As long as the load touches the body, the velocity of the latter is equal to the horizontal component of the velocity of the load, and the acceleration of the body is equal to the horizontal component of the acceleration of the load.
Let a be the total acceleration of the load. Then we can write a = at + ac, where ac is the centripetal acceleration of the load moving in the circle of radius l, i.e., ac = v2/l, where v is the velocity of the load (Fig. 154). The horizontal component of the acceleration is

The body also has the same acceleration. We can write the equation of motion for the body:

where N is the force of normal pressure exerted

by the load on the body. At the moment of separation of the load, N = 0 and

The acceleration component at at the moment of separation of the load is only due to the force of gravity:

Thus, the velocity of the load at the moment of separation is

and the velocity of the body at the same moment is

According to the energy conservation law, we have

Substituting the obtained expression for v at the moment of separation and the value of sin α = sin pi/6 = 1/2 into this equation, we obtain the ratio:

The velocity of the body at the moment of separation is
