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Q. An electric dipole is situated in an electric field of uniform intensity $E$ whose dipole moment is $p$ and moment of inertia is $I$. If the dipole is displaced slightly from the equilibrium position, then the angular frequency of its oscillations is

Electrostatic Potential and Capacitance

Solution:

When dipole is given a small angular displacement $\theta$ about its equilibrium position, the restoring torque will be
$\tau = -pE sin\theta $(as $ sin\theta = \theta)$
or $I \frac{d^2\theta}{dt^2} = - pE \theta $( as $\tau = I\alpha = I \frac{d^2\theta}{dt^2})$
or $\frac{d^2\theta}{dt^2} = -\omega^2 \theta$ with $\omega^2 = \frac{pE}{I} $
$\Rightarrow \omega = \sqrt{\frac{pE}{I}}$