In order to solve the problem, it is sufficient to note that the motion of the swing is a rotation about an axis passing through the points where the ropes are fixed, i.e. the system is a "tilted simple pendulum" (Fig. 190).
The component of the force of gravity mg along the rotational axis does not influence the oscillations, while the normal component mg sin a is in fact the restoring force.
Therefore, using the formula for the ** of a simple pendulum, we can write
Consequently, the ** of small oscillations of the swing is