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-   -   MFJ-269 Antenna Analyzer experience (https://www.radiobanter.com/antenna/146011-mfj-269-antenna-analyzer-experience.html)

Sal M. Onella August 25th 09 04:51 AM

MFJ-269 Antenna Analyzer experience
 
..
snip

Basically what you do is calibrate the instrument at the measurement
point, whether that point is the instrument connector or at the end of
a length of coax.

You attach an open, a short and a known resistance; 50 ohms by default
but it is user definable.

The instrument than frequency sweeps and stores the results in a user
definable calibration file.

When you make a measurement of an unknown, you define which calibration
file to use and the instrument corrects the readings to display the
characteristics at the measurement point.

Given that this is a $500 insturment and not a $20,000 labratory

instrument
there are going to be limits to how accurate all this is.


When I inspected antennas, we had two multi-kilobuck "Site Master"
instruments from Anritsu, mentioned here, that had a set of calibrated
terminations. IIRC, to calibrate the unit(s), we had to connect the
terminations, a short, a 50-ohm resistor and a shielded open circuit, one at
a time, to the instrument and tell it which one was connected. It swept the
frequencies of interest and stored its own baseline behavior over that band
of interest. Then, anything connected to it was referenced to that
baseline. We could also store a range of sweep frequencies (usually by the
name or type of antenna we intended to sweep) and it would recall all the
parameters. Automated, repeatable sweep testing is not available (yet) in
lower cost instruments.

I presume we could have calibrated any given cable, too. (Never required by
our test memos.)

Sal



Jim Lux August 25th 09 11:03 PM

MFJ-269 Antenna Analyzer experience
 
Sal M. Onella wrote:
.
snip
Basically what you do is calibrate the instrument at the measurement
point, whether that point is the instrument connector or at the end of
a length of coax.

You attach an open, a short and a known resistance; 50 ohms by default
but it is user definable.

The instrument than frequency sweeps and stores the results in a user
definable calibration file.

When you make a measurement of an unknown, you define which calibration
file to use and the instrument corrects the readings to display the
characteristics at the measurement point.

Given that this is a $500 insturment and not a $20,000 labratory

instrument
there are going to be limits to how accurate all this is.


When I inspected antennas, we had two multi-kilobuck "Site Master"
instruments from Anritsu, mentioned here, that had a set of calibrated
terminations. IIRC, to calibrate the unit(s), we had to connect the
terminations, a short, a 50-ohm resistor and a shielded open circuit, one at
a time, to the instrument and tell it which one was connected. It swept the
frequencies of interest and stored its own baseline behavior over that band
of interest. Then, anything connected to it was referenced to that
baseline. We could also store a range of sweep frequencies (usually by the
name or type of antenna we intended to sweep) and it would recall all the
parameters. Automated, repeatable sweep testing is not available (yet) in
lower cost instruments.



The $600 TenTec/TAPR VNA does open/short/thru/load calibration with
sweeps, etc. I don't have the AIM, but I'll bet it does too. These
days, it's not a big deal to include it.



Sal M. Onella August 26th 09 05:45 AM

MFJ-269 Antenna Analyzer experience
 

"Jim Lux" wrote in message
...
Sal M. Onella wrote:
.
snip
Basically what you do is calibrate the instrument at the measurement
point, whether that point is the instrument connector or at the end of
a length of coax.

You attach an open, a short and a known resistance; 50 ohms by default
but it is user definable.

The instrument than frequency sweeps and stores the results in a user
definable calibration file.

When you make a measurement of an unknown, you define which calibration
file to use and the instrument corrects the readings to display the
characteristics at the measurement point.

Given that this is a $500 insturment and not a $20,000 labratory

instrument
there are going to be limits to how accurate all this is.


When I inspected antennas, we had two multi-kilobuck "Site Master"
instruments from Anritsu, mentioned here, that had a set of calibrated
terminations. IIRC, to calibrate the unit(s), we had to connect the
terminations, a short, a 50-ohm resistor and a shielded open circuit,

one at
a time, to the instrument and tell it which one was connected. It swept

the
frequencies of interest and stored its own baseline behavior over that

band
of interest. Then, anything connected to it was referenced to that
baseline. We could also store a range of sweep frequencies (usually by

the
name or type of antenna we intended to sweep) and it would recall all

the
parameters. Automated, repeatable sweep testing is not available (yet)

in
lower cost instruments.



The $600 TenTec/TAPR VNA does open/short/thru/load calibration with
sweeps, etc. I don't have the AIM, but I'll bet it does too. These
days, it's not a big deal to include it.




Thanks for bringing me into the present.

I have an analyzer already. When I drop it off the roof (inevitable), I
will look at the TenTec/TAPR VNA.



Michael Coslo August 26th 09 02:00 PM

MFJ-269 Antenna Analyzer experience
 
Roy Lewallen wrote:


And suppose that these are exactly what our measurement of the cable
said. We measure 21 + j20 at the input end, and conclude that the
impedance of the antenna is 322 - j105 ohms.

But suppose the measurement at the input end was inaccurate by about 5%,
and that the actual input end Z was 22 + j21. Then the load Z is 273 -
j125, about 15% off in R, 20% in X. . .



Thanks Roy,

My knowledge of the matter is at the noobie level, but given that loss
eventually gets you reading only the Z0 of the cable, it's what I
suspected. I hadn't thought about a big mismatch between the cable and
antenna, so there's another data point.


- 73 de Mike N3LI -

J. B. Wood August 28th 09 11:50 AM

MFJ-269 Antenna Analyzer experience
 
In article , Michael Coslo
wrote:

My knowledge of the matter is at the noobie level, but given that loss
eventually gets you reading only the Z0 of the cable, it's what I
suspected. I hadn't thought about a big mismatch between the cable and
antenna, so there's another data point.


