Answer:
[tex]f = \frac{1}{2\pi}\sqrt{\frac{(kh^2 + mgL)}{mL^2}}[/tex]
Explanation:
As the pendulum is slightly shifted to the left then we have restoring torque on it given as
[tex]\tau = I \alpha[/tex]
so here we have
[tex]\tau = kx(h) + mg sin\theta L[/tex]
here we know that
[tex]x = h\theta[/tex]
also for small angular displacement
[tex]\tau = kh^2\theta + mgL\theta[/tex]
now we have its moment of inertia about suspension point given as
[tex]I = mL^2[/tex]
now it is given as
[tex]mL^2 \alpha = (kh^2 + mgL)\theta[/tex]
[tex]\alpha = \frac{(kh^2 + mgL)}{mL^2}\theta[/tex]
so we have
[tex]\omega^2 = \frac{(kh^2 + mgL)}{mL^2}[/tex]
so angular frequency is given as
[tex]f = \frac{1}{2\pi}\sqrt{\frac{(kh^2 + mgL)}{mL^2}}[/tex]