Consider a metal sphere of radius $R$ that is cut in two parts along a plane whose minimum distance from the sphere's centre is $h$. Sphere is uniformly charged by a total electric charge $Q$. The minimum force necessary to hold the two parts of the sphere together, is
$\frac{{{Q^2}\left( {{R^2} - {h^2}} \right)}}{{4\pi \,{ \in _0}\,{R^4}}}$
$\frac{{{Q^2}}}{{4\pi \,{ \in _0}\,{R^2}}}$
$\frac{{{Q^2}\left( {R - h} \right)}}{{32\pi \,{ \in _0}\,{R^3}}}$
$\frac{{{Q^2}\left( {{R^2} - {h^2}} \right)}}{{32\pi \,{ \in _0}\,{R^4}}}$
Let $E_1(r), E_2(r)$ and $E_3(r)$ be the respective electric fields at a distance $r$ from a point charge $Q$, an infinitely long wire with constant linear charge density $\lambda$, and an infinite plane with uniform surface charge density $\sigma$. if $E_1\left(r_0\right)=E_2\left(r_0\right)=E_3\left(r_0\right)$ at a given distance $r_0$, then
If the total charge enclosed by a surface is zero, does it imply that the electric field everywhere on the surface is zero ? Conversely, if the electric field everywhere on a surface is zero, does it imply that net charge inside is zero.
Consider an atom with atomic number $Z$ as consisting of a positive point charge at the centre and surrounded by a distribution of negative electricity uniformly distributed within a sphere of radius $R$. The electric field at a point inside the atom at a distance $r$ from the centre is
Obtain the expression of electric field at any point by continuous distribution of charge on a $(i)$ line $(ii)$ surface $(iii)$ volume.
A long charged cylinder of linear charged density $\lambda$ is surrounded by a hollow co-axial conducting cylinder. What is the electric field in the space between the two cylinders?