connecting it to the previous rod. This velocity can be obtained from the energy conservation law:
By hypothesis (the motion is without jumps), the impact of the wheel against the rod is perfectly inelastic. This means that during the impact, the projection of the momentum of the wheel on the straight line connecting the centre of the wheel to the rod vanishes. Thus, during each collision, the energy
where sin α ≈ l/r, is lost (converted into heat). For the velocity v to remain constant, the work done by the tension T of the rope over the path l must compensate for this energy loss. Therefore,