(a)-
Field outside the sphere:-
Suppose
the charge q is uniformly distributed over a sphere of radius R as shown in
figure.
Let us
find the electric field E at the point P outside the sphere for which we draw a
Gaussian surface shown by dotted curve at a concentric sphere of radius OP=r.
So by Gauss theorem
The flux
through the surface
∮E.dS = q/εo
Or E∮dS = q/εo
Or E.4πr2= q/εo
E = 1/4πεo q/r2
Which is
same as electric field at distance r from the point P & charge q. Hence it
is clear that the charge may be concentrated at the centre.
(b)- At a
point on the sphere:-
We put r=R then,
Electric field on the surface of
sphere
E=1/4πεo q/R2
(c)-
Electric field inside the sphere:-
Let us
find the electric field E at the point P inside the charged sphere. We draw a
Gaussian surface of radius r1.
The outward flux throw the surface of
sphere.
∮E.dS = E.4πr12………………..(1)
Now the
total charge inclosed by the Gaussian surface.
q’ = volume inclosed by the Gaussian surface X charge density
= 4/3 πr12 X ρ………………………….(2)
Since ∮E.dS = q/εo
Hence
from (1) & (2) we have
EX4πr12 = 4/3 πr13 .ρ
E = ρr1/3εo
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