(c) Torque about$\ P = - (kx)\frac{L}{2} + \left( - kx\frac{L}{2} \right) = - kxL = - k\frac{L^{2}}{2}\theta$
For small angle $\theta,\ x = \frac{L}{2}\theta;\ \tau = - I\alpha$
[image:14_image64.emf]
$\Rightarrow - \frac{KL^{2}}{2}\theta = \frac{ML^{2}}{12}\alpha$
$\Rightarrow \frac{- 6K\theta}{M} = \alpha$
$\Rightarrow \omega = \sqrt{\frac{6K}{M}}$ and $f = \frac{\omega}{2\pi} = \frac{1}{2\pi}\sqrt{\frac{6K}{M}}$