Problem Set 8 : Equivalence principle, Exercises of Guiding Electromagnetic Systems

Problem Set 8 : using Huygens equivalence principle

Typology: Exercises

2023/2024

Uploaded on 10/28/2024

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Problem Set #8
1. A slab of current density in the region
−∞ <x<
,
−∞ <y<
, –Δ < z < Δ has
J=ˆ
y J0
.
(a) Use the Green’s function
ejkzz
2jkz
to find the magnetic vector potential
Ay
as a function of z in the z > Δ region.
What is
kz
?
(b) Find the
Hx
field as a function of z in the z > Δ region.
2. Find equivalent electric and magnetic surface currents (Note #21) located on a
sphere of radius a, centered at the origin, that if radiating in free space reproduce
the fields of a Hertzian dipole at the origin. (Hint: Define these directly in
spherical coordinates.)
3. The fields of a thin, linear dipole are often obtained by approximating the
equivalent electric current density by the “sinusoidal triangle” function considered
in Problem Set #7, Problem 4:
J(x,y,z)=ˆ
z I0sin kh k z
( )
δ
(x)
δ
(y)p(z;h,h)
Using the result of Problem 4 on Problem Set #7 to assist you, show that the
component of the electric field of this source can be expressed without
approximation as
Ez(x,y,z)=j
η
I0
ejkR1
4
π
R1
+ejkR2
4
π
R2
2 cos(kh)ejkr
4
π
r
What are R1 and R2 in this expression?
Hint: Use the fact that
pf2

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Problem Set #

  1. A slab of current density in the region −∞ < x < ∞ , −∞ < y < ∞ , – Δ < z < Δ has

J =

y J

0

(a) Use the Green’s function

e

jk

z

z

2 jk

z

to find the magnetic vector potential A

y

as a function of z in the z > Δ region.

What is k

z

(b) Find the H

x

field as a function of z in the z > Δ region.

  1. Find equivalent electric and magnetic surface currents (Note #21) located on a

sphere of radius a , centered at the origin, that if radiating in free space reproduce

the fields of a Hertzian dipole at the origin. (Hint: Define these directly in

spherical coordinates .)

  1. The fields of a thin, linear dipole are often obtained by approximating the

equivalent electric current density by the “sinusoidal triangle” function considered

in Problem Set #7, Problem 4 :

J ( x , y , z ) =

z I

0

sin khk z

δ ( x ) δ ( y ) p ( z ;− h , h )

Using the result of Problem 4 on Problem Set #7 to assist you, show that the ˆ z

component of the electric field of this source can be expressed without

approximation as

E

z

( x , y , z ) = − j η I

0

e

jkR

1

4 π R

1

e

jkR

2

4 π R

2

− 2 cos( kh )

e

jkr

4 π r

What are R 1

and R 2

in this expression?

Hint: Use the fact that

E

z

( x , y , z ) =

j ωε

0

z • (∇∇ • + k

2

)( J ∗ G )

j ωε

0

z • (∇∇ • J + k

2

J ) ∗ G

j ωε

0

d

2

J

z

dz

2

  • k

2

J

z

) ∗ G

  1. Consider a coplanar waveguide (CPW) type of transmission line, consisting of

two equal-size slots cut into an infinite PEC ground plane, as sketched:

The CPW line is used in the ground-signal-ground configuration (the outer planes

are used as the ground). The complementary structure, consisting of two co-

planar strips (CPS), is sketched below.

Assuming that these structures are each used as a TEM transmission line,

(a) sketch the E and H fields associated with a transmission line mode on each

(b) define an impedance for each, and in a manner similar to that carried out in

Note #23, determine the relationship between the impedance of the CPW line and

that of the CPS line.