Exam 4: Electromagnetic Fields at St. Vincent College - Problems and Solutions, Exams of Electromagnetism and Electromagnetic Fields Theory

Solutions to exam 4 of the electromagnetic fields course at st. Vincent college. It includes the calculation of potentials for a spherical shell of charge, determination of coefficients for a given function, and finding the force exerted on a charge near a wire and a conducting sheet.

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St. Vincent College
PH 252: Electromagnetic Fields
Exam 4
10/22/2010
1. (35 pts) In class, we started a problem involving a spherical shell of charge carrying charge density
σ(θ) = P0cos θ. We applied boundary conditions on the potential at r and r0, using a partial
solution to Laplace’s Equation in spherical coordinates, and arrived at potentials
ϕin =A1+C1rcos θ(r < R)
ϕout =B2
r+D2
r2cos θ(r > R)
Apply the remaining boundary conditions, ϕin =ϕout at the shell (r=R) and Eout Ein =σ0, to
solve for the remaining undetermined coefficients in the two potentials. Make sure to write out and
clearly identify the final potentials, both for r < R and r > R.
pf3
pf4

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St. Vincent College PH 252: Electromagnetic Fields

Exam 4

  1. (35 pts) In class, we started a problem involving a spherical shell of charge carrying charge density σ(θ) = P 0 cos θ. We applied boundary conditions on the potential at r → ∞ and r → 0 , using a partial solution to Laplace’s Equation in spherical coordinates, and arrived at potentials

ϕin = A 1 + C 1 r cos θ (r < R)

ϕout =

B 2

r

D 2

r^2 cos θ (r > R)

Apply the remaining boundary conditions, ϕin = ϕout at the shell (r = R) and E⊥out − E⊥in = σ/ǫ 0 , to solve for the remaining undetermined coefficients in the two potentials. Make sure to write out and clearly identify the final potentials, both for r < R and r > R.

  1. (30 pts) Any function f (x) may be written, over the interval ( 0 < x < a), as

f (x) =

∑^ ∞

0

Cn sin

( (^) nπ a

x

a) (15 pts) Show that the coefficients Cn are given by

Cn =

a

∫^ a

0

f (x) sin

( (^) nπ a

x

dx

You may find the following helpful on both parts (a) and (b) of this problem:

∫^ a

0

sin

( (^) nπx a

sin

( (^) mπx a

dx =

{ (^) a 2 ;^ n^ =^ m 0; n 6 = m

∫^ a

0

sin

( (^) nπx a

cos

( (^) mπx a

dx = 0

∫ sin^2 ax dx =

x 2

sin 2ax 4 a

cos^2 ax dx =

x 2

sin 2ax 4 a

  1. (35 pts) A long, straight wire with uniform linear charge density λ lies parallel to, and at a distance d from, an infinite, flat, grounded, conducting sheet. Determine the force exerted on a charge q when placed at d/ 2 from the sheet directly below the wire (i.e. it is also d/ 2 from the wire). (Hint: It may help to first determine the electric field at that location and then compute the force on charge q. Also, you do not need to solve Laplace’s Equation for this problem.)