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W5DXP August 12th 03 11:25 PM

Roy Lewallen wrote:
And if Cecil's work leads to the conclusion that the source impedance
impacts the line's SWR, then it's wrong.


It doesn't. In fact, just the opposite. My examples do NOT even
include a source impedance.
--
73, Cecil http://www.qsl.net/w5dxp



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Richard Clark August 12th 03 11:32 PM

On Tue, 12 Aug 2003 17:04:59 -0500, W5DXP
wrote:

Richard Clark wrote:
I see you still live in a dimensional aberration where you experience
22 days as 66 minutes.


I see that you still ignore the technical questions so I will repeat mine:
Are you saying that SWR doesn't equal (1+|rho|)/(1-|rho|)?


Hi Cecil,

Why don't you solve the first problem before presenting your own?

73's
Richard Clark, KB7QHC

Richard Clark August 12th 03 11:33 PM

On 12 Aug 2003 15:22:42 -0700, (Tom Bruhns) wrote:

Had a look at the refs. I'm curious, did you actually read the
sentence that Roy wrote?

Cheers,
Tom


Hi Tom,

Yes, did you?

73's
Richard Clark, KB7QHC

Tom Bruhns August 12th 03 11:34 PM

(Dr. Slick) wrote in message . com...
....
You're right about this, and it reminds us that if there is any
loss at all, we theoritically move away from a purely resistive
characteristic impedance into a complex one. This furthers the
complexity on the problem, as we must expect reactance in our coax.


It's not just theory, it's practice and measurable. But it's not a
requirement that loss introduce reactance to Zo; it's just that if the
line is lossless it must have a non-reactive Zo. Clearly if L/C =
R/G, the impedance will be non-reactive.

Also, consider what reactance you do get in practical lines, at what
frequencies. What effect does frequency have on the reactance? Why?
Under what conditions will it really be a problem? Might the reactive
part be so small that it will be totally swamped out by variations in
the real part? Think a bit about how much it will or won't mess up
the measurements you want to make.

Cheers,
Tom

Tarmo Tammaru August 13th 03 12:34 AM


"W5DXP" wrote in message
...
Dr. Slick wrote:
I didn't think you could tell us. I've never seen an SWR meter
that you could "calibrate" to 50 or 75 ohms, or less.


The calibration of the SWR meter is controlled by the internal sampling
load resistor, the 'R' in Peter's V + IR equation. I have a home-brewed
SWR meter that measures SWR on both balanced 450 ohm feedlines and on
300 ohm feedlines simply by changing the internal load resistors.
--
73, Cecil http://www.qsl.net/w5dxp

Cecil,

When you do this, does the scale still display the correct SWR for
conditions other than 1:1 ?

Tam/WB2TT



Richard Clark August 13th 03 12:52 AM

On Tue, 12 Aug 2003 15:52:05 -0700, Roy Lewallen
wrote:

It's admittedly hard for me to follow what you've written, but it sounds
like you're saying that:


Hi Roy,

1. Source impedance affects line SWR, and
2. It's impossible to tell by how much.

Did I get that right?

No. The sources offered and the data exhibited provide a very clear
answer. To state this yet again, it is the lack of knowledge in the
distances traversed between reflecting interfaces that introduces the
Mismatch Uncertainty. A smart lad might conspire to present any
particular Power measurement if he could withhold other details from
scrutiny. A lad who considered himself smart may do the same but
think he invented a free power amplifier (or dissipationless load).

This is simply an account of poor boundary controls that turn some
folk into magicians and others into the reincarnation of Galileo.
Either outcome is achieved through delusion.

Incidentally, you've brought up a new topic, that of an SWR meter.

Look at the Subject line.

As for the aside about SWR meter reading, I have performed SWR
measurements with a variety of NBS methods (many hundreds of times) -
none of them described here very often, and some never at all. I
doubt any here are so well versed in these methods as to challenge my
data by employing them (it would only confirm the results). I would
be happy to see as much effort put to it - in that it would represent
a technical rebuttal rather than echoed denials. I would be happy to
retract my points if someone revealed an error of commission/omission
- such has not happened and discussion of that data has been wholly
absent.

Look Roy, skip the rhetoric (from all sources including me) and
explain or refute the data I obtained. If you cannot accept it,
reveal the error. If the method is too tedious to replicate - say so.
This is not the first time I've broached the subject and I certainly
don't expect many to care for one, or follow blithely for another. It
only matters in issues of accurate Power determination.

73's
Richard Clark, KB7QHC

W5DXP August 13th 03 04:39 AM

Tarmo Tammaru wrote:

"W5DXP" wrote:
The calibration of the SWR meter is controlled by the internal sampling
load resistor, the 'R' in Peter's V + IR equation. I have a home-brewed
SWR meter that measures SWR on both balanced 450 ohm feedlines and on
300 ohm feedlines simply by changing the internal load resistors.


