With the popularity of the nanoVNA, one of the applications that is coming up regularly in online discussion is the use to measure velocity factor of cable and / or tuning of phasing sections in antenna feeds.
‘Tuning’ electrical lengths of transmission line sections
Online experts offer a range of advice including:
- use the datasheet velocity factor;
- measure velocity factor with your nanoVNA then cut the cable;
- measure the ‘tuned’ length observing input impedance of the section with the nanoVNA; and
- measure the ‘tuned’ length using the nanoVNA TDR facility.
All of these have advantages and pitfalls in some ways, some are better suited to some applications, others may be quite unsuitable.
Let’s make the point that these sections are often not highly critical in length, especially considering that in actual use, the loads are not perfect. One application where they are quite critical is the tuned interconnections in a typical repeater duplexer where the best response depends on quite exact tuning of lengths. Continue reading nanoVNA – measuring cable velocity factor
Deepelec store on Aliexpress sells a small test jig for use with their nanoVNA..
Above is the top view of the test jig mounted on a DIY PVC plinth. The test jig alone cost $17 on Aliexpress and took three months to arrive. Continue reading nanoVNA-H – Deepelec test jig
This article documents a station for propagation observations on 144MHz, in this case the antenna system part of the entire system.
Above, the antenna is a 4 element Yagi with Gamma match. Continue reading 144MHz propagation experiment – antenna
A new version of Antscope2 has been released.
Online posters are excited that it supports some versions of nanoVNA, and one thread attempts to answer the questions:
The SWR image shows that the SWR minimum is at the center phase angle as you would expect. My question is:
what are the other points that look like resonance,
and should I trim my antenna based on phase?
If so which one?
They are interesting questions which hint the ham obsession with resonance as an optimisation tartget.
Properly interpreting VNA or analyser measurements starts with truly understanding the statistic being interpreted.
In this case, the statistics being discussed are Phase and VSWR, and their relationship.
What is the Phase being discussed?
Above is an Antscope2 phase plot for an archived antenna measurement. The measurements are of a 146MHz quarter wave mobile antenna looking into about 4m of RG58C/U cable. We will come back to this. Continue reading Rigexpert Antscope2 – v1.1.1
A recent post by David Knight described dimensional issues with the N connector on his AA-600 and problems with the seller in having it resolved.
Warned of a potential quality issue, I measured my own AA-600.
Above, the test of the inner pin forward surface distance from the reference plane on the N jack on the AA-600. The acceptable range on this gauge for the female connector is the red area, and it is comfortably within the red range.
Above is a table of critical dimensions for ‘ordinary’ (ie not precision) N type connectors from Amphenol.
This dimension is important, as if the centre pin protrudes too much, it may damage the mating connector.
Pleased to say mine is ok, FP at 0.192″.
I used a purpose made gauge to check this, but it can be done with care with a digital caliper (or dial caliper or vernier caliper), that is what I did for decades before acquiring the dial gauge above.
At nanoVNA-H – measure ferrite transformer I gave an example of using a nanovna to measure loss of a ferrite cored transformer.
Noelec makes a small transformer, the Balun One Nine, pictured above and they offer a set of |s11| and |s12| curves in a back to back test. (Note: back to back tests are not a very reliable test.) Continue reading nanoVNA-H – measure ferrite transformer – Noelec balun
Having seen some recent discussion where the online experts opined that an example given of a VSWR plot that contained a fairly consistent ripple was
quite normal, this article suggests there is an obvious possible explanation and that to treat it as quite normal may be to ignore the information presented.
Above is a partial simulation of a scenario using Rigexpert’s Antscope. It starts with an actual measurement of a Diamond X-50N around 146MHz with the actual feed line de-embedded. Then a 100m lossless feed line of VF=0.66 is simulated to produce the plot that contains a ripple apparently superimposed on an expected V shaped VSWR curve.
This is the type of ripple that the expert’s opine is
quite normal. Continue reading VSWR ripple
The popularity of the nanovna with new users has led to a lot of ‘beginners’ seeking advice of the online experts.
A recent question and the responses exposes some common misunderstanding / woolly thinking.
A beginner in search of wisdom asked if
there an easy way to measure balun loss?
One of the responses was…
Measure the return loss of the balun with the balun shorted. The return loss should be about twice the balun loss. This is similar to measuring the loss of a shorted or open piece of cable.
This was expanded by others, basically supporting the concept. Continue reading Transformer loss from half return loss
Articles describing how to make a Return Loss Bridge are pretty common, but they don’t often spell out component values that are critical to accuracy.
Above is a schematic for discussion. It is somewhat simplified, but it is complete and will work. Continue reading Return Loss Bridge – some important details
Let’s explore measurement of a test inductor with the nanovna.
Above is the test inductor, enameled wire on an acrylic tube.
An online expert’s advice make this task look like a no-brainer:
For a 100 nH inductor you are probably using an air wound coil so you won’t see that much change in inductance with frequency. However, inductors made with toroids will because the permeability of the core goes down with frequency.
So, this is an air cored inductor, permeability is approximately that of free space, a constant 4πe-7 independent of frequency. Nevertheless we will see that apparent inductance can change with frequency. Continue reading nanoVNA-H – measuring an inductor – is it a no-brainer?