kavoshcom rf communication circuits. impedance and admittance matrices impedance matrix admittance...
TRANSCRIPT
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KAVOSHCOM
RF Communication Circuits
Dr. Fotowat-AhmadiSharif University of TechnologyFall-1391Prepared by: Siavash Kananian & Alireza Zabetian
Lecture 3: S- Parameters
Dr. Fotowat-AhmadiSharif University of TechnologyFall-1391Prepared by: Siavash Kananian & Alireza Zabetian
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Impedance and Admittance matrices
nnnnn
n
n
n I
I
I
ZZZ
ZZZ
ZZZ
V
V
V
.
.
..
.....
.....
..
..
.
.
2
1
21
22212
12111
2
1
nnnnn
n
n
n V
V
V
YYY
YYY
YYY
I
I
I
.
.
..
.....
.....
..
..
..
2
1
21
22212
12111
2
1
Impedance matrix Admittance matrix
For n ports network we can relate the voltages and currents by impedance and admittance matrices
1 ZYwhere
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Reciprocal and Lossless NetworksReciprocal networks usually contain nonreciprocal media such as ferrites or plasma, or active devices. We can show that the impedance and admittance matrices are symmetrical, so that.
Lossless networks can be shown that Zij or Yij are imaginary
jiijjiij YYor ZZ
Refer to text book Pozar pg193-195
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ExampleFind the Z parameters of the two-port T –network as shown below
Z B
Z C
Z A
Solution
V1 V2
I1 I2
CAI
ZZI
VZ
01
111
2
CCB
CCB
CB
C
I
ZZZ
ZZZ
ZZ
Z
I
V
I
VZ
2
2
02
112
1
Port 2 open-circuited
Port 1 open-circuited
CBI
ZZI
VZ
02
222
1
Similarly we can show that
CI
ZI
VZ
01
221
2
This is an example of reciprocal network!!
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S-parameters
Microwave device
Port 1 Port 2
Vi1
Vr1
Vt2
Vi2
Vr2
Vt1
Transmission and reflection coefficients
i
t
V
V
i
r
V
V
Input signalreflected signal
transmitted signal
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S-parametersVoltage of traveling wave away from port 1 is
22
21
1
11 i
i
ti
i
rb V
V
VV
V
VV
Voltage of Reflected waveFrom port 1
Voltage ofTransmitted waveFrom port 2
22
21
1
12 i
i
ri
i
tb V
V
VV
V
VV
Voltage of transmitted wave away from port 2 is
Let Vb1= b1 , Vi1=a1 , Vi2=a2 , ,2
212
i
t
V
V,
1
11
i
r
V
V
2
22and
i
r
V
V
1
121
i
t
V
V
Then we can rewrite
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S-parameters
212111 aab
221212 aab Hence
In matrix form
2
1
221
121
2
1
a
a
b
b
2
1
2221
1211
2
1
a
a
SS
SS
b
bS-matrix
•S11and S22 are a measure of reflected signal at port 1 and port 2 respectively•S21 is a measure of gain or loss of a signal from port 1 to port 2.•S12 ia a measure of gain or loss of a signal from port 2 to port 1.
Logarithmic formS11=20 log(r1) S22=20 log(r2)S12=20 log(t12)S21=20 log(t21)
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S-parameters
0111
2
1
r
r
Vi
V
VS 02
212
2
rVi
t
V
VS
01
121
1
rVi
t
V
VS
02
222
1
rVi
r
V
VS
Vr2=0 means port 2 is matched
Vr1=0 means port 1 is matched
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Multi-port network
network
Port 1
Port 2
Port
3
Port 4
Port 5
5
4
3
2
1
5554535251
4544434241
3534333231
2524232221
1514131211
5
4
3
2
1
a
a
a
a
a
SSSSS
SSSSS
SSSSS
SSSSS
SSSSS
b
bb
b
b
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Example8.56 8.56
141.8
Below is a matched 3 dB attenuator. Find the S-parameter of the circuit.
