The period of oscillation of a dipole in a uniform electric field is given by the formula: \[ T = 2\pi \sqrt{\frac{I}{PE}} \] Where \(T\) is the period of oscillation, \(I\) is the moment of inertia, \(P\) is the dipole moment, and \(E\) is the electric field. This equation represents simple harmonic motion where the restoring torque is proportional to the angular displacement.
The correct option is (B): \(2\pi\sqrt\frac{1}{PE}\)
For a uniform rectangular sheet shown in the figure, the ratio of moments of inertia about the axes perpendicular to the sheet and passing through \( O \) (the center of mass) and \( O' \) (corner point) is: