An electric dipole of mass $m$, charge $q$, and length $l$ is placed in a uniform electric field $\vec{E} = E_0\hat{i}$. When the dipole is rotated slightly from its equilibrium position and released, the time period of its oscillations will be:
$\frac{1}{2\pi}\sqrt{\frac{m\,l}{2qE_0}}$
$\frac{1}{2\pi}\sqrt{\frac{2m\,l}{qE_0}}$
$2\pi\sqrt{\frac{m\,l}{2qE_0}}$
$2\pi\sqrt{\frac{m\,l}{qE_0}}$