A uniformly charged thin spherical shell of radius R carries uniform surface charge density of σ per unit area. It is made of two hemispherical shells, held together by pressing them with force F (see figure). F is proportional to
We know that the electrostatic pressure at a point on the surface of a uniformly charged sphere is P=σ22ϵ0
The force on the shell is F= pressure × surface area .
F=σ22ϵ0×4πR2
Thus, F∝1ϵ0σ2R2