ECE 6341 HW 2: Analysis of Leaky Modes in Dielectric Slabs and Rectangular Waveguides, Assignments of Electrical and Electronics Engineering

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, as well as deriving the exact expression for the electric field above the interface and the far-field pattern for the tex leaky mode. Additionally, the document includes problems on plotting the magnitude of the normalized far-field pattern and the electric field versus angle and position, respectively.

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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
β
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)
()
(
)
() ( )
11
1
n
nnnn
nn
fz
zzzz fz fz
+−
⎛⎞
=− ⎜⎟
⎜⎟
⎝⎠
.
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
EzAe
=
where LW
zzz
kj
β
α
=− and A is an amplitude constant. The exact electric field above the
interface is
.
where
()
1/2
22
0xz
kkk=− . The branch of the square root is chosen so that that Im 0.
x
k
<
Show that
() ()
1
,0, ,
2xz
jk x jk z
yyzz
Exz E ke e dk
π
−∞
=
()
()
lw
2
lw 2
0, 2 z
yz
zz
k
Ek jA
kk
⎛⎞
⎜⎟
=− ⎜⎟
⎝⎠
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 β/ k 0

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 f (^) s. Then, for a frequency that is 10% lower than the splitting point frequency (i.e., f = 0.9 f (^) s ) 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

  • − −
  1. 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

jk LWz z E (^) y z Ae − =

where k zLW = β z − j α z and A is an amplitude constant. The exact electric field above the

interface is .

where ( )

2 2 1/ 2 k (^) x = k 0 − kz. The branch of the square root is chosen so that that Im k (^) x <0. Show that

jk x x jk zz

E y x z π E y kz e e dkz

∞ − − −∞

lw 0, (^2) lw 2 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 f ( k z ) is an arbitrary function of k z , ( )

2 2 1/

k x = k 0 − kz , k z 0 = k 0 sin θ, and

x = ρ cosθ, z = ρ sinθ. Assuming this relation, derive the far-field pattern EyFF ( ρ ,θ)

of the TE x leaky mode.

5) Assume that we have a TE x leaky mode with β z = ( 3 / 2) k 0 and α z = 0.002 k 0. Plot the

magnitude of the normalized far-field pattern EyFF ( ρ ,θ ) versus angle θ from –90o^ to

90 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 E y ( x z , ) (not in

dB) versus x. Plot over the range 0 < x < 20 λ 0 for the following fixed values of z : z = 1 λ 0 , 5 λ 0 ,10 λ 0 , 50 λ 0 ,100λ 0. 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 β z = ( 1.5) k 0 and α z = 0.002 k 0. 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 k (^) z and the cutoff frequencies for all

h ε r

z

x

0 4 0 0 0

x z cos ,

jk x jk z jk j

f k z e e dk z f k z k k e e

π θ π^ ρ ρ

∞ − − − −∞

line source