spring 2015 - university of houstoncourses.egr.uh.edu/ece/ece6345/class notes/topic 10 spectral...
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Spring 2015
Notes 25
ECE 6345
Prof. David R. Jackson ECE Dept.
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Overview
In this set of notes we use the spectral-domain method to find the input impedance of a rectangular patch antenna. This method uses the exact spectral-domain Green’s function, so all radiation physics, including surface-wave excitation, is automatically included (no need for an effective permittivity). It does not account for the probe inductance (the way it is formulated here), so the CAD formula for probe inductance is added on at the end.
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D. M. Pozar, “Input impedance and mutual coupling of rectangular microstrip antennas,” IEEE Trans. Antennas and Propagation, vol. 30, pp. 1291-1196, Nov. 1982.
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Spectral Domain Method
x
z
L
0 0( , )x yh
sxJ
izJ rε
0 1 [ ]I A=
Set 0=xE ( ) Syx ∈,
[ ] [ ] 0=+ izxsxx JEJE ( ) Syx ∈,
S is the patch surface
This is the “Electric Field Integral Equation (EFIE)”
The probe is viewed as an impressed current.
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Spectral Domain Method (cont.)
Let ( ) ( )
( )
, ,
, cos
sx x x
x
J x y A B x y
xB x yLπ
=
=
[ ] 0ix x x x zA E B E J + =
Pick a “testing” function T(x,y):
[ ]{ }[ ]
( , ) 0
( , ) ( , ) 0
ix x x x z
S
ix x x x z
S S
T x y A E B E J dS
A T x y E B dS T x y E J dS
+ =
+ =
∫
∫ ∫
The EFIE is then
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Spectral Domain Method (cont.) Galerkin’s Method: xT x, y B x, y
( )
( ) [ ]
, ,,,
iix x zz xS
xx xx x x
S
B x y E J dS J BA
B BB x y E B dS
= − = −∫
∫
(The testing function is the same as the basis function.)
[ ] ( )( , ) , 0ix x x x x x z
S S
A B x y E B dS B x y E J dS + = ∫ ∫
The solution for the unknown amplitude coefficient Ax is then
Hence
5
( ), ,i iz x x z x
S
J B E J B x y dS ≡ ∫ [ ], ( , )x x x x xS
B B E B B x y dS= ∫
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Spectral Domain Method (cont.)
The input impedance is calculated as:
[ ]iz z z z sxE E J E J = +
The total field comes from the patch and the probe:
20
*2
0
2
2 12
inin
iz z
V
iz z
V
PZI
E J dVI
E J dV
=
= −
= −
∫
∫ (The probe current is real and equal to 1.0 [A].)
6
Pin = complex power coming from impressed probe current (in the presence of the patch).
V = volume of probe current
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Spectral Domain Method (cont.) Hence
[ ]i i iin z z z z z sx
V V
Z J E J dV J E J dV = − − ∫ ∫
Then we have
[ ]iin probe z z sx
V
Z Z J E J dV= − ∫
,i i i iprobe z z z z z
V
Z J E J dV J J ≡ − = − ∫Define:
or
[ ] ,i iin probe x z z x probe x x z
V
Z Z A J E B dV Z A B J= − = −∫
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Spectral Domain Method (cont.)
We have from reciprocity that
, iin probe x x zZ Z A B J= −
so that 2
,,
ix z
in probex x
B JZ Z
B B= +
8
, ,i iz x x zJ B B J=
,,
iz x
xx x
J BA
B B= −
where
Note: Zzx is easier to calculate than Zxz.
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Spectral Domain Method (cont.) Define:
,
,xx x x
izx x z
Z B B
Z B J
≡ −
≡ −
Note: The subscript notation on Zij follows the usual MoM convention.
2zx
in probexx
ZZ ZZ
9
We then have:
Note: The minus sign is added to agree with typical MoM convention.
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Spectral Domain Method (cont.) Note: The probe impedance may be approximately calculated by using a CAD formula:
probe pZ jX
00 0
1ln ln ln/p r r r
hXa
η µ γ π µ ελ λ
= − − −
0.57722 ( )γ Euler's constant
This result comes from a probe inside of an infinite parallel-plate waveguide.
Nlote: Calculating Zprobe exactly from the spectral-domain method can be done, but this would be a lot of work, and the improvement would be small.
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Spectral Domain Method (cont.)
Hence, integrating over the patch surface, we have
[ ],xx x x x x xS
Z B B E B B dS= − = −∫
[ ]( )
( )2
12
x yj k x k yx x xx x x yE B G B e dk dk
π
∞ ∞− +
−∞ −∞
= ∫ ∫
( )( ) ( ) ( )2
1 , , ,2xx xx x y x x y x x y x yZ G k k B k k B k k dk dkπ
∞ +∞
−∞ −∞
= − − −∫ ∫
The next goal is to calculate the reactions Zxx and Zxz in closed form.
