Consider a thin spherical shell of radius R with a positive charge q distributed uniformly on the surface. As the charge is uniformly distributed, the electric field is symmetrical and directed radially outward.
(i) Electric field outside the shell:
For point
r>R; draw a spherical gaussian surface of radius r.
Using gauss law,
∮E.ds=qendq0Since
→E is perpendicular to gaussian surface, angle betwee
→E is 0.
Also
→E being constant, can be taken out of integral.
So, E(4πr2)=qq0
So, E=14πε0qr2
Thus electric field outside a uniformly charged spherical shell is same as if all the charge q were concentrated as a point charge at the center of the shell.
(ii) Inside the shell:
In this case, we select a gaussian surface concentric with the shell of radius r (r>R).
So, ∮E.ds=E(4πr2)
According to gauss law,
E(4πr2)=Qendε0
Since charge enclosed inside the spherical shell is zero.
So, E=0
Hence, the electric field due to a uniformly charged spherical shell is zero at all points inside the shell.