Problem Set #5: Calculating Electromagnetic Fields of Current Sheets and Line Sources - Pr, Study notes of Guiding Electromagnetic Systems

This problem set includes four problems related to calculating the electromagnetic fields of current sheets and line sources in free space. The problems involve finding the e and h fields produced by a current sheet in the z = 0 plane, and the y-component of the h-field produced by a line source for both perpendicular and parallel polarizations. Hints are provided to help construct the solutions.

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2010/2011

Uploaded on 12/15/2011

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Problem Set #5
1. Find the E and H fields produced by a current sheet of the form
JS(x)=ˆ
x J0ejkxx
located in the z = 0 plane, in free space.
2. In class, we determined the fields of a line source for the perpendicular
polarization (TM to y). Using your answer from problem (1), find the y-
component of the H-field produced in free space by a line source of the form
JS(x)=ˆ
x I0
δ
(x)
δ
(y)
In that manner, you will determine the fields of the line source for the parallel
polarization (TE to y). Hint: The initial form of the superposition integral looks
simple, but the easiest approach is actually to manipulate this into the form of the
integral that we did for the TM-to-y case, namely
I=ej k2kx
2 z
k2kx
2
−∞
ejkxxdkx=
π
H0
(2 ) (k
ρ
)
There is a little trick to getting it into that form, but it is the most straightforward
way to construct the solution!
3. Using the results from Note #13, and problem set 4, determine an expression for
the H-field components (x, y, and z) of the point source in (13.1). Express your
answers in the form of derivatives of the quantity
I0
ejk0r
4
π
r
Hint: You should be able to do this by inspection!

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Problem Set #

  1. Find the E and H fields produced by a current sheet of the form

J

S

( x ) =

x J

0

e

jk

x

x

located in the z = 0 plane, in free space.

  1. In class, we determined the fields of a line source for the perpendicular

polarization (TM to y ). Using your answer from problem (1), find the y -

component of the H - field produced in free space by a line source of the form

J

S

( x ) =

x I

0

δ ( x ) δ ( y )

In that manner, you will determine the fields of the line source for the parallel

polarization (TE to y ). Hint: The initial form of the superposition integral looks

simple, but the easiest approach is actually to manipulate this into the form of the

integral that we did for the TM-to- y case, namely

I =

e

j k

2

k

x

2

z

k

2

k

x

−∞ 2

e

jk

x

x

dk

x

= π H

0

( 2 )

( k ρ)

There is a little trick to getting it into that form, but it is the most straightforward

way to construct the solution!

  1. Using the results from Note #13, and problem set 4, determine an expression for

the H - field components ( x , y , and z ) of the point source in (13.1). Express your

answers in the form of derivatives of the quantity

I

0

e

jk

0

r

4 π r

Hint: You should be able to do this by inspection!