length of the thread
17/ 2 ±(L/2) 2
and the free-fall acceleration
L/2
= g
I /1 2 + (L/2) 2
(^196) Aptitude Test Problems in Physics
where L = AD.
Thus, the required period of small oscillations
of the system is
T =2n17 —7=2n 1/1- —
21
.
g
1.99. In order to solve the problem, it is sufficient
to note that the motion of the swing is a rotation
Fig. 190
about an axis passing through the points where
the ropes are fixed, i.e. the system is a "tilted sim-
ple 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.