(c) [image:1_image323.emf]
The electric field due to the spherical shell at point $+ P.$
$E = \frac{1}{4\pi\varepsilon_{0}}.\frac{q}{r^{2}}\ \ \ \ \ \ \ \ \ \ (\because r > R)$
$or\ \ \ E \propto \frac{1}{r^{2}}\ \ $
$or\ \ \ E \propto r^{- 2}$
According to Gauss’s law inside the shell electric field is zero.
$ie,\ \ \ \ \ \oint_{}^{}{\mathbf{E.ds} = 0}$
$or\ \ \ \ E = 0$
the electric field due to the shell at a point inside is zero and varies as $r^{- 2}$outside it.