Solution
Z1=Z2= 8.56 W and Z3= 141.8 W
By assuming the output port is terminated by Zo = 50 W, then
oin
oin
Vi
r
ZZ
ZZ
V
VS
r
01
111
2
50)5056.88.141/()5056.8(8.14156.8
05050
505011
S Because of symmetry , then S22=0
)//( 231 oin ZZZZZ
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Continue
02
221
2
rVi
t
V
VS
From the fact that S11=S22=0 , we know that Vr1=0 when port 2 is matched, and that Vi2=0. Therefore Vi1= V1 and Vt2=V2
11
33132
32122
707.056.850
50
56.844.41
44.41
//
//
VV
ZZ
ZV
ZZ
Z
ZZZ
ZZVVV
o
oo
o
ot
8.56 8.56
141.8 V1 V2
Therefore S12 = S21 = 0.707
Vo
0707.0
707.00S
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Lossless networkFor lossless n-network , total input power = total output power. Thus
n
iiii
n
ii bbaa
1
**
1
Where a and b are the amplitude of the signal
Putting in matrix form at a* = bt b*
=at St S* a*
Thus at (I – St S* )a* =0 This implies that St S* =I
Note that bt=atSt and b*=S*a*
In summation form
jifor
jiforSS kj
n
kki 0
1*
1
Called unitary matrix
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Conversion of Z to S and S to Z
UZUZS 1
SUSUZ 1
where
1..0
.1..
...0
0.01
U
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Reciprocal and symmetrical network
For reciprocal network
tUU Since the [U] is diagonal , thus
tZZ
tSS
Since [Z] is symmetry
Thus it can be shown that
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ExampleA certain two-port network is measured and the following scattering matrix is obtained:
From the data , determine whether the network is reciprocal or lossless. If a short circuit is placed on port 2, what will be the resulting return loss at port 1?
oo
oo
S02.0908.0
908.001.0
Solution
Since [S] is symmetry, the network is reciprocal. To be lossless, the S parameters must satisfy
jifor
jiforSS kj
n
kki 0
1*
1
|S11|2 + |S12|2 = (0.1)2 + (0.8)2 = 0.65
Since the summation is not equal to 1, thus it is not a lossless network.
For i=j
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continueReflected power at port 1 when port 2 is shorted can be calculated as follow and the fact that a2= -b2 for port 2 being short circuited, thus
b1=S11a1 + S12a2 = S11a1 - S12b2
b2=S21a1 + S22a2 = S21a1 - S22b2
(1)
(2)
From (2) we have
a2
-a2=b2
Short at port 2
122
212 1
aS
Sb
633.0
2.01
8.08.01.0
1 22
211211
1
21211
1
1
jj
S
SSS
a
bSS
a
b
Dividing (1) by a1 and substitute the result in (3) ,we have
(3)
dB97.3633.0log20log20 Return loss
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ABCD parameters
NetworkV1V2
I1 I2
Voltages and currents in a general circuit
122 VVI 212 IIV
This can be written as
221 IVV 221 IVI
Or
221 BIAVV 221 DICVI
A –ve sign is included in the definition of D
In matrix form
Given V1 and I1, V2 and I2 can be determined if ABDC matrix is known.
2
2
1
1
I
V
DC
BA
I
V
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Cascaded network
a b
I1a
V1a
I2a
V2a V1b
I1b I2b
V2b
a
a
aa
aa
a
a
I
V
DC
BA
I
V
2
2
1
1
b
b
bb
bb
b
b
I
V
DC
BA
I
V
2
2
1
1
However V2a=V1b and –I2a=I1b then
b
b
bb
bb
aa
aa
a
a
I
V
DC
BA
DC
BA
I
V
2
2
1
1
Or just convert to one matrix
b
b
a
a
I
V
DC
BA
I
V
2
2
1
1
Where
bb
bb
aa
aa
DC
BA
DC
BA
DC
BA
The main use of ABCD matrices are for chaining circuit elements together
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Determination of ABCD parameters221 BIAVV 221 DICVI
Because A is independent of B, to determine A put I2 equal to zero and determine the voltage gain V1/V2=A of the circuit. In this case port 2 must be open circuit.
