**Required math: calculus**

**Required physics: electrostatics**

Reference: Griffiths, David J. (2007) Introduction to Electrodynamics, 3rd Edition; Prentice Hall – Chapter 3, Post 41.

The average electric field inside a sphere of radius due to a point charge at position inside the sphere is the field integrated over the volume of the sphere divided by the sphere’s volume:

where the integral extends over the interior of the sphere. (Note that the statement of the problem in Griffiths’ book has a typo: the unit vector in the integral in part (a) should be script ‘r’, not .)

Now suppose we have a uniformly charged sphere with charge density and wish to find the field at point due to this charge. This time the field at due to volume element is so the overall field is

The two fields are the same if we set

From Gauss’s law, we can work out if we work out the integrals below for a sphere of radius :

Since points in the radial direction due to symmetry,

The dipole moment of a single point charge at position is , so the field can be written as

From the superposition principle, we can extend this result so that it applies to any distribution of charge within the sphere.

If is outside the sphere, the formula for is the same as before, with the integral still extending over the interior of the sphere. The formula for is also the same, but this time if we use Gauss’s law and integrate over a spherical surface of radius , we get

The RHS of the second line arises from the fact that all of the charged sphere is now interior to the surface of integration, while on the LHS, we are still integrating over a spherical surface of radius . The average field produced by a point charge is thus the same as the field produced by this charge at the centre of the sphere. By superposition we can apply this argument to any distribution of charge external to the sphere.

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