When you do this, does the scale still display the correct SWR for
conditions other than 1:1 ?


The scale is calibrated using known loads so yes, it displays the
correct SWR up to 5.83:1. Above 5.83:1 the resolution of the scale
is poor because the full scale SWR is infinity. I have marks at
5.83:1 and 10:1. 5.83:1 is where the reflected power equals half
the forward power. Incidentally, the Z0 of my '450' ohm ladder-
line is closer to 388 ohms.
--
73, Cecil http://www.qsl.net/w5dxp



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Dr. Slick August 13th 03 04:52 AM

W5DXP wrote in message ...
Dr. Slick wrote:
I didn't think you could tell us. I've never seen an SWR meter
that you could "calibrate" to 50 or 75 ohms, or less.


The calibration of the SWR meter is controlled by the internal sampling
load resistor, the 'R' in Peter's V + IR equation. I have a home-brewed
SWR meter that measures SWR on both balanced 450 ohm feedlines and on
300 ohm feedlines simply by changing the internal load resistors.



BTW, how do you know the accuracy of your homebrew SWR meter?


Slick

W5DXP August 13th 03 05:03 AM

Dr. Slick wrote:
Would these be the termination resistors to ground, one for each
directional coupler?


Yes

I would think that you would have to adjust the
width of the traces as well, or the thickness of the dielectric
material, or the space between the couplers and the thru-line to use
it for an impedance other than 50 Ohms (talking about commercial
equipment, that is).


I use a toroid to sense the RF current and an R=Z0 resistor to turn it
into a voltage. I have a capacitive voltage divider on the RF voltage
which is adjustable for calibration purposes. The only real difference
between it and a 50 ohm SWR meter is the internal load resistor. It's
actually a bridge circuit with a Z0 reference resistor. Unfortunately,
it is not very accurate for the relatively high SWRs that I run on my
ladder-line, e.g. 4:1 to 16:1
--
73, Cecil http://www.qsl.net/w5dxp



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Dr. Slick August 13th 03 05:15 AM

(Tom Bruhns) wrote in message m...
(Dr. Slick) wrote in message . com...
...
You're right about this, and it reminds us that if there is any
loss at all, we theoritically move away from a purely resistive
characteristic impedance into a complex one. This furthers the
complexity on the problem, as we must expect reactance in our coax.


It's not just theory, it's practice and measurable. But it's not a
requirement that loss introduce reactance to Zo; it's just that if the
line is lossless it must have a non-reactive Zo. Clearly if L/C =
R/G, the impedance will be non-reactive.


True. Never considered this before, thank you. Makes sense that
if the ratio of the series resistance and shunt conductance are the
same as the ratio of the series inductance and shunt capacitance, that
the transmission line will still be non-reactive.


Also, consider what reactance you do get in practical lines, at what
frequencies. What effect does frequency have on the reactance? Why?
Under what conditions will it really be a problem? Might the reactive
part be so small that it will be totally swamped out by variations in
the real part? Think a bit about how much it will or won't mess up
the measurements you want to make.

Cheers,
Tom


In general, using an MFJ antenna analyzer to get a rough idea of
what the series equivalent complex impedance is (these are not $80,000
vector network analyzers!), it seems that cheap 3' RG-8x jumper coax
cables mainly add series inductance to the system, as the reactance
gets higher with increasing frequency.
We try to design 9 element chebychev low-pass filters, which is
not difficult at very low power levels, as two 1/4 watt 100 Ohm
resistors make a decent dummy load all the way out to 200 megs or so.

The problem is characterizing insertion loss using higher power
transmitters, when we know that the 1000 watt cantenna swings from 40
to 70 Ohms (with reactance too) as you get above 80 megs or so. It
become difficult to know if you are moving in the right direction or
not.

Slick

W5DXP August 13th 03 05:15 AM

Dr. Slick wrote:
BTW, how do you know the accuracy of your homebrew SWR meter?


I have a bunch of 50W 600 ohm non-inductive resistors that I use
for calibration purposes. And I really don't know the accuracy.
An SWR of 20:1 looks the same as an SWR of 25:1 on the scale.
I have an upper and lower acceptable limit to the SWRs with the
matching method I use. The SWR meter tells me if the SWR is
outside of that acceptable range.
--
73, Cecil http://www.qsl.net/w5dxp



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Roy Lewallen August 13th 03 06:48 AM

Dr. Slick wrote:

As you might know, the input S11 or SWR will change when you go
from an antenna analyzer or network analyzer to measuring with the
actual full power PA and meter hooked up. This may be partly due to
the fact that the meter is usually not a perfect 50 ohm thru, and
partly due to the fact that the analyzers outputs are closer to 50
ohms than the PA.


