Electricity & Magnetism
FINAL EXAMINATION
PHYSICS 1220
17 April 1997
- Please answer all the questions on this test.
- All questions are worth 10 marks each.
- Show all your work.
- For problems involving forces and fields, include
free body diagrams.
- Please start each problem on a new page in the
exam booklet.
- One 8½ × 11 sheet containing formulas is allowed.
- Formula sheet must be submitted with examination
to receive marks.
- Time to do the test is three hours maximum.
- If you have any questions, raise your hand and
remain seated.
- Two capacitors, C1 = 80 μF
and C2 = 20 μF,
are separately, fully charged by a 20 V battery. The two capacitors
are then put in a circuit with a resistor, R = 1000 Ω,
and an open switch S as shown below.
(a) What is the charge on each capacitor before being
placed in the circuit?
(b) What is the charge on each capacitor after being
placed in the circuit (S is open)? Explain.
(c) When switch S is closed, how will the total charge
stored on the two capacitors, QT = Q1 +
Q2, change with time?
(d) How is the charge on each capacitor related to
QT(t)?
(e) How long with it take for the charge on C1
to drop to 35% of its original value?
(f) What will be the charge on C2 at t
= 0.25 seconds after the switch is closed?
- A thin ring of radius R has a charge Q uniformly
distributed on it.
(a) From first principles, determine the electric
field at a distance along an axis through the centre of the ring
and perpendicular to the ring.

(b) Derive the potential difference between x = 0 and x = 5R.
(c) If a charge q = 1.00 μC
is released at x =0, how fast will the charge be moving when it
gets to x = 5R. The mass of the charge is m = 0.100 kg. Assume
Q = 5.00 μC
and R = 0.100 m.
- A sphere consists of a hollow centre of radius
R and two concentric spherical shells each of thickness R/2. The
inner shell carries a uniformly distributed charge of -Q, the
outer shell 3Q. What is ρinner,
the charge density of the inner shell? What is ρouter,
the charge density of the outer shell? Give expressions for E(r)
in all four regions. Sketch E(r) as a function of R.
- The diagram below shows a loop of wire carrying
a current I. The curved part of the loop is circular with radius
R. Distance s is the distance from point P to the horizontal wire
segment. The angle α
is less than 90°.
Using the Law of Biot-Savart, derive an expression for the magnetic
field at point P, the centre of the circular arc. Express your
answer in terms of μ0,
I, R, s, and α.
Hint - consider each piece separately and for the horizontal piece
express the limits of integration in terms of s and α.
- The consists of three batteries and three resistors.
Resistor R2 and battery ε2
are unknown but R1 = 10 Ω,
R3 = 15 Ω,
ε1
= 12 Volts, and ε3
= 4 Volts. What would ε2
have to be so that no current flows through R2?
- The diagram below shows a region of uniform magnetic
field B = 0.250 T out of the paper. In the bottom left hand corner
of the region is a velocity selector of unknown electric field
E which has a small gap to allow only certain particles to pass
through. The gap is a distance d = 15.0 cm from a plate. A sample
of radioactive cesium is emitting alpha particles ( |q|
= 2e and m = 6.6413 × 10-27 kg) into the velocity selector.
What must be the direction and magnitude of the minimum electric
field in the velocity selector if the alpha particles are not
to hit the plate? Is the ion positive or negative? Explain.
- In the diagram below, a flat conducting loop of
wire of dimensions h = 30.0 cm by l = 20.0 cm is
immersed perpendicularly in a magnetic field which changes with
time,
B(t) = t4-3t3-6t2+4t+1 .
The diagram shows t = 0, where B > 0 indicates
that the magnetic field is coming out of the paper. The resistanceless
wire is connected to a resistor R = 25.0 Ω.
Find
(a) when the induced emf is a maximum. Determine
the magnitude and direction of the current in the loop.
(b) when the induced emf is a minimum. Determine
the magnitude and direction of the current in the loop.
[If you cannot recall how to find extrema, I will
tell you for a small deduction of marks.]
- The current density in a cylindrical wire of radius
R is given by
j(r) = A(1-er) ,
where A is a positive constant. Use Ampere's Law
to determine the magnetic field produced by the wire as a function
of the radial distance from the centre of the wire. Sketch the
result.
- A rectangular loop of wire carries a current of
6.3 A. Nearby in the plane of the loop is a straight wire carrying
a current of 5.4 A. What is the magnitude and direction of the
net force on the entire loop if the directions and dimensions
are as given below in the diagram?
- As shown below, two capacitors are connected
in parallel with a 9.0-V battery across them. Each capacitor has
a plate area of 15 cm by 12 cm and a plate separation of 2.2 mm.
One capacitor has an air gap, the other has a nylon dielectric
(k = 3.5).
(a) What is the capacitance of each capacitor?
(b) What is the charge on each capacitor?
(c) A switch is opened and the dielectric is then
removed from the second capacitor leaving it with an air gap.
What are the new charge and potential difference on each capacitor?
Formulas
Coulomb's Law and Electric Fields:
| F = kq1q2/r2 |
F= q0E |
EPoint Charge = kQ/r2 |
| Ewire = 2kλ/r |
Eplate = Σ/2ε0 |
Esphere = KQ/r2 |
Gauss' Law
|
φE
= òE
·ndA |
= Qinside/ε0 |
| cylinders - |
E(a)2πaL |
= [2πL
òr(r)rdr]/ε0 |
| spheres - |
E(a)4πa2 |
= [4pòr(r)r2dr]/ε0 |
Electrostatic Potential
| ΔV = V(b) - V(a) =
-òbaE·dl = -òbaE(r)dr |
| Vpoint charge = kQ/r |
V = V1 + V2 + ... |
ΔK =ΔU =
-qΔV |
Capacitors
| C = Q/V |
CP = C1+C2 |
1/Cs = 1/C1+1/C2 |
| Cplates = ε0A/d |
Eplates = Q/ε0A |
Cdielectric = kC0 |
| Edielectric = kE0 |
Σb = [(k-1)/k]sf |
U = ½Q2/C = ½QV = ½CV2 |
| charging: |
Q = Cε(1 - e-t/RC) |
I = (ε /R)e-t/RC |
| discharging: |
Q = Q0e-t/RC |
I = (ε /R)e-t/RC |
Resistors
| Rs = R1 + R2 |
1/Rp = 1/R1 + 1/R2 |
| V = IR |
P = I2R = V2/R = VI |
| åEi -åIiRi = 0 |
åqin =åqout |
Magnetic Field
| F = qv×B |
F = IL×B |
r = mv/qB |
| f = 1/T = qB/2πm |
vselector = E/B |
m = NIAn |
| τ =
m×B |
B = (μ0/4πr2)qv×r |
| dBBiot-Savart =
(μ0/4πr2)IdL×r |
Bwire = μ0I/2πR |
| Bloop = μ0I/2R |
Bsolenoid = μ0nI |
Ampere's Law
| òCB·dl |
= μ0Iinside |
| cylindrical wires: |
B2πa |
= 2pm0òj(r)rdr |
Magnetic Induction
| φm = BAcosθ |
Einduced = dφm/dt |
|Emotional| = vBl |
Constants
| k = 8.99 × 109 N m2/C2 |
ε0 = 8.85 × 1012 F/m |
μ0 = 4π × 107 T-m/A |
Identities and Integrals
| if ax2+bx+c=0, x = {b±[b2- 4ac]½}/2a |
S = Rθ, dS = Rdθ |
| òxndx
= xn+1/(n+1) + C | òx-1dx
= lnx + C |
| òebxdx
= ebx/b + C |
òxebxdx
= (x - b)ebx + C |
| òcosΩxdx
= (sinΩx)/Ω + C |
òsinΩxdx
= -(cosΩx)/Ω + C |
| ò(a/[a2+x2]3/2)dx
= 1/[a[a2+x2]1/2] + C |
ò(x/[a2+x2]3/2)dx
= -1/[a2+x2]1/2 + C |
Questions?
mike.coombes@kwantlen.ca