
$\tau=2 k x \frac{L}{2}=2 k \frac{L^{2}}{4} \theta=\frac{k L^{2}}{2} \theta$
Now, $\tau=1 \alpha$
$\frac{\mathrm{kL}^{2}}{2} \theta=\frac{\mathrm{mL}^{2}}{12} \alpha \quad ; \quad \alpha=\frac{6 \mathrm{k}}{\mathrm{m}} \theta$
$\tau=\frac{\omega}{2 \pi}=\frac{1}{2 \pi} \sqrt{\frac{6 k}{m}}$


$ x = 2 \sin \omega t \,;$ $ y = 2 \sin \left( {\omega t + \frac{\pi }{4}} \right)$
The path of the particle will be :
