THE UNIVERSITY OF BRITISH COLUMBIA
 
Physics 122 Assignment # 5 SOLUTIONS:
 
POTENTIAL & CAPACITANCE
 
Fri. 1 Feb. 2002 - finish by Fri. 8 Feb.

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 $E = k_E/r_0 \int_0^e QdQ = {1\over2} k_E e^2/r_0$. If we set this equal to m c2 we get $\ds{ r_0 = {1\over2} k_E {e^2 \over m c^2 }
= { (8.998 \times 10^9)(1.6022 \times 10^{-19})^2 \over
2 (9.11 \times 10^{-31})(2.998 \times 10^8)^2 } }$ or \fbox{ $r_0 = 1.409 \times 10^{-15}$ ~m } . 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 $C^\prime$ 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 $C = \epsz A/d$. 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 $1/C^\prime = 1/C_1 + 1/C_2
= 2/4C = 1/2C$. Thus \fbox{ $C^\prime = 2 C$\space } .

 

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 $2.5 \times 10^{-4}$ m thick. The number of layers is therefore $N = 5 \times 10^{-2} / 2.5 \times 10^{-4} = 200$ and the total area is $A = N \times 0.05 \times 0.05 = 0.5$ m2. The capacitance is $C = \kappa \epsz A/d$ where d = 150 µm. The dielectric constant of SrTiO3 is (from Table 27-2) $\kappa = 310$, so $C = 310 \times 8.85 \times 10^{-12}
\times 0.5 / 1.5 \times 10^{-4}$ or \fbox{ $C = 9.145 \times 10^{-6}$ ~F or $9.145$ ~$\mu$ F } .
(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 $8 \times 10^6$ V/m. Our dielectric sheet has a thickness of $1.50 \times 10^{-4}$ m, so the breakdown voltage is 1200 V. At that potential, Q = CV gives \fbox{ $Q = 0.01097$ ~C } .1
(c)
the total energy we can store in this small cube.   ANSWER The total energy stored in a capacitor is given by \fbox{ $U = {1\over2} C V^2 = 6.584$ ~J } .

4.
ARRAY of CAPACITORS:
\epsfig{file=PS/capacitor_array.ps,width=1.75in}

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 $i^{\rm th}$ 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 \fbox{ $Q_1 = Q_3 = 8.0 \times 10^{-6}$ ~C } and \fbox{ $Q_2 = Q_4 = 4.5 \times 10^{-6}$ ~C } .
(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 $Q_{12} \equiv Q_1 + Q_2 = Q_{34} \equiv Q_3 + Q_4$ 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 $Q_{12} = Q_{34} = 6/(10^6/3.0 + 10^6/7.0)
= 12.6 \times 10^{-6}$ C. Meanwhile the voltage across C1 must be the same as that across C2: $Q_1/C_1 = Q_2/C_2 \Longrightarrow Q_2 = Q_1(C_2/C_1) = {1\over2} Q_1
\Longrightarrow Q_{12} = {3\over2} Q_1$ or \fbox{ $Q_1 = {2\over3} Q_{12} = 8.4 \times 10^{-6}$ ~C } and \fbox{ $Q_2 = Q_{12} - Q_1 = 4.2 \times 10^{-6}$ ~C } . Similarly, $Q_3/C_3 = Q_4/C_4 \Longrightarrow Q_4 = Q_3(C_4/C_3) = {3\over4} Q_3
\Longrightarrow Q_{34} = {7\over4} Q_3$ or \fbox{ $Q_3 = {4\over7} Q_{34} = 7.2 \times 10^{-6}$ ~C } and \fbox{ $Q_4 = Q_{34} - Q_3 = 5.4 \times 10^{-6}$ ~C } .

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 $\pm \sigma$ is given by $E = \sigma / \epsz$. Thus $\sigma = \epsz E
= 8.85 \times 10^{-12} \times 200 = 1.77 \times 10^{-9}$ C/m2. Over an area of $A = 200 \times 10^6 = 2 \times 10^8$ m2, this gives a total charge of \fbox{ $Q = \sigma A = 0.354$ ~C } .
(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 $U/V = {1\over2} \epsz E^2 = 0.5 \times 8.85 \times 10^{-12} \times (200)^2
= 0.177 \times 10^{-6}$ J/m3. The volume between the cloud and the ground is $V = 2000 \times 2 \times 10^8
= 4 \times 10^{11}$ m3, so \fbox{ $U = 0.708 \times 10^5$ ~J } .



Jess H. Brewer
2002-02-03