Complex conjugate matching produces the maximum small signal transfer of power from a source that is not a transmission line to a load at the sacrifice of:...
Maximizing power transfer versus power efficiency
The theorem was originally misunderstood (notably by Joule) to imply that a system consisting of an electric motor driven by a battery could not be more than 50% efficient since, when the impedances were matched, the power lost as heat in the battery would always be equal to the power delivered to the motor. In 1880 this assumption was shown to be false by either Edison or his colleague Francis Robbins Upton, who realized that maximum efficiency was not the same as maximum power transfer. To achieve maximum efficiency, the resistance of the source (whether a battery or a dynamo) could be made close to zero. Using this new understanding, they obtained an efficiency of about 90%, and proved that the electric motor was a practical alternative to the heat engine.
Conjugate matching is not the same as reflectionless matching, which refers to matching the load to the line impedance,ZL=Z0, in order to prevent reflections from the load.
Your calculations are right, Γ is not 0. Here is most interesting links I've found to help with your question:
1. http://www.analog-rf.com/match.shtml
2. **broken link removed**
3. http://www.ece.rutgers.edu/~orfanidi/ewa/ch13.pdf
From [1]:
From [2]:
From[3]:
to be honest, I do not have good understanding on this topic. I think that reading on basic theory like in [3] may help. Maybe someone with better understanding will clarify your question.
This is a reflection coefficient for Voltage Wave.When we calculate the reflection coefficient of the circuit,
we use Γ=(ZL-Zg)/(ZL+Zg).
Reflection coefficient for Voltage Wave is not zero.What if Zg is conjugate matching we ZL which means Zg=ZL*, and Zg=R+jX, ZL=R-jX?
The Γ is not 0.
Reflection coefficient for Power Wave is zero.I think the conjugate matching make sure that there is no power reflect back to source generator so the Γ should be 0.
Wrong.Reflection coefficient is no useful parameter to describe conjugate matching.
//****************************************************************************
/*BEGIN_DOC
FUN_NAME:zin()
FUN_DESCRIPTION: Given a reflection coefficient and the reference impedance, this measurement returns the input impedance looking into the measurement ports.
RETURNED_VALUE: Integer, real or complex
CATEGORY: S-Parameter
SYNTAX: z = zin(Sii, Z)
EXAMPLE: zIN = zin(S11, 50.0)
ARGUMENT
ARG_NAME: Sii
ARG_DESCRIPTION: complex reflection coefficient.
ARG_DEFAULT: None
ARG_RANGE: (-inf:inf)
ARG_TYPE: Complex
ARG_REQUIRED: YES
ARGUMENT
ARG_NAME: zRef
ARG_DESCRIPTION: reference impedance
ARG_DEFAULT: 50.0
ARG_RANGE: (-inf:inf)
ARG_TYPE: Integer, real or complex
ARG_REQUIRED: NO
DEFINED IN: $HPEESOF_DIR/expressions/ael/network_fun.ael
SEE ALSO: vswr(), yin()
EXTERNAL: yes
AUTHOR: Agilent Technologies
DATE: Unknown
VERSION_CREATED: ADS 1.0
END_DOC*/
//****************************************************************************
defun zin(sii,zRef)
{
decl zi = if (zRef == NULL) then 50.0 else zRef;
return (conj(zi)+zi*sii)/(1-sii);
}
ADS2016 give S11 as Voltage-Reflection Coefficient ?Keysight ADS 2016:
ADS2016 give S11 as Voltage-Reflection Coefficient ?
Power Wave Formulation in ADS is well known in FAQ.I haven't seen your conjugate S11 definition before.
Show me result of "zin(0.0, 50+j*50)" in Data Display Window.Yes, obviously.
That is also consistent with the S11 definition that our RF/microwave textbooks are teaching.
Show me result of "zin(0.0, 50+j*50)" in Data Display Window.
I noticed that your usage of "S1P_Eqn" is wrong in https://www.edaboard.com/attachment.php?attachmentid=147815&d=1531330031But anyway, I've been a happy RF/μW engineer for decades now
without power wave reflection coefficient definition,
using real impedance reference values with the non-conjugate equation from textbooks
zin() is surely for Power Wave formulation even in ADS2016."Given a reflection coefficient and the reference impedance,
this measurement returns the input impedance looking into the measurement ports."
I wonder what the highlighted section really means.
It doesn't say this is the impedance of the DUT,
the wording is a bit strange.
I noticed that your usage of "S1P_Eqn" is wrong in https://www.edaboard.com/attachment.php?attachmentid=147815&d=1531330031
Z[1] is a "Port reference impedance" not input impedance.
I've been a happy RF/μW engineer for decades invariablyYou are correct, my testcase was wrong!
using complex impedance reference values with the conjugate equation from RF expert textbooks
**broken link removed**
No.Maybe that topics is teached differently in Japan, due to Kurokawa's efforts?
No.They suggest that Pseudowaves "have long been a cornerstone of microwave circuit theory"
but I've only found a couple publications that mention pseudowaves or pseudo s parameters (aside from the author's other works),
and the first use of the term came 27 years after Kurokawa's paper.
"Microwave Engineering" Written by David M. PozarGeneralized S-parameters where port impedances are complex value are not taught at all even in Japan.
For example, see the following standard text book on microwave engineering.
**broken link removed**
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