( iv ) Electric Field due to a Uniformly Charged Sphere: -
Let r = uniform volume charge density on a sphere of radius R.
( a ) For points inside the sphere: Applying Gauss’s Theorem to a sphere of radius r £ R,
4 pr2 E( r ) = (4p r 3 r) / 3e0
Let r = uniform volume charge density on a sphere of radius R.
( a ) For points inside the sphere: Applying Gauss’s Theorem to a sphere of radius r £ R,
4 pr2 E( r ) = (4p r 3 r) / 3e0
The direction of the field is radially outwards if r > 0 and inwards if r < 0.
( b ) For points outside the sphere: -
Applying Gauss’s Theorem to a sphere of radius r, concentric with charged sphere of radius R ( r > R ),
4 pr2 E( r ) = (4p R 3 r) / 3e0 = Q / e0
where Q is the charge on the sphere. Thus, for points outside the sphere, the entire charge of the sphere can be treated as concentrated at its centre.
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