4 Questions around this concept.
Two light identical springs of spring constant k are attached horizontally at the two ends of a uniform horizontal rod AB of length l and mass m. The rod is pivoted at its centre 'O' and can rotate freely in horizontal plane. The other ends of the two springs are fixed to rigid supports as shown in figure. The rod is gently pushed through a small angle and released. The frequency of resulting oscillation is :
The potential energy of a particle of mass 14 Kg in motion along the x-axis is given by of U=8(1 - cos 12 x). the time period of the Particle for small oscillation is
The value of Q
Below is the figure of the Torsional pendulum which consists of a rigid object suspended by a wire attached at the top to a fixed end.

When the object is twisted through some angle $\theta$, the twisted wire exerts on the object a restoring torque and this restoring torque is proportional to the angular position.
That is $\tau=-k \theta$ where $\kappa$ is called the torsion constant of the support wire.
Applying Newton's second law for rotational motion, we find that
$$
\tau=-k \theta=I \frac{d^2 \theta}{d t^2} \Rightarrow \frac{d^2 \theta}{d t^2}=-\frac{k}{I} \theta
$$
So the Time Period of Torsional pendulum is given as
$$
T=2 \pi \sqrt{\frac{I}{k}}
$$
where
$I=$ moment of inertia
$k=$ torsional constant
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