- 1.
- CLASSICAL RADIUS OF THE ELECTRON:
You are probably familiar with Einstein's famous equation E = m c2.
If m is the mass of an electron and E is the electrostatic
potential energy required to ``assemble'' the electron from bits
of charge infinitely distant from each other into a uniform
spherical shell of radius r0 and net charge e, find the
numerical value of r0 in meters.2
ANSWER:
Start with no charge, then bring successive bits dQ in to add
uniformly to the charge Q of the shell. A given bit of charge
acquires an electrostatic potential energy
dE = kE QdQ/r0
in the process. Thus the total energy E required to assemble the
shell is
. If we set
this equal to m c2 we get
or
. The conventional value
(actually the Compton wavelength of the electron) is twice as big,
2.818 fm, where ``fm'' stands for ``femtometers'' or ``fermis''
(named after Enrico Fermi); both are the same as 10-15 m.
- 2.
- CAPACITOR WITH INSERT:
Suppose we have a capacitor made of two large flat parallel plates
of the same area A (and the same shape), separated by an air gap
of width d. Its capacitance is C. Now we slip another planar
conductor of width d/2 (and the same area and shape)
between the plates so that it is centred halfway in between.
What is the capacitance
of the new system of three
conductors, in terms of the capacitance C of the original pair
and the other parameters given?
(Neglect ``edge effects'' and any dielectric effect of air.)
ANSWER:
The original capacitance was
. The capacitor with
the insert as shown is equivalent to two identical capacitors in
series, each of which has a gap of d/4 between its plates,
so that
C1 = C2 = 4 C. The equivalent capacitance of two
capacitors in series is given by
. Thus
.
- 3.
- CUBIC CAPACITOR
Suppose we take a roll of very thin (
50 µm) copper sheet and a roll of
150 µm thick strontium titanate dielectric
(see Table 29-2 on p. 671 of the textbook)
and form a capacitor as follows: cut the sheets into strips
5 cm wide and sandwich the dielectric sheet between
two sheets of copper. Then fold the sandwich back and forth
to fill a cube
5 cm on each side. Assuming that we can press the layers
together so that there are no empty spaces, find:
- (a)
- the capacitance of the resulting cube-shaped capacitor;
ANSWER:
Each layer consists of 2 sheets of Cu and 1 sheet of SrTiO3
and so is 250 µm or
m
thick. The number of layers is therefore
and the
total area is
m2.
The capacitance is
where d = 150 µm.
The dielectric constant of SrTiO3 is (from Table 27-2)
, so
or
.
- (b)
- the maximum charge it will hold without breaking down;
ANSWER:
Table 27-2 lists the dielectric strength of SrTiO3 as 8 kV/mm,
which is the same as
V/m. Our dielectric sheet
has a thickness of
m, so the breakdown
voltage is 1200 V. At that potential, Q = CV gives
.1
- (c)
- the total energy we can store in this small cube.
ANSWER:
The total energy stored in a capacitor is given by
.
- 4.
- ARRAY of CAPACITORS:
The battery B supplies
6 V. The capacitances are
C1 =
2.0 µF,
C2 =
1.0 µF,
C3 =
4.0 µF and
C4 =
3.0 µF.
- (a)
- Find the charge on each capacitor
when switch S1 is closed but switch S2 is still open.
ANSWER:
Let Qi denote the charge on the
capacitor Ci.
From charge conservation we have Q1 = Q3 and Q2 = Q4.
Both pairs of capacitors in series (1 and 3; 2 and 4) must make up
the full voltage:
VB = Q1/C1 + Q3/C3 = Q2/C2 + Q4/C4.
Therefore
VB = Q1[1/C1 + 1/C3] = Q2[1/C2 + 1/C4]
yielding
Q1 = Q3 = 6/(106/2.0 + 106/4.0) and
Q2 = Q4 = 6/(106/1.0 + 106/3.0) or
and
.
- (b)
- What is the charge on each capacitor if S2 is also closed?
ANSWER:
Now C1 and C2 are effectively just one big capacitor
C12 = C1 + C2 = 3.0 µF and similarly for
C34 = C3 + C4 = 7.0 µF. Charge conservation
now requires
and the two effective capacitors in series must make up the
full voltage:
VB = Q12/C12 + Q34/C34.
Thus
VB = Q12[1/C12 + 1/C34] giving
C.
Meanwhile the voltage across C1 must be the same as that across C2:
or
and
.
Similarly,
or
and
.
- 5.
- THUNDERCLOUD CAPACITOR:
A large thundercloud hovers over the city of Vancouver at a height of
2.0 km. Between the cloud and the ground
(both of which we may treat as parallel conducting plates,
neglecting edge effects) the electric field is about
200 V/m. The cloud has a horizontal area of
200 km2.
- (a)
- Estimate the number of Coulombs [C] of positive charge
in the cloud, assuming that the ground has the same surface density
of negative charge.
ANSWER:
The electric field between two flat plates with surface charge densities
is given by
. Thus
C/m2.
Over an area of
m2,
this gives a total charge of
.
- (b)
- Estimate the number of joules [J] of energy
contained in the air between the cloud and the ground.
ANSWER:
The energy density stored in an electric field is given by
J/m3. The volume between the cloud
and the ground is
m3, so
.