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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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Spring 2009
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.
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
x leaky mode has a field on the interface ( x = 0) due to a line source at z = 0 that is
represented as
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
k k k. 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).
will be discussed later in the semester, we can asymptotically evaluate the field radiated
by the leaky mode, by using the result
z
f k (^) is an arbitrary function of z
k (^) ,
1/ 2 2
x 0 z
k k k , 0 0
sin z
k k , and
FF
y
of the TE x leaky mode.
0
z
k and 0
z
k. Plot the
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.
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.
0
z
k and 0
z
k. This
corresponds to a leaky mode that is in the non-physical region.
Derive transcendental equations for the wavenumber kz and the cutoff frequencies for all
r
0 4
0 0
0
x z
j jk x (^) jk z jk
z z z
(^)
line source