02
1
2
I
V
VA for port 2 open circuit for port 2 short circuit
for port 2 open circuit for port 2 short circuit
02
1
2
I
V
IC
02
1
2
V
I
ID
02
1
2
V
I
VB
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ABCD matrix for series impedanceZ
I1I2
V1V2
02
1
2
I
V
VA
02
1
2
V
I
VB
02
1
2
I
V
IC
02
1
2
V
I
ID
for port 2 open circuit for port 2 short circuit
for port 2 open circuit for port 2 short circuit
V1= V2 hence A=1 V1= - I2 Z hence B= Z
I1 = - I2 = 0 hence C= 0 I1 = - I2 hence D= 1
The full ABCD matrix can be written
10
1 Z
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ABCD for T impedance network
Z1 Z2
Z3V1
I1 I2
V2
02
1
2
I
V
VA for port 2 open circuit
131
32 V
ZZ
ZV
then
therefore
3
1
3
31
2
1 1Z
Z
Z
ZZ
V
VA
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Continue
02
1
2
V
I
VB for port 2 short circuit
1
32
321
32
32
2V
ZZZZ
Z
ZZ
ZZ
VZ
Solving for voltage in Z2
But
222ZIVZ
Hence
3
2112
2
1
Z
ZZZZ
I
VB
I2Z1
Z3Z2
VZ2
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Continue
02
1
2
I
V
IC for port 2 open circuit
I1 I2
Z1
Z3V2
31322 ZIZIV
12 II
32
1 1
ZV
IC
Therefore
Analysis
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Continue
02
1
2
V
I
ID for port 2 short circuit I2
Z1
Z3Z2
VZ2
132
32 I
ZZ
ZI
I1
I1 is divided into Z2 and Z3, thus
Hence
3
2
2
1 1Z
Z
I
ID
Full matrix
3
2
3
3
2121
2
1
11
1
Z
Z
Z
Z
ZZZZ
Z
Z
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ABCD for transmission line
Input V1
I1
V2
I2
Zo gTransmission line
z =0z = -
For transmission line
ztjb
ztjf eeVeeVzV )(
ztjb
ztjf
oeeVeeV
ZzI 1)(
b
b
f
fo I
V
I
VZ
f and b represent forward and backward propagation voltage and current Amplitudes. The time varying term can be dropped in further analysis.
ztjb
ztjf eeVeeV
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continueAt the input z = -
eVeVVV bf)(1 eVeV
ZII bf
o
1)(1
At the output z = 0
bf VVVV )0(2 bf
oVV
ZII
1)0(2
(1) (2)
(3) (4)
Now find A,B,C and D using the above 4 equations
02
1
2
I
V
VA for port 2 open circuit
For I2 =0 Eq.( 4 ) gives Vf= Vb=Vo giving
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continueFrom Eq. (1) and (3) we have
)cosh(2
)(
o
o
V
eeVA
Note that
2
)()cosh(
xx eex
2
)()sinh(
xx eex
02
1
2
V
I
VB for port 2 short circuit
For V2 = 0 , Eq. (3) implies –Vf= Vb = Vo . From Eq. (1) and (4) we have
)sinh(2
)(
oo
oo ZV
eeVZB
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continue
02
1
2
I
V
IC for port 2 open circuit
For I2=0 , Eq. (4) implies Vf = Vb = Vo . From Eq.(2) and (3) we have
ooo
o
ZZV
eeVC
)sinh(
2
)(
02
1
2
V
I
ID for port 2 short circuit
For V2=0 , Eq. (3) implies Vf = -Vb = Vo . From Eq.(2) and (4) we have
)cosh(2
)(
oo
oo
VZ
eeVZD
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continue
The complete matrix is therefore
)cosh()sinh(
)sinh()cosh(
o
o
Z
Z
)cos()sin(
)sin()cos(
kZ
kj
kjZk
o
o
When the transmission line is lossless this reduces to
