b/Example 19.c/Example B. Part of the
outside sphere has been drawn
as if it is transparent, in order to
show the inside sphere.No. Consider, for instance, an alternative universe in which elec-
tric forces are twice as strong as in ours. The numerical value of
kis doubled. Becausekis doubled, all the electric field strengths
are doubled as well, which quadruples the quantityE^2. In the ex-
pressionE^2 / 8 πk, we’ve quadrupled something on top and dou-
bled something on the bottom, which makes the energy twice as
big. That makes perfect sense.
Potential energy of a pair of opposite charges example 19
Imagine taking two opposite charges, b, that were initially far
apart and allowing them to come together under the influence
of their electrical attraction.
According to our old approach, electrical energy is lost because
the electric force did positive work as it brought the charges to-
gether. (This makes sense because as they come together and
accelerate it is their electrical energy that is being lost and con-
verted to kinetic energy.)
By the new method, we must ask how the energy stored in the
electric field has changed. In the region indicated approximately
by the shading in the figure, the superposing fields of the two
charges undergo partial cancellation because they are in oppos-
ing directions. The energy in the shaded region is reduced by
this effect. In the unshaded region, the fields reinforce, and the
energy is increased.
It would be quite a project to do an actual numerical calculation of
the energy gained and lost in the two regions (this is a case where
the old method of finding energy gives greater ease of computa-
tion), but it is fairly easy to convince oneself that the energy is
less when the charges are closer. This is because bringing the
charges together shrinks the high-energy unshaded region and
enlarges the low-energy shaded region.
A spherical capacitor example 20
.A spherical capacitor, c, consists of two concentric spheres of
radiiaandb. Find the energy required to charge up the capacitor
so that the plates hold charges +qand−q.
.On page 102, I proved that forgravitational forces, the inter-
action of a spherical shell of mass with other masses outside it
is the same as if the shell’s mass was concentrated at its cen-
ter. On the interior of such a shell, the forces cancel out exactly.
Since gravity and the electric force both vary as 1/r^2 , the same
proof carries over immediately to electrical forces. The magnitude
of the outward electric field contributed by the charge +qof the
central sphere is therefore
|E+|={
0, r<a
k q/r^2 , r>a,
whereris the distance from the center. Similarly, the magnitude
Section 10.4 Energy in fields 607