The electric potential at the centre of two concentric half rings of radii $R_1$ and $R_2$, having same linear charge density $\lambda$ is
$\frac{2 \lambda}{\epsilon_0}$
$\frac{\lambda}{2 \epsilon_0}$
$\frac{\lambda}{4 \epsilon_0}$
$\frac{\lambda}{\epsilon_0}$
Three concentric metallic spherical shell $A, B$ and $C$ or radii $a, b$ and $c$ $(a < b < c)$ have surface charge densities $- \sigma , + \sigma ,$ and $- \sigma $ respectively. The potential of shell $A$ is :
Calculate potential on the axis of a disc of radius $R$ due to a charge $Q$ uniformly distributed on its surface.
Write an equation for potential due to a system of charges
At a certain distance from a point charge, the field intensity is $500\, Vm^{-1}$ and the potential is $-3000\, V$. The distance to the charge and the magnitude of the charge respectively are
Three charged concentric nonconducting shells are given as shown in figure. Find the potential at point $A$