Note that
)cos()cosh( kjk
)sin()sinh( kjjk
jk
Wherea= attenuationk=wave propagation constant
Lossless linea = 0
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Table of ABCD network
Transmission line
Series impedance
Shunt impedance
)cosh()sinh(
)sinh()cosh(
o
o
Z
Z
10
1 Z
1
101
Z
Z
Z
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Table of ABCD network
T-network
p-network
3
2
3
3
2121
2
1
11
1
Z
Z
Z
Z
ZZZZ
Z
Z
1
3
21
3
21
32
3
111
1
Z
Z
ZZ
Z
ZZ
ZZ
Z
n
n1
0
0Ideal transformer
n:1
Z1 Z2
Z3
Z3
Z1 Z2
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Short transmission line
)cos(
)sin()sin()cos(
kZ
kj
kjZkABCD
o
o
tlineLossless transmission line
If << l then cos(k ) ~ 1 and sin (k ) ~ k then
1
11
kZ
j
kjZABCD
o
o
tlineshort
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Embedded short transmission line
Z1 Z1Transmission line
1
101
111
11
01
11 Zk
Zj
kjZ
ZABCD
o
o
embed
12
11
1
12
1
Z
kjZ
Z
kj
Z
kjZ
Z
kjZZ
kjZ
ABCDo
o
o
oo
embed
Solving, we have
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Comparison with p-network
1
3
21
3
21
32
3
111
1
Z
Z
ZZ
Z
ZZ
ZZ
Z
ABCD net
12
11
1
12
1
Z
kjZ
Z
kj
Z
kjZ
Z
kjZZ
kjZ
ABCDo
o
o
oo
embed
It is interesting to note that if we substitute in ABCD matrix in p-network, Z2=Z1 and Z3=jZok we see that the difference is in C element where wehave extra term i.e
oZ
kj
o
o
Z
k
Z
kZ
21
Both are almost same if So the transmission line exhibit a p-network
![Page 35: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/35.jpg)
Comparison with series and shunt
Series
If Zo >> Z1 then the series impedance kjZZ o
This is an inductance which is given byc
ZL o
Where c is a velocity of light
Shunt
If Zo << Z1 then the series impedance
cZC
o
This is a capacitance which is given by
oZ
kjZ
![Page 36: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/36.jpg)
Equivalent circuits
Zo ZoZoc
Zo ZoZoL
c
ZL o
cZC
o
Zo >> Z1
Zo << Z1
![Page 37: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/37.jpg)
Transmission line parameters
C
BZo
1ln
1cosh
1 21 AAA
It is interesting that the characteristic impedance and propagation constant of a transmission line can be determined from ABCD matrix as follows
![Page 38: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/38.jpg)
Conversion S to ABCD
DZCZBAZZ
BCADZDZCZBAZ
DZCZBAZSS
SS
oooo
oooo
ooo2
2
22221
1211
2
21
For conversion of ABCD to S-parameter
For conversion of S to ABCD-parameter
2112221121122211
2112221121122211
211111
11111
2
1SSSSSSSS
Z
SSSSZSSSS
SDC
BA
o
o
Zo is a characteristic impedance of the transmission line connected to theABCD network, usually 50 ohm.
![Page 39: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/39.jpg)
MathCAD functions for conversionFor conversion of ABCD to S-parameter
For conversion of S to ABCD-parameter
2,21,22,11,1
1,22,12,21,12,21,22,11,1
2,21.22,11,1 .....2
....2....
....
