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