From previous SDI theory, we have
For the patch-patch reaction we have:
x xx xE G B=
so
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Spectral Domain Method (cont.)
( )( ) ( )2
21 , ,
2xx xx x y x x y x yZ G k k B k k dk dkπ
∞ ∞
−∞ −∞
= − ∫ ∫
Since the Fourier transform of the basis function (cosine function) is an even function of kx and ky, we can write:
( ) ( )22
0 0
1 , ,xx xx x y x x y x yZ G k k B k k dk dkπ
∞ ∞
= − ∫ ∫
or
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Note: z = z′ = 0 in the spectral-domain Green’s function here.
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Spectral Domain Method (cont.)
Converting to polar coordinates, we have
( ) ( )/2
22
0
1 , ,xx xx t x t t tC
Z G k B k k dk dπ
φ φ φπ
= − ∫ ∫
13
Re tk
Im tk
0k 1k
RL C
Rh
Note: The path must extend to infinity.
0TMβ
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Spectral Domain Method (cont.)
( ) 2 2
cos2, sinc
2 22 2
x
x x y y
x
LkWB k k LW k
Lk
ππ
= −
From previous calculations, we have:
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( ) 2 21 1, ,0 cos sinxx x y TM TEG k kD D
φ φ ≡ − +
( )( )
0 1 1
0 1 1
( ) cot
( ) cot
TM TM TMt z
TE TE TEt z
D k Y jY k h
D k Y jY k h
= −
= −
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Spectral Domain Method (cont.)
[ ]( )
[ ]( )0
0 0
, ,
, ,
izx z x z
V
z xh
Z E B x y z J dV
E B x y z dz−
= −
= −
∫
∫
For the patch-probe reaction we have
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( )( )
( ) ( )0 0
0 0 21, ,
2x yj k x k y
z zx x x yE x y z G z B e dk dkπ
+∞ +∞− +
−∞ −∞
= ∫ ∫
z zx sxE G J=
so
Note: Zzx is the voltage drop at the feed location due to the current Bx.
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Spectral Domain Method (cont.)
zxG~To calculate use:
1
1 y xz
H HEj x yωε
∂ ∂= − ∂ ∂
so that
( )1
1z x y y xE jk H jk H
jωε= − +
16
We need the transforms of the transverse magnetic field components.
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Spectral Domain Method (cont.)
( )( )
( ) ( ) ( )( ) ( )( )
cos sin
cos sin
cos sin
sin cos cos sin
sin cos cos sin
x u v
TE TM
TE TMi sv i su
TE TMi sx i sx
TE TMi sx i sx
H H H
I I
I J I J
I J I J
I J I J
φ φ
φ φ
φ φ
φ φ φ φ
φ φ φ φ
= + −
= + −
= + − −
= − + − −
= − +
Using spectral-domain theory, we have
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=
=
=
=
TMt x y
TMt x y
TMss x y
TEt x y
TEt x y
TEss x y
ˆV z u E k ,k ,z
ˆI z v H k ,k ,z
ˆI z u J k ,k
ˆV z v E k ,k ,z
ˆI z u H k ,k ,z
ˆI z v J k ,k
u
v tk
x
y
φ
( ),x yk k
xk
yk
φ
tk
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Spectral Domain Method (cont.)
( ) ( )( )( ) ( )2 2
sin cos
sin cos
sin cos
sin sin cos cos
sin cos
y u v
TE TM
TE TMi sv i su
TE TMi sx i sx
TE TMi i sx
H H H
I I
I J I J
I J I J
I I J
φ φ
φ φ
φ φ
φ φ φ φ
φ φ
= +
= +
= + −
= − + −
= − −
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We also have
=
=
=
=
TMt x y
TMt x y
TMss x y
TEt x y
TEt x y
TEss x y
ˆV z u E k ,k ,z
ˆI z v H k ,k ,z
ˆI z u J k ,k
ˆV z v E k ,k ,z
ˆI z u H k ,k ,z
ˆI z v J k ,k
u
v tk
x
y
φ
( ),x yk k
xk
yk
φ
tk
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Spectral Domain Method (cont.)
( )
2
2
2 2
sincos
cos
sin cossin
sin cos
cos cos sin
cos
TEi sx
x y y x t TMi sx
TEi sx
t TMi sx
TMt i sx
TMt sx i
I Jjk H jk H jk
I J
I Jjk
I J
jk I J
jk J I
φφ
φ
φ φφ
φ φ
φ φ φ
φ
− − + = − −
− + +
= +
=
We then have
cossin
x t
y t
k kk k
φ
φ
=
=
Note:
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( )1
1z x y y xE jk H jk H
jωε= − + Recall:
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Spectral Domain Method (cont.)