1)(
AZAZZAAZZ
AAAAZAZAZZAAZ
AZAZZAAZAS
1,22,12,21,11,22,12,21,1
1,22,12,21,11,22,12,21,1
1,2 .1.1.1.1.1
.1.1..1.1
..2
1)(
SSSSSSSSZ
SSSSZSSSS
SSA
o
![Page 40: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/40.jpg)
Odd and Even Mode AnalysisUsually use for analyzing a symmetrical four port network
•Equal ,in phase excitation – even mode•Equal ,out of phase excitation – odd mode
(1) Excitation
(2) Draw intersection line for symmetry and apply •short circuit for odd mode•Open circuit for even mode
(3) Also can apply EM analysis of structure•Tangential E field zero – odd mode•Tangential H field zero – even mode
(4) Single excitation at one port= even mode + odd mode
![Page 41: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/41.jpg)
Example 1
Line ofsymmetry
1 2
43
odevodevodevodev
odevodevodevodev
odevodevodevodev
odevodevodevodev
SSSSSSSS
SSSSSSSS
SSSSSSSS
SSSSSSSS
S
4444434342424141
3434333332323131
2424232322222121
1414131312121111
2
1
The matrix contains the odd and even parts
Since the network is symmetry, Instead of 4 ports , we can only analyze 2 port
Edge coupled line
![Page 42: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/42.jpg)
continueWe just analyze for 2 transmission lines with characteristic Ze and Zo respectively. Similarly the propagation coefficients be and bo respectively. Treat the odd and even mode lines as uniform lossless lines. Taking ABCD matrix for a line , length l, characteristic impedance Z and propagation constant b,thus
)cos()sin(
)sin()cos(
Zj
jZABCD
tline
DZCZBAZZ
BCADZDZCZBAZ
DZCZBAZS
oooo
oooo
ooo2
2
2 2
21
Using conversion
![Page 43: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/43.jpg)
continue
Z
ZZjZ
ZZ
ZZj
Z
ZZjZ
So
o
oo
o22
22
2
22
sin2
2sin
sincos2
1
Taking 2
Then
22
22
22 2
21
oo
oo
o ZZZZj
ZZjZZ
ZZS
(equivalent to quarter-wavelength transmission line)
![Page 44: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/44.jpg)
continue
S11
S21
S12
S22
2-port network matrix
Convert toS11
S21
S12
S22
S11
S21
S12
S22
S11
S21
S12
S22
S11
S21
S12
S22
S33
S44
S34
S43
S13 S14S23
S24
S32
S31
S42S41
4-port network matrix
Odd + even
![Page 45: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/45.jpg)
continue
Assuming bev = bod = Then
222223321441 2 ood
od
oev
evo
ZZ
Z
ZZ
ZjZSSSS
)(
)(
)(
)(
2 2222
2
ood
evod
oev
oodevo
ZZ
ZZ
ZZ
ZZZjZ
2
For perfect isolation (I.e S41=S14=S32=S23=0 ),we choose Zev and Zod such that Zev Zod=Zo
2.
S11
S21
S12
S22
S13
S23
S14
S24
S31
S41
S32
S42
S33
S43
S34
S44
ev+ od
ev+ od
ev- od
ev- od
Follow symmetrical properties
![Page 46: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/46.jpg)
continue
Similarly we have
22
22
22
22
44332211 2
1
ood
ood
oev
oev
ZZ
ZZ
ZZ
ZZSSSS
))((2
12222
422
oodoev
oodev
ZZZZ
ZZZ
Equal to zero if Zev Zod=Zo2.
S11
S21
S12
S22
S13
S23
S14
S24
S31
S41
S32
S42
S33
S43
S34
S44
ev+ od
ev+ od
ev- od
ev- od
![Page 47: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/47.jpg)
continue
We have
22
22
22
22
42241331 2
1
ood
ood
oev
oev
ZZ
ZZ
ZZ
ZZSSSS
))((
)(2222
222
oodoev
oodev
ZZZZ
ZZZ
if Zev Zod=Zo2.
odev
odev
ZZ
ZZ
S11
S21
S12
S22
S13
S23
S14
S24
S31
S41
S32
S42
S33
S43
S34
S44
ev+ od
ev+ od
ev- od
ev- od
![Page 48: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/48.jpg)
continue
222243341221 2 ood
od
oev
evo
ZZ
Z
ZZ
ZjZSSSS
odevo
ZZjZ
1if Zev Zod=Zo
2.