If S11 or the SWR actually does change, you've either got a nonlinear
transmission line or a nonlinear load. That is, the impedance changes as
the signal level changes. If you *measure* a different SWR or S11, it
means that either the SWR or S11 is actually changing for the reasons I
just stated, or the meter is nonlinear in the sense that its reading
changes with power level (possibly due to RF ingress, but it could be a
host of other things), or you're measuring with two different meters
that don't agree.

It's not because of the different source impedances.

Sure, you can normalize a Smith chart to anything you'd like. That
doesn't make the SWR change with source impedance.

. . .


Roy Lewallen, W7EL


Ian White, G3SEK August 13th 03 08:06 AM

W5DXP wrote:
Dr. Slick wrote:
BTW, how do you know the accuracy of your homebrew SWR meter?


I have a bunch of 50W 600 ohm non-inductive resistors that I use
for calibration purposes. And I really don't know the accuracy.
An SWR of 20:1 looks the same as an SWR of 25:1 on the scale.
I have an upper and lower acceptable limit to the SWRs with the
matching method I use. The SWR meter tells me if the SWR is
outside of that acceptable range.


It's interesting to see an example of an SWR meter for a Z0 that isn't
50 ohms, because it helps to confirm that they all work in basically the
same way.

If [V] is a sample of the line voltage, and [i] is a sample of the line
current, then the forward reading is the sum of two RF voltages, [V] +
[i]R, where R is the resistor that converts the [i] sample into a
voltage.

The reverse reading is the difference, [V] - [i]R. The "calibration to
Z0" procedure consists of terminating the line in the design value of
Z0, and then adjusting R so that the reverse reading [V] - [i]R is zero.

The RF voltages are either summed or subtracted, and then the resultant
is detected by the diode.

Just one small point, though... it is not necessary that R = Z0. The
value required depends on the sampling factors kV and kI that relate the
voltage and current in the line to the sampled values [V] and [i]. In
full, the instrument is calibrated to Z0 when:

kV*V - kI*I*R = 0

In a typical bridge, two out of the three constants kV, kI and R are
fixed, and the third is adjustable. In a Bruene bridge, kI is fixed by
the number of turns on the current-sampling toroid, R is fixed, and you
calibrate the bridge by adjusting the kV factor in the voltage divider.
However, it would be equally good to build-in fixed values of kV and kI,
and balance the bridge by making R a small trimpot. So R really does not
have to equal Z0... and in most published circuits, it doesn't.

This can also be shown in a different way, by thinking of it as a
Wheatstone bridge, with Z0 as one arm. The requirement for balance is
only that Z0/R2 = R3/R4. It is not necessary for any of the other
resistors R2, R3 or R4 to equal Z0 in order to achieve balance.

AFAIK, the only situation where the "terminating" resistor truly needs
to equal Z0 is in parallel-line couplers for microwaves, when the
sampling line approaches a quarter-wavelength long and its own
characteristic impedance is Z0 too.


--
73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB)
Editor, 'The VHF/UHF DX Book'
http://www.ifwtech.co.uk/g3sek

Ian White, G3SEK August 13th 03 08:21 AM

Dr. Slick wrote:
As you might know, the input S11 or SWR will change when you go
from an antenna analyzer or network analyzer to measuring with the
actual full power PA and meter hooked up. This may be partly due to
the fact that the meter is usually not a perfect 50 ohm thru, and
partly due to the fact that the analyzers outputs are closer to 50 ohms
than the PA.

Sorry, that is exactly wrong. S11, SWR and the impedance itself, do
*not* change when you connect a different instrument to the same load.
All the changes you have described are due entirely to instrument
errors.

That's how the instrument errors are determined... by knowing for a fact
that, whatever all the different instruments may say, the impedance
they're trying to measure is the one thing that has *not* changed.

--
73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB)
Editor, 'The VHF/UHF DX Book'
http://www.ifwtech.co.uk/g3sek

Dr. Slick August 13th 03 02:56 PM

"Ian White, G3SEK" wrote in message ...

Sorry, that is exactly wrong. S11, SWR and the impedance itself, do
*not* change when you connect a different instrument to the same load.
All the changes you have described are due entirely to instrument
errors.

That's how the instrument errors are determined... by knowing for a fact
that, whatever all the different instruments may say, the impedance
they're trying to measure is the one thing that has *not* changed.



You are right, but i never stated that the impedance we are
feeding ever changes, only the measured SWR.

Hey, we live in the real world, with real instrument errors. This
is the case i am talking about when i started the thread. I usually
DON'T measure the same SWR from antenna analyzer versus PA and meter
hooked up, and this may be due to the fact that the PA has a different
source impedance than the analyzer. I'm not claiming that the
impedance we are feeding has changed. And if you read my original
post, you will notice that the SWR didn't change when the coax length
was changed, mainly the incident power.

How would you explain what Cecil wrote? How are some people
improving SWR by changing coax length, when in theory they shouldn't
be able to do this?

Do you think the series reactance a system offers a PA may
actually improve it's incident power?

