A long, straight wire is surrounded by a hollow, thin, long metal cylinder whose axis coincides with that of wire. The wire has a charge per unit length of $\lambda$, and the cylinder has a net charge per unit length of $2\lambda$. Radius of the cylinder is $R$
Surface charge density on the inner surface of the cylinder is $\frac{\lambda }{{2\pi R}}$
Surface charge density on the outer surface of the cylinder is $\frac{3\lambda }{{2\pi R}}$
The electric field outside the cylinder,a distancer from the axis is $\frac{3}{2}\frac{\lambda }{{{ \in _0}\,\pi R}}$
The electric field outside the cylinder a distance $r$ from the axis is $\frac{{2\lambda }}{{{ \in _0}\,\pi R}}$
Obtain Gauss’s law from Coulomb’s law.
Electric field intensity at a point in between two parallel sheets with like charges of same surface charge densities $(\sigma )$ is
At a point $20\, cm$ from the centre of a uniformly charged dielectric sphere of radius $10\, cm$, the electric field is $100\, V/m$. The electric field at $3\, cm$ from the centre of the sphere will be.......$V/m$
Obtain the expression of electric field by charged spherical shell on a point outside it.
The electric field at $20 \,cm$ from the centre of a uniformly charged non-conducting sphere of radius $10 \,cm$ is $E$. Then at a distance $5 \,cm$ from the centre it will be