S11
S21
S12
S22
S13
S23
S14
S24
S31
S41
S32
S42
S33
S43
S34
S44
ev+ od
ev+ od
ev- od
ev- od
![Page 49: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/49.jpg)
continue
12
412
312
212
11 SSSS
(1) Power conservation
Reflected power transmitted
power to port 4
transmitted power to
port 3
transmitted power to
port 2
Since S11 and S41=0 , then
12
312
21 SS
(2) And quadrature condition221
11
S
SArg
This S-parameter must satisfy network characteristic:
![Page 50: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/50.jpg)
continueFor 3 dB coupler
2
12
odev
odev
ZZ
ZZ2
1
odev
odev
ZZ
ZZor
Rewrite we have
223)2(1
)2(1
od
ev
Z
Z
In practice Zev > Zod so 83.5223 od
ev
Z
Z
However the limitation for coupled edge
2od
ev
Z
Z(Gap size ) also bev and bod are not pure TEM
thus not equal
![Page 51: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/51.jpg)
A l/4 branch line coupler
Z 2
Z1
Z 2
Z1
1
3
2
4
90 o
90 o
90 o90 o
Z 2
Z1
Z1
1 2
90 o
45 o45 o
Z 2
Z1
Z1
1 2
90 o
45 o45 o
O/C O/C
Symmetrical line
Odd
Even
![Page 52: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/52.jpg)
AnalysisStub odd (short circuit) 11, 4
tan ZZX ods
Stub even (open circuit) 11, 4cot ZZX evs
The ABCD matrices for the two networks may then found :
ss
s
ss X
Z
X
jZ
Z
j
jZX
Z
jXZ
jjZ
jXABCD
222
2
22
2
2
11
01
0
0
11
01
stub stubTransmission line
![Page 53: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/53.jpg)
continue
DZCZBAZZ
BCADZDZCZBAZ
DZCZBAZS
oooo
oooo
ooo2
2
2 2
21
Convert to S
2
2
22
2
2
2
2
22
2
2
2
2
22
2
22 2
2
2
1
Z
Zj
X
ZZjjZZ
ZZ
Zj
X
ZZjjZ
Z
Zj
X
ZZjjZ
X
ZZ o
s
oo
oo
s
o
o
s
o
s
o
For perfect isolation we require
011111111 odevodev SSSS Thus 01111 odev SS
02
2
22
2
211 Z
Zj
X
ZZjjZS o
s
o or 122
2
2 ZZZ
ZZX
o
os
From
previous definition
![Page 54: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/54.jpg)
continueSubstituting into S-parameter gives us
0
01
222
2 o
o
o
odd Z
Z
jZZZS
0
01
222
2 o
o
o
even Z
Z
jZZZSand
Therefore for full four port
o
odev Z
ZjSSSSSS 2
212134431221 2
1
2
22
212123321441 12
1
oodev
Z
ZSSSSSS
And
044332211 SSSS
024421331 SSSS
![Page 55: KAVOSHCOM RF Communication Circuits. Impedance and Admittance matrices Impedance matrix Admittance matrix For n ports network we can relate the voltages](https://reader035.vdocuments.us/reader035/viewer/2022062304/56649c755503460f94929a35/html5/thumbnails/55.jpg)
continue
For power conservation and quadrature conditions to be met
Equal split S
2
1221
oZ
ZS or
22
oZZ
And
o
oo
oo
o
os Z
ZZ
ZZ
ZZ
ZZZX
2
222
2
21
2
2
If Zo= 50 W then Z2 = 35.4 W