**Field due to a uniformly charged thin spherical shell**

Let σ be the uniform surface charge density of a
thin spherical shell of radius R. The field at any point P, outside or inside,
can depend only on r (the radial distance from the centre of the shell to the
point) and must be radial (i.e., along the radius vector).

(i)

**Field outside the shell:**Consider a point P outside the shell with radius vector r. To calculate E at P, we take the Gaussian surface to be a sphere of radius r and with centre O, passing through P. All points on this sphere are equivalent relative to the given charged configuration. The electric field at each point of the Gaussian surface, therefore, has the same magnitude E and is along the radius vector at each point.
Thus, E and ΔS at every point are parallel and the
flux through each element is E ΔS. Summing over all ΔS, the flux through the
Gaussian surface is E × 4 π r

^{2}. The charge enclosed is σ × 4 π R^{2}. By Gauss’s law
The electric field is directed outward if q > 0
and inward if q < 0. This, however, is exactly the field produced by a
charge q placed at the centre O. Thus for points outside the shell, the field
due to a uniformly charged shell is as if the entire charge of the shell is
concentrated at its centre.

**(ii) Field inside the shell:**In Fig., point P is inside the shell. The Gaussian surface is again a sphere through P centred at O.

The flux through the Gaussian surface, calculated as before, is
E × 4 π r

^{2}. However, in this case, the Gaussian surface encloses no charge. Gauss’s law then gives E × 4 π r^{2}= 0 i.e., E = 0 (r < R).
The field due to a uniformly charged thin shell is
zero at all points inside the shell. This important result is a direct consequence
of Gauss’s law which follows from Coulomb’s law.

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