Hence we have
we then identify that
( ) ( )( )1
cos TMtzx i
kG z I zφωε
=
( )1
1 cos TMz t sx iE jk J I
jφ
ωε=
z zx sxE G J= Using
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Spectral Domain Method (cont.)
Hence
1( ) ( ) cos ( )TM TMi i zI z I h k z h= − +
From TL theory, we have the property that
( ) 11
cos ( )cos ( )TMtzx i z
kG z I h k z hφωε
= − +
(The short circuit at z = -h causes the current to have a zero derivative there.)
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Spectral Domain Method (cont.) For the field due to the patch basis function, we then have
( )( )
( ) ( )
( )( ) ( )
( )( ) ( )
0 0
0 0
0 0
0 0 2
2
121
1, ,2
12
1 cos ( ) cos ( )2
x y
x y
x y
j k x k yz z x y
j k x k yzx x x y
j k x k yTMti z x x y
E x y z E z e dk dk
G z B e dk dk
k I h k z h B e dk dk
π
π
φωεπ
+∞ +∞− +
−∞ −∞
+∞ +∞− +
−∞ −∞
+∞ +∞− +
−∞ −∞
=
=
= − +
∫ ∫
∫ ∫
∫ ∫
( )0
1 1 10
cos ( ) cos sinch
z z zh
k z h dz k z dz h k h−
′ ′+ = =∫ ∫
Note that
( )0
0 0, ,zx zh
Z E x y z dz−
= − ∫
Recall that
z z h′ = + 22
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Spectral Domain Method (cont.)
( )( ) ( ) ( )0 0
121
1 ( ) cos sinc2
x yj k x k yTMtzx i x z x y
kZ I h B h k h e dk dkφωεπ
+∞ +∞− +
−∞ −∞
= − −∫ ∫
Hence we have
cos x
t
kk
φ =
where
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Spectral Domain Method (cont.)
The result is then
( ){ }( ) ( )
/2
121 0 0
0 0
( ) cos sinc
sin cos
TMzx t i x z
x y t t
j hZ k I h B k h
k x k y k dk d
π
φπ ωε
φ
∞ = + −
⋅
∫ ∫
The integrand is an even function of ky and an odd function of kx (due to the cosine term). Hence we use the following combinations to reduce the integration to one over the first quadrant:
( ) ( ) ( ) ( ) ( ) ( ) ( ) ( )
( ) ( ) ( ) ( )
( ) ( ) ( )
( ) ( )( ) ( )
0 0 0 00 0 0 0
0 0
0 0
0 0
0
0 0
0 0
2 sin 2 sin
2 sin
2 sin 2cos
4 sin cos
y y y yx x x x
y y
y y
j k y j k y j k y j k yj k x j k x j k x j k x
j k y j k yx x
j k y j k yx
x y
x y
e e e e e e e e
j k x e j k x e
j k x e e
j k x k y
j k x k y
− − + +− + + −
− +
− +
− − +
= − −
= − + = −
= −
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Quadrant 1 Quadrant 2 Quadrant 3 Quadrant 4
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Spectral Domain Method (cont.)
( ){ }( ) ( )
/22
121 0
0 0
( ) cos sinc
sin cos
TMzx t i x z
C
x y t
j hZ k I h B k h
k x k y dk d
π
φπ ωε
φ
= −
⋅
∫ ∫
The final result is then:
25
Re tk
Im tk
0k 1k
RL C
Rh
Note: The path must extend to infinity.
0TMβ
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Spectral Domain Method (cont.)
Note on material loss:
The spectral-domain method already accounts for radiation into space and into surface waves, and accounts for dielectric loss by using an complex permittivity. In order to account for conductor loss, we can use
1 1 1tan effloss d cQ Q Q
δ = = +
It is also possible to account for conductor loss by using a impedance boundary condition on the patch, but using an effective loss tangent is a simpler approach (no need to modify the code – simply increase the loss tangent to account for conductor loss).
26
tandQ δ= 0 0( )2c r ave
s
k hQR
η µ =
where
( )1 taneffr r effjε ε δ′= −
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Spectral Domain Method (cont.)
( )TMiI h−
0TMZ
1TMZ
(0)TMVz
1 [ ]A
z h= −( )TMiI h−
+ −
( )0 1 1
(0) (1)1
cot1
TM TMi in
TM TMz
TM
V Z
Y jY k h
D
=
=−
=
We now calculate the needed current function
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Spectral Domain Method (cont.)