Slick

W5DXP August 13th 03 04:08 PM

Dr. Slick wrote:
And i don't think you can expect the measured SWR with the meter
and PA to be exactly the same as what you get with a small-signal
analyzer. It's usually a bit different.


The actual conceptual SWR and the difficulty in measuring the SWR are two
different things. Low power level SWRs are difficult to measure because
of the diode voltage drops. Better to use a class-B amp for such where the
zero-crossing points are aligned.
--
73, Cecil http://www.qsl.net/w5dxp



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Ian White, G3SEK August 13th 03 04:18 PM

Dr. Slick wrote:
"Ian White, G3SEK" wrote in message
...

Sorry, that is exactly wrong. S11, SWR and the impedance itself, do
*not* change when you connect a different instrument to the same load.
All the changes you have described are due entirely to instrument
errors.

That's how the instrument errors are determined... by knowing for a fact
that, whatever all the different instruments may say, the impedance
they're trying to measure is the one thing that has *not* changed.



You are right, but i never stated that the impedance we are
feeding ever changes, only the measured SWR.

Oh dear... just when I thought it was safe to go back into the waves...

[On the other points, I'll reply to your second, corrected, posting.]


How would you explain what Cecil wrote?


Who else but Cecil would dare attempt that? :-)

How are some people
improving SWR by changing coax length, when in theory they shouldn't
be able to do this?

There are two possible reasons. One is instrument error - SWR meters are
not perfect.

The other possible reason is that the *outer* surface of the coax has
currents on it, so it has become part of the antenna. In that case,
changing the length of coax is not only changing the length of feedline
(the inner surfaces of the coax), but also is changing the antenna
itself. The voltage and current distributions on all the wires will
shift around, resulting in a different V, I and relative phase at the
top of the coax - in other words, a different feedpoint impedance. Then
the SWR (as measured on the *inside* of the feedline) genuinely will
change.

This SWR change is usually quite difficult to predict, because you
didn't mean there to be any current on the outer surface of the coax in
the first place. The only practical way to see if there could be a
problem is to use a clamp-on RF current meter to see how much surface
current is present.

If the SWR changes with feedline length *and* you have significant
surface current, then you know one probable reason... but in all cases,
these can also be instrument error in the SWR meter.

Do you think the series reactance a system offers a PA may
actually improve it's incident power?


To answer your exact question: I don't think there is a valid general
answer. It depends on the specific PA design, and also on what you mean
by "improve".

What I do know is that changes in the load impedance presented to a PA
will change several of its operating conditions, all at the same time.
Some of those changes will be "improvements" - but others definitely
won't be.

For example, reducing the load impedance will usually make the output
device operate in a more linear way... but the efficiency drops and the
greater heat dissipation and current are likely to shorten the lifetime
of the device. Is that an improvement?


--
73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB)
Editor, 'The VHF/UHF DX Book'
http://www.ifwtech.co.uk/g3sek

W5DXP August 13th 03 04:23 PM

Ian White, G3SEK wrote:
The RF voltages are either summed or subtracted, and then the resultant
is detected by the diode.


I know you know this, Ian, but let's make sure that everyone understands
that the summation (or subtraction) is a phasor (vector) summation. It is
the phasing between the total voltage and total current that allows the
forward wave to be separated from the reflected wave, and vice versa. The
directional coupler designer assumes that the ratio of Vfor/Ifor = Z0
and that the ratio of Vref/Iref = Z0. If that assumption is incorrect,
the SWR meter will still assume that the assumption is correct.

Just one small point, though... it is not necessary that R = Z0.


That's true and is just a habit on my part. I set R=Z0 and then adjust the
voltage accordingly for calibration purposes. For awhile, I was using a
450 ohm load for ladder-line with a measured Z0 of 388 ohms. It still
worked pretty well.

AFAIK, the only situation where the "terminating" resistor truly needs
to equal Z0 is in parallel-line couplers for microwaves, when the
sampling line approaches a quarter-wavelength long and its own
characteristic impedance is Z0 too.


In most of the slotted line pickups that I have seen, the internal load
resistor is equal to the Z0 of the slotted line. I don't know if that
is necessary or not.
--
73, Cecil http://www.qsl.net/w5dxp



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W5DXP August 13th 03 04:30 PM

Dr. Slick wrote:

Roy Lewallen wrote:
Sure, you can normalize a Smith chart to anything you'd like. That
doesn't make the SWR change with source impedance.

I disagree on this point. You are caught up in the 50 Ohm world,
which i admit is easy to do. The SWR is based on the ratio of the
forward to the reflected power. If you had an analyzer that was
calibrated to 20 Ohms (the same as normalizing the Smith for 20 Ohms
in the center) you would certainly have reflected power and high SWR
going into a 50 Ohm load.


Not if the feedline has a Z0 of 50 ohms. The problem would be in believing
what you believe about what the 20 ohm SWR meter is trying to tell you.

It is trying to tell you that it is being misused but you are inferring
that it is trying to tell you the actual SWR. It is not.

And a 20 Ohm load would have a 1:1 SWR.


Not if the feedline has a Z0 of 50 ohms. If a DC voltmeter gives an
erroneous reading for RF voltage, do you blame the voltmeter or the
user of the voltmeter?
--
73, Cecil http://www.qsl.net/w5dxp



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Ian White, G3SEK August 13th 03 04:37 PM

Dr. Slick wrote:
"Ian White, G3SEK" wrote in message
...
Dr. Slick wrote:
As you might know, the input S11 or SWR will change when you go
from an antenna analyzer or network analyzer to measuring with the
actual full power PA and meter hooked up. This may be partly due to
the fact that the meter is usually not a perfect 50 ohm thru, and
partly due to the fact that the analyzers outputs are closer to 50 ohms
than the PA.

Sorry, that is exactly wrong. S11, SWR and the impedance itself, do
*not* change when you connect a different instrument to the same load.
All the changes you have described are due entirely to instrument
errors.

That's how the instrument errors are determined... by knowing for a fact
that, whatever all the different instruments may say, the impedance
they're trying to measure is the one thing that has *not* changed.



On second thought, i believe we are all wrong to equate S11 with
SWR!

Input S11 of a system will certainly never change. But the SWR
is absolutely dependant on the source impedance.


No! SWR, S11, return loss, rho, Y-parameters, Z-parameters, etc, etc are
all different derived functions of the same two variables: an arbitrary
complex impedance, and the system reference impedance Z0 (a constant
which may or may not be defined as complex).

Only those two variables are involved, so all of these functions are
locked together. If one variable changes, all the derived functions
change too. Either all change, or none change; nothing else is logically
possible.

As Roy says, the equations relating any one of these parameters to any
other are all well known. NONE of them ever involves source impedance.


If you had a network
analyzer calibrated for 20 Ohms, you would certainly have reflected
power and high VSWR going into 50 Ohms, and a 1:1 SWR going into 20
Ohms.

This would be the same as re-normalizing the Smith Chart for 20
Ohms in the center. You certainly can do this in MIMP.

I don't blame anyone for believing it's a 50-Ohm-only world!


No argument about any of that... but it's a totally separate point that
has no relevance whatever to your earlier statements about source
impedance.



--
73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB)
Editor, 'The VHF/UHF DX Book'
http://www.ifwtech.co.uk/g3sek

Tom Bruhns August 13th 03 05:55 PM

Non-linear, or time variant. I'd expect some variation going between
low and high power with typical dummy loads, because the resistance
will change with temperature. In fact, the loss in the transmission
line will change with temperature, too, and it's significant enough to
be able to measure with ham-type equipment if you are careful. But
I'd FIRST suspect other things going on: different calibrations
between different instruments, and the fact that SWR meters that use
uncompensated diode detectors will not read the same SWR at low power
as at high: they will fail to read high enough at low powers.

The resistance of the copper in the transmission line changes with
temperature. If ambient is 20C and you put in enough power to heat up
the line (center conductor) to 70C, that's a 50C change, and will
result in about an 18% increase in resistance. So if you had a line
which had 3dB loss at 20C, it would increase to about 3.5dB at 70C.
If the load end has a 2:1 SWR, then the sending end will have about
1.40:1 SWR at 20C and about 1.35:1 at 70C. It's not a _big_ change,
but it should be observable on an SWR meter that is accurate over a
wide range of powers.

I want to make it clear that this is in support of what Roy and Ian
are saying, as an added detail, and not contrary to the notion that
SWR on a line in a linear, time-invariant system with steady-state
excitation does not depend on the source impedance.

Cheers,
Tom


Roy Lewallen wrote in message ...
Dr. Slick wrote:

As you might know, the input S11 or SWR will change when you go
from an antenna analyzer or network analyzer to measuring with the
actual full power PA and meter hooked up. This may be partly due to
the fact that the meter is usually not a perfect 50 ohm thru, and
partly due to the fact that the analyzers outputs are closer to 50
ohms than the PA.


If S11 or the SWR actually does change, you've either got a nonlinear
transmission line or a nonlinear load. That is, the impedance changes as
the signal level changes. If you *measure* a different SWR or S11, it
means that either the SWR or S11 is actually changing for the reasons I
just stated, or the meter is nonlinear in the sense that its reading
changes with power level (possibly due to RF ingress, but it could be a
host of other things), or you're measuring with two different meters
that don't agree.

It's not because of the different source impedances.

Sure, you can normalize a Smith chart to anything you'd like. That
doesn't make the SWR change with source impedance.

. . .


Roy Lewallen, W7EL


Tom Bruhns August 13th 03 06:23 PM

(Dr. Slick) wrote in message . com...

On second thought, i believe we are all wrong to equate S11 with
SWR!


(Of course they are not equal, just related by a formula [which is
usually stated slightly incorrectly])

If your reference impedance for measuring S11 is not the line
characteristic impedance, it's true that SWR = (1+|S11|)/(1-|S11)
won't give you the right answer. But then you haven't really measured
the reflection coefficient on the line, if you've used the wrong
reference impedance, since reflection coefficient is _defined_ as
reverse voltage divided by forward voltage. All this is right at the
heart of why I've been telling you that you should make sure your SWR
meter is calibrated to the impedance you think it is, and in
particular, to the line impedance (or close to that) if you really
want to know the SWR on the line. On the other hand, knowing measured
S11 and the reference impedance for it, and the line characteristic
impedance, you can determine the SWR on that line. But your "SWR"
meter isn't really an S11 meter; at best it's a |S11| meter.

This also brings up another point: do YOU define S11 to be the same
as reflection coefficient?

Cheers,
Tom

Tom Bruhns August 13th 03 06:47 PM

(Dr. Slick) wrote in message om...

The problem is characterizing insertion loss using higher power
transmitters, when we know that the 1000 watt cantenna swings from 40
to 70 Ohms (with reactance too) as you get above 80 megs or so. It
become difficult to know if you are moving in the right direction or
not.


So if you have 200 feet of RG-213 and 200 feet of RG-58, put those in
series to the cantenna. Coil them loosely and cool them with a fan if
needed, if you are running high power (or start the chain with larger
coax). That should get you close to 15dB attenuation in the coax at
100MHz and a 1.02:1 or better SWR at the input end for a 2:1 SWR at
the cantenna. At lower frequencies where the line loss is lower, the
cantenna is good enough that you don't need the line loss as
compensation. Do I have you worried about what the actual impedance
of the coax is from earlier postings? If so, good! Now you're in a
position to think about what's good enough, and measure what you have
to see if it meets the desired goals.

If that's all too kludgey for you, go buy a good load. Or just tune
the cantenna for bands of interest. You could make a set of small
boxes with L networks, each of which compensates the cantenna on a
particular band. Or look up one of the articles about how to make a
better "cantenna", probably starting with the parts you have. There
are lots of options. Why settle for a setup which will only lead you
deeper into confusion? Short of really precision measurements,
there's a lot you can do trading off time and careful thought for the
high cost of commercial equipment.

Cheers,
Tom

Tom Bruhns August 13th 03 06:54 PM

Roy Lewallen wrote in message ...

I stand by my statement.


I, and I'm sure many others, likely including the authors of certain
cited papers, stand beside you.

Cheers,
Tom

Roy Lewallen August 13th 03 08:24 PM

Tom Bruhns wrote:

So if you have 200 feet of RG-213 and 200 feet of RG-58, put those in
series to the cantenna. Coil them loosely and cool them with a fan if
needed, if you are running high power (or start the chain with larger
coax). . .


One thing to keep in mind when you use coax as an attenuator or dummy
load is that the portion of the cable nearest the transmitter dissipates
most of the power. If you had, say, 6 dB per 100 ft attenuation and a
200 ft cable, the first 50 ft dissipate 1/2 the power (and that's
concentrated toward the transmitter end), the next 50 ft dissipate 1/4
the power, the next 50 ft 1/8, and the final 50 ft 1/16. So do as Tom
says and put the heavier coax up front, and allow for more air
circulation for the coax nearest the transmitter if dissipation becomes
a problem.

Roy Lewallen, W7EL


W5DXP August 13th 03 09:50 PM

Ian White, G3SEK wrote:
Dr. Slick wrote:
How would you explain what Cecil wrote?


Who else but Cecil would dare attempt that? :-)


In my example, the SWR on the ladder-line is not changing (except
for losses in the ladder-line). Changing the length of the
ladder-line changes the 50 ohm SWR meter *reading*, i.e. it
changes the impedance seen by the transmitter.
--
73, Cecil http://www.qsl.net/w5dxp



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W5DXP August 13th 03 10:02 PM

Tom Bruhns wrote:
On the other hand, knowing measured
S11 and the reference impedance for it, and the line characteristic
impedance, you can determine the SWR on that line.


That's true for a one-port load but not usually true for a two-port
impedance discontinuity in the transmission line.

This also brings up another point: do YOU define S11 to be the same
as reflection coefficient?


S11 is the (physical) reflection coefficient when a2 equals zero. When
a2 is not zero, the physical reflection coefficient, S11, will not usually
equal the measured reflection coefficient, the square root of Pref/Pfwd.
--
73, Cecil http://www.qsl.net/w5dxp



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JDer8745 August 13th 03 10:50 PM

Roy Lewallen, W7EL sed...

"The transmitter output impedance has no effect whatsoever on the line's SWR."
---------------------------------------------

Of course.

Good grief, is there still someone out there who does not know this???

Jack K9CUN



Reg Edwards August 13th 03 11:28 PM



--
=======================
Regards from Reg, G4FGQ
For Free Radio Design Software
go to http://www.g4fgq.com
=======================
"JDer8745" wrote in message
...
Roy Lewallen, W7EL sed...

"The transmitter output impedance has no effect whatsoever on the line's

SWR."
---------------------------------------------

Good grief, is there still someone out there who does not know this???

-----------------------------------------------

Here comes the $64,000 question . . . . Of what possible use is the SWR
when they think they've got it ???



Roy Lewallen August 14th 03 12:06 AM

Dr. Slick wrote:

I disagree on this point. You are caught up in the 50 Ohm world,
which i admit is easy to do. The SWR is based on the ratio of the
forward to the reflected power.


That's not correct. The SWR (more correctly VSWR) is, by definition, the
ratio of the highest to lowest voltages which appear on a line long
enough to have both a maximum and minimum. It can be calculated from the
forward and reverse voltage waves. ISWR, the current standing wave
ratio, is numerically equal to the VSWR.

If you had an analyzer that was
calibrated to 20 Ohms (the same as normalizing the Smith for 20 Ohms
in the center) you would certainly have reflected power and high SWR
going into a 50 Ohm load.

And a 20 Ohm load would have a 1:1 SWR.

Loads do not have an SWR, only transmission lines do. The fact that you
get a reading on an SWR meter when it's connected to a resistor doesn't
alter that.

You have to realize that an SWR meter isn't really measuring SWR, as Reg
has repeatedly pointed out. It's actually measuring an impedance, and
reporting that on a scale marked SWR. So you have to be careful to avoid
making the mistake of confusing an SWR meter reading with the SWR on a
cable it's connected to. The two correspond only if the cable's Z0
equals the SWR meter's.

Likewise, you have to realize that you don't change the SWR or
"reflected power" when you change the normalization of your network
analyzer or Smith chart. Those things are a function only of the load
and transmission line impedance, not on your measurements or calculations.

Roy Lewallen, W7EL


Roy Lewallen August 14th 03 12:09 AM

Dr. Slick wrote:

On second thought, i believe we are all wrong to equate S11 with
SWR!

Input S11 of a system will certainly never change. But the SWR
is absolutely dependant on the source impedance.


I give up. People will believe what they want to believe, no matter what
-- it's like arguing religion. But I hope some of the lurkers have
learned that SWR is independent of source impedance, even if some of the
active posters just can't seem to.

. . .


Roy Lewallen, W7EL


Dr. Slick August 14th 03 12:55 AM

"Ian White, G3SEK" wrote in message ...

Input S11 of a system will certainly never change. But the SWR
is absolutely dependant on the source impedance.


No! SWR, S11, return loss, rho, Y-parameters, Z-parameters, etc, etc are
all different derived functions of the same two variables: an arbitrary
complex impedance, and the system reference impedance Z0 (a constant
which may or may not be defined as complex).


Correct, but it doesn't have to be 50 Ohms.


Only those two variables are involved, so all of these functions are
locked together. If one variable changes, all the derived functions
change too. Either all change, or none change; nothing else is logically
possible.


How about a 50 Ohm resistor, which is always 50 Ohms (impedance
doesn't change), fed with 20 ohms? Or 75?

Cecil is correct in saying that the SWR meter would then have to
be designed for 20 or 75 ohms, but that is beside the point.

SWR doesn't have to be strictly 50 ohms, and will involve TWO
impedances. If your source doesn't match your reference impedance
(normalized center of Smith Chart), then you won't be measuring the
reflected power coming right off the source.

And because most PA are not 50 ohms output, and most SWR meters
are 50 Ohms, there is problem.


As Roy says, the equations relating any one of these parameters to any
other are all well known. NONE of them ever involves source impedance.




Assuming the source impedance is 50 ohms, which it usually isn't
with most PAs.



If you had a network
analyzer calibrated for 20 Ohms, you would certainly have reflected
power and high VSWR going into 50 Ohms, and a 1:1 SWR going into 20
Ohms.

This would be the same as re-normalizing the Smith Chart for 20
Ohms in the center. You certainly can do this in MIMP.

I don't blame anyone for believing it's a 50-Ohm-only world!


No argument about any of that... but it's a totally separate point that
has no relevance whatever to your earlier statements about source
impedance.



it's very relevant if you consider the port on a network analyzer
to be 50 ohms or not... It should be, but your PA may be quite far
off.


Slick

Richard Clark August 14th 03 01:04 AM

On Wed, 13 Aug 2003 16:13:13 -0700, Roy Lewallen
wrote:

Believe me, Ian, I know how frustrating it can get. But remember all the
lurkers out there who benefit from your insightful postings. Please keep
it up -- it is worth while. For their sake.

