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- 10-10
- (a) Since the two spheres have the same potential,
where
,
, and
. So we get
and
. Then the electric field near the
surface of the first sphere is
, and that of the second sphere is
.
(b) The electric potential is the same for each sphere:
.
- 11-1
- (a) From ,
. (b) The
capacitance is not dependent on the charges. (c) The new potential is
.
- 11-2
- From
,
.
- 11-3
- From
, we get
.
- 11-4
- (a) The equivalent capacitance is
. So the total charge is
. All capacitors have the same amount of charge. Therefore the
potential difference for each capacitor is
and
.
(b) In this situation, the overall voltage is zero, which means that
both capacitors have the same magnitude of the potential difference.
The sum of the charges needs to be the same as twice the accumulated
charge in (a), which means that
. So we
get . For the first capacitor,
and
. (c) In this case,
the steady state maintains no net charge or potential differences.
- 11-5
- Repeatedly using the equivalence formulae part by part,
we get .
- 11-6
- The potential of the metal sphere is
determined from
with . Then the electric field on the surface of the sphere is
. So the energy density at the surface is
.
Next: About this document ...
Up: Homework Solutions for PHYS262,
Previous: Homework Solutions for PHYS262,
Hyok-Jon Kwon
2001-08-29