[PL-259 vs. N on 430 MHz follow-up] – Many OM assert that they can not withstand the performance penalty introduced in the 430 MHz band by a SO-239/PL-259 pair.
Curiously, all the major rig makers seem to ignore this fact. For example the Icom IC2820, the IC7000 and the newer IC7100, the Yaesu FT857/FT897, Alinco DR635, Yaesu FTM-400 and the new Yaesu FT991, among with many others, have a version with SO-239 on the UHF band.
Even the Motorola Radius R100 UHF professional repeater has two SO239 on the back! We are not talking about cheap rigs: many of them are top the range.
In one of my previous posts, PL-259 vs. N on 430 MHz, I tried to verify this issue with a simple measurement. Those tests received some interesting criticism, so I did further testing: if this penalty is true, there must be a way to “see” it.
Let’s play harder
My previous post set off many comments and criticism on various social networks. Some were out of topic: I am not debating about GHz measurement instruments nor QRO EME transmissions. Some argued that the test was not realistic because no power was used; others observed that my connectors were cheap junk and this explained why the N-N connection performed as the PL259-SO239.
So I decided to make further investigations, both with measurement instruments and with my European Yaesu FT857, which is one of the rigs sold in Europe with a N connector and in the rest of the world with a SO-239.
Also, I wanted to remove my N converters from the equation: the tests will have to be done comparing a direct N->N connection with a N->PL259->SO239->N:
This is unfair to the PL, since is being compared to “no connector”. But whatever result it would have given, I expected not to be worse than a rig directly equipped with SO-239.
Some serious measurements
The N connector is undoubtedly an electrically better connector. Its impedance is maintained precise and constant inside the whole RF path, while this is not true for the PL connector.
The S11/S21 plot of my N->PL259->SO239->N converters reports:
At 435 MHz, the PL causes VSWR to jump at 1.18. At the same frequency, it adds an attenuation of 0.17dB. Note that this measure (S21) includes both the attenuation due to impedance mismatch (S11, reflected power) and attenuation due to internal resistance.
We can actually see the impedance inside the PL connector by running a Time Domain Reflectometry with step response:
The green line shows the N connection on its own: impedance is almost perfect (50Ω) everywhere. The black shows when the SO239-PL259 pair is added to the chain: inside this PL the impedance drops to less than 46Ω. The resulting impedance transformation, that causes increased VSWR, is more significant at higher frequencies, because a few millimeters become a relevant fraction of the wavelength. This explains why by adding this PL converter, VSWR at 435MHz goes up to 1.18.
Down to real world
Now we have established that our PL converter adds some millimeters of transmission line with a characteristic impedance of 46Ω. We verified that this causes VSWR to raise to 1.18 and we measured that the transmission loss is 0.17dB.
Ok, but what do these figures mean on real-world operations? Can a human operator detect the effects of that, or are we facing some kind of audiophile syndrome?
In order to answer this question I’ll test my Yaesu FT857, one of the models that is produced both with SO239 and N. Mine has an N connector and, as anticipated, I will test it with direct N-N vs. N->PL259->SO239->N double conversion.
First of all, am I safe to run transmission tests with VSWR at 1.18? The FT857 user manual states:
In my case, VSWR is 1.18 and impedance is |Z|=44.87Ω: I am well inside the “minor excursion” range. I should be safe and expect “no consequence”. After all, a VSWR of 1.18 implies a theoretical reflection of… 0.682%!
Obviously I could not run reception test by tuning to a local UHF FM repeater and reading the S-Meter that bangs over 9+60 even without an antenna plugged in. Also, I did not want to tune to a weak distant station, because natural QSB would have invalidated any reading.
Instead, I put my signal generator on the roof to serve as a steady, low power, nearby CW beacon. I wanted the test signal to be weak but not affected by propagation. The signal was then received by a vertical Comet GP-6 dual band antenna on the same roof about 20m away.
To have readings more accurate than my ears and the internal S-Meter, I extracted the signal from the FT-857D IF and I fed it to an SDR receiver.
Test 1 – 10+ meters of RG58
As a preliminary test, just to see whether the “test bench” was working, I tested reception with and without the insertion of extra 10m of cheap RG-58.
As expected, the signal dropped significantly. With such a weak signal, the note from the radio loudspeaker become very noisy. A weaker signal would have disappeared in the noise floor. The difference was immediately perceivable both by watching the SDR waterfall and by listening to the radio itself.
Test 2 – Beacon, N-N vs N-PL-SO-N
In this test I added and removed the N->PL259/SO239->N converters pair.
Even with this setup, the fluctuation of the received signal was too wide (over 1dB) to appreciate any difference: the values appeared to float within the same range.
Test 3 – Signal generator, N-N vs N-PL-SO-N
In the attempt of reducing the floating, I connected the signal generator directly to the radio. Again, I tested with and without the the PL converters.
This time the dBm fluctuation was much lower, mostly within few tenth of a dB. However, neither in this case the penalty of having an extra PL259/SO239 conversion could be detected.
Some of the criticisms about my previous test were that it was conducted at very low power (0dBm, 1mW).
The FT857/897 can deliver 20W on the UHF band, while other rigs of those available with SO-239, can deliver up to 50W. I set my FT857 to maximum power, connected it to a Weinschel 3GHz attenuator and then into my spectrum analyzer.
When transmitting with the PL converters, the FT857 showed an increased VSWR by lighting one dot in the SWR meter:
However, the readings on the spectrum analyzer were identical:
My spectrum analyzer, despite of the two decimal digits on the display, has an actual resolution of 0.3dB. Therefore, the two reported values might be different, but no more than 0.3dB, which is coherent with the 0.17dB measured by the network analyzer. Taking in account the attenuation of cables and attenuator, this measurement reported that my FT857 was actually delivering over 25W.
My goal was to understand whether a UHF radio delivered with a SO-239 instead of a N plug carries a price in terms of performances. In my investigation, I have not been able to find a single test involving the real rig, even if connected to measurement instruments, that could show any difference: only a Vector Network Analyzer, with an accurate setup and calibration, has been able to characterize the SO239/PL259 connection.
Furthermore, I have tested a plain “N-N” connection versus a “N->SO239->PL259->N” pair: a PL-equipped rig would use a somewhat better “SO239->PL259” direct connection.
Under the light of these facts I have to conclude that, in the 70cm band there is no relevant performance difference if a N, SO239 or even a PL/N converter is used in this kind of rigs.