(0)(0 )TM
TM ii TM
in
VIZ
− −=
( )1 1tanTM TMin zZ jZ k h=
( ) 1
1 11(0 ) tanTM TM
i zTMI jZ k hD
−− = −
TMinZ
(0)TMV
z
(0 )TMiI −
+ −
so
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1(0)TMi TMV
D=
From last slide:
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Spectral Domain Method (cont.) Also,
( )1(0 ) ( )cosTM TMi i zI I h k h− = −
so
( )
( ) ( )
1
1
1 1 1
( ) (0 )sec
1 tan sec
TM TMi i z
TMz zTM
I h I k h
jZ k h k hD
−
−
− =
= − Hence
( ) ( ) ( )10 1 1 1 1
1 1( ) seccot tan
TMi zTM TM TM
z z
I h k hY jY k h jZ k h
− = − −
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( )( )1( ) ( )cos 0TM TMi i zI z I h k z h h z= − + − ≤ <
And therefore
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Results
[6] E. H. Newman and P. Tulyathan, “Analysis of microstrip antennas using moment methods,” IEEE Trans. Antennas Propagat., vol. AP-29. pp. 47-53, Jan. 1981.
D. M. Pozar, “Input impedance and mutual coupling of rectangular microstrip antennas,” IEEE Trans. Antennas Propagat., vol. AP-30. pp. 1191-1196, Nov. 1982.
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Two Basis Functions
( ) ( ) ( ), , ,s x x y yJ x y A B x y A B x y= +
EFIE:
[ ][ ]
: 0
: 0
ix x x x y x y x z
iy x y x y y y y z
E A E B A E B E J S
E A E B A E B E J S
+ + = + + =
on
on
y
0 0( , )x y
S
xsxJ
syJ
L
W
Note: Using two basis
functions is important for circular polarization or
for dual-polarized patches.
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Define:
0
0
x xS
y yS
E B dS
E B dS
=
=
∫∫
, , ,
, , ,
ix x x y y x z x
ix x y y y y z y
A B B A B B J B
A B B A B B J B
+ = −
+ = −
,
,
ij j i
izi i z
Z B B
Z B J
≡ −
≡ −
Two Basis Functions (cont.) Galerkin testing:
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By symmetry,
x xx y xy xz
x yx y yy yz
A Z A Z ZA Z A Z Z
+ = −
+ = −
0xy yxZ Z= =
[ ]( ) ( )( ) ( )
, Odd
, Eveny x
y
E B x y y
B x y y
=
=
This follows since
Two Basis Functions (cont.)
( ) ( ), , ,yx x y y y xS
Z B B B x y E B x y dS= − = ∫
xy yxZ Z=
(reciprocity)
and
(from symmetry)
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Hence, the two testing equations reduce to:
= −
= −x xx xz
y yy yz
A Z ZA Z Z
xzx
xx
yzy
yy
ZA
ZZ
AZ
= −
= −
Two Basis Functions (cont.)
The solution is:
zxx
xx
zyy
yy
ZA
ZZ
AZ
= −
= −
Using reciprocity:
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Hence, using the previous results for Ax and Ay, we have
,
, ,
isin probe z
i iprobe x x z y y z
probe x zx y zy
Z Z J J
Z A B J A B J
Z A Z A Z
= −
= − −
= − +
22zyzx
in probexx yy
ZZZ Z
Z Z= − −
Two Basis Functions (cont.) As before,
[ ]iin probe z z s
V
Z Z J E J dV= − ∫ ( )sx sJ J→
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( ) ( )
2 2
2
1 = − +
y xyy
m t e tt
k kG
D k D kk
Two Basis Functions (cont.)
( ) ( )/2
22
0
1 , ,xx xx t x t t tC
Z G k B k k dk dπ
φ φ φπ
= − ∫ ∫
( ) ( )
22
2
1 yxxx
m t e tt
kkG
D k D kk
= − +
( ) ( )/2
22
0
1 , ,yy yy t y t t tC
Z G k B k k dk dπ
φ φ φπ
= − ∫ ∫
Similarly,
From our derivation:
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Two Basis Functions (cont.)
( ){ }( ) ( )
/22
121 0
0 0
( ) cos sinc
sin cos
TMzx t i x z
C
x y t
j hZ k I h B k h
k x k y dk d
π
φπ ωε
φ
= −
⋅
∫ ∫
( ){ }( ) ( )
/22
121 0
0 0
( ) sin sinc
sin cos
TMzy t i y z
C
y x t
j hZ k I h B k h
k y k x dk d
π
φπ ωε
φ
= −
⋅
∫ ∫
From our derivation:
Similarly,
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Two Basis Functions (cont.)
( ) 2 2
cos2, sinc
2 22 2
x
x x y y
x
LkWB k k LW k
Lk
ππ
= −
( ) 2 2
cos2, sinc
2 22 2
y
y x y x
y
WkLB k k WL k
Wk
ππ
= −
The transforms of the basis functions are: