Let's consider the cylinder is rotating at its place, so that its center of mass has no linear displacement. we are going to discuss here the oscillatory motion about the point of contact.
We can write AO=2R and the angular displacement θ about o is θ , So,
A′A=2Rθ
So, extension in one spring= Contraction in other spring
=Rθ
Here we consider that θ is very small so that extension and compression remain linear.
Now the restoring force acting on spring as well as the cylinder is:
F= force due to both springs
=(k+k)Rθ
⇒F=2kRθ
Moment of this force is=F.2R=4R2θ.k (about point o)
Now the moment of inertia of the cylinder about point of contact is:
I0=IC.M+mR2=12mR2+mR2
⇒I0=32mR2
So the angular torque of the body is:
⇒I0d2θdt2=(32mR2)d2θdt2
So, the equation motion of cylinder:
(32mR2)d2θdt2=−4kR2θ
⇒d2θdt2+(8k3m)θ=0
Angular frequency =ω=√8km
So, Time Period T=2π√m8k=π√m2k