At the moment of snapping of the right string, the rod is acted upon by the tension T of
the left string and the forces N1 and N2 of normal pressure of the loads of mass m1 and m2 (Fig. 165). Since the rod is weightless (its mass is zero), the
equations of its translatory and rotary motions will have the form
The second equation (the condition of equality to zero of the sum of all moments of force about point O) implies that
N1 = 2N2........(1)
Combining these conditions, we get (see Fig. 165)
T = N1 — N2 = N2..............(2)
At the moment of snapping of the right string, the accelerations of the loads of mass m1 and m2 will be vertical (point O is stationary, and the rod is inextensible) and connected through the relation
a2 = 2a1...............(3)
Let us write the equations of motion for the loads at this instant:
where N'1 and N'2 are the normal reactions of the rod on the loads of mass m1 and m2. Since N'1 = N1 and N'2 = N2, we have
Hence we can find N2, and consequently (see Eq. (2)) the tension of the string