Appendix D.Two-port parameter conversion
.pdfRadio Frequency Circuit Design. W. Alan Davis, Krishna Agarwal
Copyright 2001 John Wiley & Sons, Inc.
Print ISBN 0-471-35052-4 Electronic ISBN 0-471-20068-9
APPENDIX D
Two-Port Parameter Conversion
D.1 TWO-PORT VOLTAGE AND WAVE PARAMETERS
Conversion between the z, y, h, and g two-port voltage-current parameters is simply rearrangement of two linear equations relating voltages and currents at the two ports. Converting between these and the S parameters requires relating the voltage waves to voltages and currents. This latter relationship always includes the characteristic impedance, Z0, by which the S parameters are defined. Typically this value is 50 . Table D.1 shows this conversion. The program PARCONV is basically a code of many of the conversions in Table D.1.
The definitions of the various two-port parameters are described below. In each case it is assumed that the current is flowing into the port terminal.
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z11 |
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292
293
TABLE D.1 S-Parameter Conversion Chart
S |
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ABCD |
S11
S12
S21
S22
z11
z12
z21
z22
y11
y12
y21
y22
A
B
C
D
S11
S12
S21
S22
1 C S11 1 S22 C S12S21 Z0 1 S11 1 S22 S12S21
2S12
Z0 1 S11 1 S22 S12S21
2S21
Z0 1 S11 1 S22 S12S21
1 S11 1 C S22 C S12S21 Z0 1 S11 1 S22 S12S21
1 S11 1 C S22 C S12S21 Y0 1 C S11 1 C S22 S12S21
2S12
Y0 1 C S11 1 C S22 S12S21
2S21
Y0 1 C S11 1 C S22 S12S21
1 C S11 1 S22 C S12S21 Y0 1 C S11 1 C S22 S12S21
1 C S11 1 S22 C S12S21
2S21
Z0
1 C S11 1 C S22 S12S21
2S21
1 1 S11 1 S22 S12S21
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2S21 |
1 S11 1 C S22 S12S21
2S21
z11 Z0 z22 C Z0 z12z21
z11 C Z0 z22 C Z0 z12z21
2z12Z0
z11 C Z0 z22 C Z0 z12z21
2z21Z0
z11 C Z0 z22 C Z0 z12z21 z11 C Z0 z22 Z0 z12z21
z11 C Z0 z22 C Z0 z12z21
z11
z12
z21
z22 z22
z11z22 z12z21z12
z11z22 z12z21z21
z11z22 z12z21 z11
z11z22 z12z21 z11
z21
z11z22 z12z21
z21
1
z21 z22
z21
Y0 y11 Y0 C y22 C y12y21
Y0 C y11 Y0 C y22 y12y21
2y12Y0
Y0 C y11 Y0 C y22 y12y21
2y21Y0
Y0 C y11 Y0 C y22 y12y21 Y0 C y11 Y0 y22 C y12y21
Y0 C y11 Y0 C y22 y12y21
y22
y11y22 y12y21y12
y11y22 y12y21y21
y11y22 y12y21 y11
y11y22 y12y21
y11
y12
y21
y22
y22
y21
1
y21
y11y22 y12y21 y21
y11
y21
A C B/Z0 CZ0 D
A C B/Z0 C CZ0 C D
2 AD BC
A C B/Z0 C CZ0 C D
2
A C B/Z0 C CZ0 C DA C B/Z0 CZ0 C D
A C B/Z0 C CZ0 C D
A
C
AD BC
C
1
C
D
C
D
B
BC AD
B
1
B
A
B
A
B
C
D
294 TWO-PORT PARAMETER CONVERSION
For conversion to and from S parameters for circuits with more than two ports, the following formulas may be used [1]. Each variable is understood to be a matrix representing the S, z, or y parameters. The conversion formulas are
SD F Z GŁ Z C G 1F 1 Z D F 1 I S 1 SG C GŁ F
SD F I GŁY I C GY 1F 1 Y D F 1G 1 I C S 1 I S F
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D.7
D.8
D.9
D.10
D.11
D.12
The I in Eqs. (D.8) through (D.10) is the square identity matrix, and the Z0i, i D 1, . . . , n, are the characteristic impedances associated with each of the ports. An example of the usage of PARCONV is shown below. In using the program make sure to include the decimals with the input data. The bold values represent user inputs to the program. To exit the program, use Ctrl. C.
TYPE SOURCE AND LOAD REFERENCE IMPEDANCE Z01,Z02 =
50.,50.
Y --> S = YS OR S --> Y = SY
Z --> S = ZS OR S --> Z = SZ
ABCD --> S = AS OR S --> ABCD = SA H --> S = HS OR S --> H = SH
H --> Z = HZ OR Z --> H =ZH
SY
INPUT S11, MAG. AND PHASE (deg)
.9,-80.
INPUT S21, MAG. AND PHASE (deg)
1.9,112.
INPUT S12, MAG. AND PHASE (deg)
.043,48.
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REFERENCES |
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INPUT S22, MAG. AND PHASE (deg) |
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.7,-70. |
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Y --> S = YS OR S --> Y = SY |
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Z --> S = ZS OR S --> Z = SZ |
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ABCD --> S = AS OR S --> ABCD = SA |
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H --> Z = HZ OR Z --> H =ZH |
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TABLE D.2 S Parameter to Hybrid Parameter Conversion Chart |
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S11 |
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h11 Z0 h22Z0 C 1 h12h21Z0 |
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h11 C Z0 h22Z0 C 1 h12h21Z0 |
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S22 |
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h11 C Z0 1 h22Z0 C h12h21Z0 |
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h11 C Z0 h22Z0 C 1 h12h21Z0 |
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1 C S11 1 C S22 S12S21 |
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h11 |
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2S12 |
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1 S11 1 C SS22 C S12S21 |
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2S21 |
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h21 |
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1 S11 1 C SS22 C S12S21 |
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h22 |
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Z0 1 S11 1 C SS22 C S12S21 |
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REFERENCES
1.K. Kurokawa, “Power Waves and the Scattering Matrix,” IEEE Trans. Microwave Theory Tech., Vol. MTT-11, pp. 194–202, 1965.