Two unlike charges of magnitude $q$ are separated by a distance $2d$. The potential at a point midway between them is
Zero
$\frac{1}{{4\pi {\varepsilon _0}}}$
$\frac{1}{{4\pi {\varepsilon _0}}}.\frac{q}{d}$
$\frac{1}{{4\pi {\varepsilon _0}}}.\frac{{2q}}{{{d^2}}}$
Charges are placed on the vertices of a square as shown. Let $E$ be the electric field and $V$ the potential at the centre. If the charges on $A$ and $B$ are interchanged with those on $D$ and $C$ respectively, then
A charge is spread non-uniformly on the surface of a hollow sphere of radius $R$, such that the charge density is given by $\sigma=\sigma_0(1-\sin \theta)$, where $\theta$ is the usual polar angle. The potential at the centre of the sphere is
Concentric metallic hollow spheres of radii $R$ and $4 R$ hold charges $Q _{1}$ and $Q _{2}$ respectively. Given that surface charge densities of the concentric spheres are equal, the potential difference $V ( R )- V (4 R )$ is
The potential at a point, due to a positive charge of $100\,\mu C$ at a distance of $9\,m$, is
Calculate potential on the axis of a disc of radius $R$ due to a charge $Q$ uniformly distributed on its surface.