Analysis of Leaky Modes in Dielectric Slabs and Waveguides (ECE 6341, Spring 2009, HW 2), Assignments of Electrical and Electronics Engineering

Homework problems related to the analysis of leaky modes in dielectric slabs and rectangular waveguides. The problems involve finding the normalized phase constant, cutoff frequency, splitting point frequency, and complex solution for the tm1 leaky mode in a grounded teflon slab using numerical search methods. Additionally, the document derives the exact electric field above the interface for a tex leaky mode and uses the method of stationary phase to derive the far-field pattern.

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ECE 6341
Spring 2009
HW 2
1) A grounded dielectric slab of Teflon has a relative permittivity of 2.2 and a thickness of
50 mils (1.534 mm). Use a numerical search to find the normalized phase constant
0
/k
of the TM0 surface-wave mode at the following frequencies: 1 GHz, 10 GHz, 100 GHz.
2) Assume that we have the same grounded slab as in the previous problem, but now we are
interested in the TM1 mode. First, find the cutoff frequency of this mode. Then, by
numerically searching for the improper surface-wave solutions, find the splitting point
frequency fs. Then, for a frequency that is 10% lower than the splitting point frequency
(i.e., f = 0.9 fs) numerically search to find the complex TM1 leaky-mode solution (the one
that has a positive attenuation constant). You can use whatever numerical search routine
you want. Note that the secant method works in the complex plane, and is usually a good
choice. This method is allows you to find the complex roots (zeros) of a complex
function f (z). The method is represented by the following iterative formula (which
requires two initial guesses z0 and z1)
1 1
1
n
n n n n
n n
f z
z z z z f z f z
.
3) A TEx leaky mode has a field on the interface (x = 0) due to a line source at z = 0 that is
represented as
0,
LW
z
jk z
y
E z A e
where
LW
z z z
k j
and A is an amplitude constant. The exact electric field above the
interface is
.
where
1/ 2
2 2
0x z
k k k
. The branch of the square root is chosen so that that
Im 0.
x
k
Show that
1
1
, 0, ,
2
x z
jk x jk z
y y z z
E x z E k e e dk
lw
2
lw 2
0, 2
z
y z
z z
k
E k jA
k k

pf3

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ECE 6341

Spring 2009

HW 2

  1. A grounded dielectric slab of Teflon has a relative permittivity of 2.2 and a thickness of

50 mils (1.534 mm). Use a numerical search to find the normalized phase constant 0

/ k

of the TM 0 surface-wave mode at the following frequencies: 1 GHz, 10 GHz, 100 GHz.

  1. Assume that we have the same grounded slab as in the previous problem, but now we are

interested in the TM 1 mode. First, find the cutoff frequency of this mode. Then, by

numerically searching for the improper surface-wave solutions, find the splitting point

frequency fs. Then, for a frequency that is 10% lower than the splitting point frequency

(i.e., f = 0.9 fs ) numerically search to find the complex TM 1 leaky-mode solution (the one

that has a positive attenuation constant). You can use whatever numerical search routine

you want. Note that the secant method works in the complex plane, and is usually a good

choice. This method is allows you to find the complex roots (zeros) of a complex

function f ( z ). The method is represented by the following iterative formula (which

requires two initial guesses z 0 and z 1 )

1 1

1

n

n n n n

n n

f z

z z z z

f z f z

 

3) A TE

x leaky mode has a field on the interface ( x = 0) due to a line source at z = 0 that is

represented as

 0,^ 

LW z jk z

y

E z Ae

 

where

LW

z z z

k    j  and A is an amplitude constant. The exact electric field above the

interface is

where

1/ 2 2 2

x 0 z

kkk. The branch of the square root is chosen so that that^ Im 0. x

k

Show that

x z jk x jk z

y y z z

E x z E k e e dk

 

 

lw

2 lw 2

z

y z

z z

k

E k jA

k k

and thus derive an exact expression for the field above the interface due to the leaky

mode. (The expression will be in the form of an integral, as shown above).

  1. According to the method of stationary phase (or the method of steepest-descents) which

will be discussed later in the semester, we can asymptotically evaluate the field radiated

by the leaky mode, by using the result

where  

z

f k (^) is an arbitrary function of z

k (^) ,

1/ 2 2

x 0 z

kkk , 0 0

sin z

kk , and

x   cos, z   sin. Assuming this relation, derive the far-field pattern  , 

FF

y

E  

of the TE x leaky mode.

5) Assume that we have a TE x leaky mode with  

0

z

  k and 0

z

  k. Plot the

magnitude of the normalized far-field pattern  , 

FF

y

E   versus angle  from –

o to

o

. Plot in dB and normalize the plot so that the peak of the pattern is at zero dB.

6) For the same TE x leaky wave as above, plot the magnitude of the field ^ 

y

E x z (not in

dB) versus x. Plot over the range (^0) 0  x  20  for the following fixed values of z :

0 0 0 0 0

z  1  , 5  ,10  , 50  ,100

. Assume that A = 1. Comment on the variation that you

observe vertically. The field should be calculated numerically by using the result from

Problem 2.

7) Repeat problems 5-6, assuming now that ^ ^

0

z

  k and 0

z

  k. This

corresponds to a leaky mode that is in the non-physical region.

  1. A rectangular waveguide is loaded with dielectric slabs on either side, as shown below.

Derive transcendental equations for the wavenumber kz and the cutoff frequencies for all

h 

r

z

x

0 4

0 0

0

cos ,

x z

j jk x (^) jk z jk

z z z

f k e e dk f k k e e

k

 

 (^)  

 

line source