Simple Nature - Light and Matter

(Martin Jones) #1
of theinwardfield contributed by the outside sphere is

|E−|=


{


0, r<b
k q/r^2 , r>b

.


In the region outside the whole capacitor, the two fields are equal
in magnitude, but opposite in direction, so they cancel. We then
have for the total field

|E|=





0, r<a
k q/r^2 , a<r<b
0, r>b

,


so to calculate the energy, we only need to worry about the region
a<r<b. The energy density in this region is

dUe
dv

=


1


8 πk

E^2


=


k q^2
8 π

r−^4.

This expression only depends onr, so the energy density is con-
stant across any sphere of radiusr. We can slice the region
a< r < binto concentric spherical layers, like an onion, and
the energy within one such layer, extending fromrtor+ dris

dUe=

dUe
dv
dv

=

dUe
dv
(area of shell)(thickness of shell)

= (
k q^2
8 π

r−^4 )(4πr^2 )(dr)

=


k q^2
2
r−^2 dr.

Integrating over all the layers to find the total energy, we have

Ue=


dUe

=


∫b

a

k q^2
2

r−^2 dr

=−


k q^2
2
r−^1


∣∣



b

a
=

k q^2
2

(


1


a


1


b

)


608 Chapter 10 Fields

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