- 73 de Mike N3LI -


Hello, and I ran into this issue years ago when trying to measure high (
10 or 20) VSWR loads (in this case out-of-band shipboard HF antenna
feedpoint impedance) connected via a length of transmission line.
Accurate determination of load resistance is difficult to ascertain under
these conditions. A 1953 AIEE (a progenitor of the IEEE) paper by W.W.
Macalpine, "Computation of Impedance and Efficiency of Transmission Lines
with High Sanding Wave Ratio" describes the problem.

I was, however, able to obtain accurate results when I included the small
imaginary part (frequency dependent) of the characteristic impedance that
is present in a low-loss line. Outside the high VSWR load issue the
imaginary part can be ignored. Sincerely, and 73s from N4GGO,

John Wood (Code 5550) e-mail:
Naval Research Laboratory
4555 Overlook Avenue, SW
Washington, DC 20375-5337

Owen Duffy August 28th 09 09:34 PM

MFJ-269 Antenna Analyzer experience
 
(J. B. Wood) wrote in
:

....
Hello, and I ran into this issue years ago when trying to measure high
( 10 or 20) VSWR loads (in this case out-of-band shipboard HF antenna
feedpoint impedance) connected via a length of transmission line.
Accurate determination of load resistance is difficult to ascertain
under these conditions. A 1953 AIEE (a progenitor of the IEEE) paper
by W.W. Macalpine, "Computation of Impedance and Efficiency of
Transmission Lines with High Sanding Wave Ratio" describes the
problem.

I was, however, able to obtain accurate results when I included the
small imaginary part (frequency dependent) of the characteristic
impedance that is present in a low-loss line. Outside the high VSWR
load issue the imaginary part can be ignored. Sincerely, and 73s from
N4GGO,


John,

If I understand correctly, Macalpine's work was in finding solutions given
the computation tools readily available.

The approximation of a real transmission line as having Zo that is real can
introduce significant error in some line calcs.

Improving the model to include an estimated X value based on the loss is a
next step that improves calcs. This technique is widely used, and is
revealed by Ro equal to the nominal Zo, whilst Xo is a small negative
quantity for practical low loss cables at HF. This model produces
significantly different results for high line VSWR at lower frequencies.

TLLC (
http://www.vk1od.net/calc/tl/tllc.php) goes a step further and
estimates a value for Ro based on the loss. For example, the Zo used for
RG58 at 1MHz is 50.06-j2.31 ohms. This model produces significantly
different results for extreme line VSWR at lower frequencies.

The more detailed models would be computationally unwieldly with log tables
or a slide rule (the tools of Macalpine's day), but TLLC demonstrates that
it is a trivial computational matter today, though not to lose sight of the
fact that mathematical function libraries are often approximations
favouring speed over ultimate accuracy.

Again, we must keep in mind that the uncertainty of the data fed into the
model (including manufacturing tolerances, and through life component
degradation) contributes to uncertainty of the output, and as Roy has
mentioned, the sensitivity of results to input data can be higher than
people might otherwise expect.

Properly implemented, the VNA OSL calibration process and measurement
process should overcome the problem of a sufficiently accurate model of the
actual transmission line used in the 'fixture', though not the phase
stability between calibration and measurement, especially where they are
done under very different environmental conditions.

Owen

J. B. Wood August 31st 09 11:30 AM

MFJ-269 Antenna Analyzer experience
 
In article , Owen Duffy
wrote:

John,

If I understand correctly, Macalpine's work was in finding solutions given
the computation tools readily available.

The approximation of a real transmission line as having Zo that is real can
introduce significant error in some line calcs.

Improving the model to include an estimated X value based on the loss is a
next step that improves calcs. This technique is widely used, and is
revealed by Ro equal to the nominal Zo, whilst Xo is a small negative
quantity for practical low loss cables at HF. This model produces
significantly different results for high line VSWR at lower frequencies.

TLLC (http://www.vk1od.net/calc/tl/tllc.php) goes a step further and
estimates a value for Ro based on the loss. For example, the Zo used for
RG58 at 1MHz is 50.06-j2.31 ohms. This model produces significantly
different results for extreme line VSWR at lower frequencies.

The more detailed models would be computationally unwieldly with log tables
or a slide rule (the tools of Macalpine's day), but TLLC demonstrates that
it is a trivial computational matter today, though not to lose sight of the
fact that mathematical function libraries are often approximations
favouring speed over ultimate accuracy.

Again, we must keep in mind that the uncertainty of the data fed into the
model (including manufacturing tolerances, and through life component
degradation) contributes to uncertainty of the output, and as Roy has
mentioned, the sensitivity of results to input data can be higher than
people might otherwise expect.

Properly implemented, the VNA OSL calibration process and measurement
process should overcome the problem of a sufficiently accurate model of the
actual transmission line used in the 'fixture', though not the phase
stability between calibration and measurement, especially where they are
done under very different environmental conditions.

Owen


Good info, Owen and it should be noted that "VNA" is a vector network
analyzer and "OSL" refers to the open, short, and load (usually 50 or 75
ohms) reference standards used to calibrate the VNA over the frequency
range of ineterest.

The small reactive (imaginary) part of the transmission line
characteristic impedance is covered (as are all things to do with RF
transmission lines) in detail in R.W.P. King's seminal work, "Transmission
Line Theory". King also covers transmission line baluns in depth. 73s,

John Wood (Code 5550) e-mail:
Naval Research Laboratory
4555 Overlook Avenue, SW
Washington, DC 20375-5337


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