Roy Lewallen, W7EL


Hi Roy,

It is nice of you to commend Ian to continue the good effort. Why
didn't you do it directly instead of posting him through me? Are the
lurkers to take some lesson by this breach of netiquette? :-)

73's
Richard Clark, KB7QHC

Dr. Slick August 14th 03 01:12 AM

(Tom Bruhns) wrote in message om...
(Dr. Slick) wrote in message . com...

impedance, you can determine the SWR on that line. But your "SWR"
meter isn't really an S11 meter; at best it's a |S11| meter.


Of course. We have no phase information. Only the magnitude of
the voltage reflection coefficient.


This also brings up another point: do YOU define S11 to be the same
as reflection coefficient?

Cheers,
Tom



I define the S11 as the complex impedance, which never changes,
but S11 can also refer to the magnitude of the reflection coefficient
at a particular phase, AT A PARTICULAR NORMALIZED REFERENCE IMPEDANCE.
If you define the reflection coefficient as having phase
information, then yes, they are the same, but only at a particular
reference impedance.

Change the reference impedance, and you will have a new reflection
coefficient, but the complex impedance will still be measured to be
the same.

You can do this is Motorola's Impedance Matching Program (MIMP).

What this all comes down to is that your 50 Ohm SWR meters only
measure reflected powers after it, not before, so any mismatch from PA
to reference impedance (50 ohm coax from PA to meter) is not measured.


Slick

Tom Bruhns August 14th 03 01:13 AM

(Dr. Slick) wrote in message . com...
The SWR is based on the ratio of the
forward to the reflected power.


Exactly! And (in a linear, time-invariant system at steady-state,
with enough forward power to be interesting,) that ratio does not
depend on where the forward power comes from; it's determined by the
load attached to the line and the line itself. (I trust we ARE
talking about a situation with only one source, feeding only one end
of the line...)

Cheers,
Tom

Dr. Slick August 14th 03 01:19 AM

"Ian White, G3SEK" wrote in message ...

How would you explain what Cecil wrote?


Who else but Cecil would dare attempt that? :-)


I can understand your fear...




Do you think the series reactance a system offers a PA may
actually improve it's incident power?



For example, reducing the load impedance will usually make the output
device operate in a more linear way... but the efficiency drops and the
greater heat dissipation and current are likely to shorten the lifetime
of the device. Is that an improvement?



By improve, i mean increase the incident power. I think this is
possible, and i've actually measured it, if you read my original post.

If you can improve the incident power (tuning) of a PA with
varying the coax length, you might be able to adjust the SWR too, in
certain cases... though in my case, the SWR stayed about the same.


Slick

Roy Lewallen August 14th 03 02:10 AM

I apologize for the discourtesy. It did indeed set a bad example.

Roy Lewallen, W7EL

Richard Clark wrote:
On Wed, 13 Aug 2003 16:13:13 -0700, Roy Lewallen
wrote:


Believe me, Ian, I know how frustrating it can get. But remember all the
lurkers out there who benefit from your insightful postings. Please keep
it up -- it is worth while. For their sake.

Roy Lewallen, W7EL



Hi Roy,

It is nice of you to commend Ian to continue the good effort. Why
didn't you do it directly instead of posting him through me? Are the
lurkers to take some lesson by this breach of netiquette? :-)

73's
Richard Clark, KB7QHC



W5DXP August 14th 03 02:32 AM

Roy Lewallen wrote:

Dr. Slick wrote:
I disagree on this point. You are caught up in the 50 Ohm world,
which i admit is easy to do. The SWR is based on the ratio of the
forward to the reflected power.


That's not correct. The SWR (more correctly VSWR) is, by definition, the
ratio of the highest to lowest voltages which appear on a line long
enough to have both a maximum and minimum. It can be calculated from the
forward and reverse voltage waves. ISWR, the current standing wave
ratio, is numerically equal to the VSWR.


For Dr. Slick: Knowing the forward and reflected powers, one can use the
following equation to obtain SWR. 'Sqrt' means "square root of".

SWR = [Sqrt(Pfwd)+Sqrt(Pref)]/[Sqrt(Pfwd)-Sqrt(Pref)]
--
73, Cecil http://www.qsl.net/w5dxp



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W5DXP August 14th 03 02:54 AM

Dr. Slick wrote:
So we never really measure the reflected
power coming right out of the PA, even if we attach the meter directly
to it's output.


If the forward power out of a PA is 100 watts and the reflected power
into the PA is 50 watts, the PA is generating 50 watts, *by definition*.

Given that definition, the implication is clear. All PA's, by definition,
must re-reflect 100% of the incident reflected energy. Thus, everything
you are worried about has already been defined out of existence. :-)
--
73, Cecil http://www.qsl.net/w5dxp



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W5DXP August 14th 03 02:56 AM

Ralph Mowery wrote:
I have not seen a whole lot of equations on SWR but the few I have seen
never mention the source at all.


When someone defined the generated power as the forward power minus the
reflected power, the entire problem was defined out of existence. :-)
--
73, Cecil http://www.qsl.net/w5dxp



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