A non-linear spherical charge distribution carries a density = ar^2 in the region r<a. If a concentric metal shell with radii b and c surrounds the inner charge, calculate the electric field in the four regions starting with region 1, inside the radius a and ending with region 4, outside the concentric spheres.
for r<a:
charge enclosed =integration of a*r^2*4*pi*r^2*dr
=4*pi*a*(r^5/5)
=0.8*pi*a*r^5
if electric field is E,
using Gauss’ law:
E*4*pi*r^2=charge enclosed/epsilon
==>E*4*pi*r^2=0.8*pi*a*r^5/epsilon
==>E=0.2*a*r^3/(epsilon)
for a<r<b:
total charge enclosed=0.8*pi*a*a^5
=0.8*pi*a^6
if electric field is E,
using Gauss law:
E*4*pi*r^2=charge enclosed/epsilon
==>E*4*pi*r^2=0.8*pi*a^6/epsilon
==>E=0.2*a^6/(epsilon*r^2)
for b<r<c:
as it is a metallic hollow cylinder, electric field inside a conductor =0
for r>c:
charge enclosed =
=0.8*pi*a*r^5 with r=a
=0.8*pi*a*a^5=0.8*pi*a^6
if electric field is E,
using Gauss' law,
E*4*pi*r^2=charge enclosed/epsilon=0.8*pi*a^6/epsilon
==>E=0.2*a^6/(epsilon*r^2)
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