The simple pendulum models a massswinging on a rigid rod of zero mass. In practice of course the mass of the rod is not zero. The compound pendulum takes the non – zero mass of the rod into account.
A compound pendulum consists of a mass( here I will assume it to be a circular disc) attached to the end of a rod of length
and mass
The rod is hung and the rod plus mass is allowed to swing in a vertical plane.
The moment of inertia of the rod about its centre isso the moment of inertia about the pivot at the top is
The moment of inertia of the disc about its centre isso the moment of inertia of the disc about the pivot
from the centre of the disc is
The moment of inertia of the pendulum is then
Now the pendulum can be modelled as a particle with moment of inertiafree to rotate in the vertical plane. If it is displaced an angle
to one side it will experience a restoring torque towards the vertical due to the mass
of
and due to the rod of
so the total restoring torque is
and this will be equal to the the neagive of the product of
and angular acceleration
The negative indicates
and
are in the opposite sense.
Ifis small,
and writing
Which becomes
where
The compound pendulum will execute simple harmonic motion.
We can check the formula by puttingthen
just as for a simple pendulum.