A charge q is uniformly distributed over a disc of radius R. A circular hole of radius R/2 is punched out, taking one radius of the original disc as the diameter of the hole. The potential at the centre of the original disc due to the remaining part is nV₀, where V₀ = [q/(2πε₀R)](1 − 1/π). Find n.
Physics · Electrostatic
A charge q is uniformly distributed over a disc of radius R. A circular hole of radius R/2 is punched out, taking one radius of the original disc as the diameter of the hole. The potential at the centre of the original disc due to the remaining part is nV₀, where V₀ = [q/(2πε₀R)](1 - 1/π). Find n.