Measure MLL using the half ReturnLoss method
Again in the theme of measuring something known, let us determine the matched line loss (or normally quoted attenuation) of our cable at 3.5MHz.
To make the measurement, just connect the two line sections in cascade with a joiner, and one end on the instrument, other end open circuit, and measure ReturnLoss.
Most analyser manuals and lots of helpful articles in journals and handbooks will tell you that MLL=RL/(2*length) where RL is the ReturnLoss of an open circuit or short circuit line section (the only requirement is that the ρ=1 at the line end).
Wow, that is so low, and using the traditional formula:
Of course we are measuring way low in the instrument’s capability and there is some considerable uncertainty… but when we consult a good transmission line loss calculator, we expect around 0.029dB/m… that is 12 times what we measured. Continue reading Exploiting your antenna analyser #4
This blog was started two years ago when VK1OD.net was closed due to forced change of call sign.
In that two years, more than 450 blog articles have been published here and there are more ‘in the wings’, around 10 articles ready for release as I write this.
Though I set out to write mostly about electronics and less about Amateur Radio application of technology, that clearly hasn’t happened as the majority of articles are about Amateur Radio related technology.
Interestingly, the most popular articles are about technology, but not about Amateur Radio technology.
Amateur Radio has relegated itself to a backwater in electronics and technology hobbies. Relegated from the proud tradition that saw many of the significant contributions to electronics and communications technology from people who were also radio amateurs, and that had help shape their development. Amateur radio has transformed itself under the active guidance of its peak bodies into a contesting activity, train-spotting if you like and promoted as “radio sport” and the ‘original’ social network, a pursuit where technology is no longer the main shared interest (or much interest at all) and bad behaviour is rewarded. Progress!
Overall, hit rates on the new site are much lower than for VK1OD.net which was quite expected. Factors, positive and negative include:
- + shorter articles intended to be more digestible to modern audiences with busier lives and shorter attention spans;
- + format that presents well on smartphones and tablets for the mobile user; and
- – diminishing interest in the underlying technology in amateur radio.
There a many current projects that will give rise to blog articles, after all, the blog is my experimental notebook. Most current projects have some Amateur Radio element, but they apply wider current technologies to the experiments and are relevant not only to Amateur Radio but to radiocommunications more generally and general applications of technology to discovery.
The sign of reactance
At Exploiting your antenna analyser #2, the matter of determining sign of reactance was mentioned.
If you have an analyser that does not measure the sign of reactance, this information should be important to you.
Above is a Smith chart plot of measurements from 15MHz to 25MHz.
One can see that the locus of Zin on the Smith chart forms an arc, and the points on the arc rotate clockwise about the arc centre with increasing frequency. Continue reading Exploiting your antenna analyser #3
Reconciling the single stub tuner results
So having found that the length of the RG58 lines sections are both 1.98m (approximately 2m), let’s try to reconcile measurement and prediction of Zin at 9MHz.
The examples discussed in this series of articles are designed for the test jig as described at Exploiting your antenna analyser #1 with a pair of nominally 2m length RG58 patch leads, a pair of 50Ω loads and some tee pieces and adapters to connect it all up. If you duplicate it, you will experience the same learning opportunities (the examples are structured). If you presume to redesign the experiment, your outcome will probably be different.
Before you read on, take a measurement of Zin at 20MHz and write down the impedance value. Do whatever you do to determine the sign of the reactance. If your instrument displays the sign properly, use it, otherwise use the method in your user manual or whatever wisdom you trust.
Done that? If so, read on… Continue reading Exploiting your antenna analyser #2
I often see posts in online fora by people struggling to make sense of measurements made with their antenna analyser.
This article is about exploitation of a modern antenna analyser beyond its capability as a self excited VSWR meter. The latter is fine, and it is often not only all you need, but the best tool in optimising some antenna systems… but if you want to exploit the other capabilities of the instrument, read on.
Great benefit can be obtained by measuring some known loads, and reconciling the measurement with the known.
A quite simple set of equipment can be used to create a scenario rich with opportunity to prove your understanding of the basics of complex impedance, transmission lines, and measurement. Lets explore a simple example.
Above is a test jig. It is two equal lengths of identical coax connected to a tee piece on the analyser. The end of one piece of coax has a tee piece with two nominal 50+j0Ω loads as used on Ethernet 10base2 networks. The analyser is a Rigexpert AA-600. Continue reading Exploiting your antenna analyser #1
I have recently installed the Threshold 2 update to Win 10, and apart from a number of small issues, it seriously broke my grabber environment on a 64 bit machine.
The error messages:
5 [main] lftp 2944 C:\bin\lftp\bin\lftp.exe: *** fatal error in forked process - fork: can't reserve memory for parent stack 0x600000 - 0x800000, (child has 0x400000 - 0x600000), Win32 error 487
1481 [main] lftp 2944 cygwin_exception::open_stackdumpfile: Dumping stack trace to lftp.exe.stackdump
6 [main] lftp 5008 fork: child -1 - forked process 2944 died unexpectedly, retry 0, exit code 0x100, errno 11
For that environment, I use an lftp port to Windows (https://nwgat.ninja/lftp-for-windows/), and had installed the 64bit verion which is essentially a cygwin compilation packaged with the necessary DLLs. (This issue probably more widely affects cygwin, or perhaps just the bash shell under cygwin.) Continue reading Win 10 Threshold 2 issues
Voltage Standing Wave Ratio is the ratio of the voltage maximum (antinode) to the adjacent voltage minimum (node) on a transmission line. (This assumes a fully developed standing wave, that the maximum and minimum are not forced by end of line). Continue reading Expression of VSWR as a simple decimal real number
Another of those threads has broken out on eHam illustrating that lots of hams do not understand the complex nature of impedance and cannot see the consequences of the formula to calculate VSWR from load impedance and transmission line characteristic impedance.
Most methods of measuring VSWR are indirect, and they are based on an assumed Zo which is purely real (ie Xo=0Ω), and we speak loosely of that as the VSWR even though the standing wave that might exist on a practical transmission line is a little different as a consequence of that assumption being a little bit in error. Continue reading VSWR=1 and X≠0
I have successfully implemented a few projects on the STC 15F104E, a Chinese 8051 architecture MCU.
The chip includes EEPROM, and some flexible extensions to the timers which potentially make it more useful than a standard 8051.
I have previously observed that the documentation is poor, and the programming tool is poor.
The project that led to the latest observations was an attempt to implement RC PWM – ON/OFF switch originally on one of these chips as it contained sufficient resources to suit the application. One of those resources was an +/- edge triggered INT0.
The code worked fine, but for only a short and variable period. Essentially, the the main loop was executing fine, the chip stopped triggering the interrupt service routing for INT0 after a variable time from 10s to 1000s… but it ALWAYS stopped working. Cycle the power and the same thing is observed. Continue reading Revised thinking on STC chips
This article describes an Aerial Under Test (AUT) that features in some of my experiments and write ups and is subject of some current experiments. It is a MobileOne M40-1 helically loaded vertical for 40m installed in the car roof. It is in the style of the popular US antenna, the Hamstick, but this is a little longer and the results are not directly applicable.
I hasten to add that this configuration is not suited to travelling, it is just a rather ideal mounting of a helically loaded whip without the questions that arise from the effects of roof racks, bumper mounts etc.
The M40-1 is fitted in the centre of the station wagon roof, the roof is 1.5m above ground and the antenna is 1.5m long including a 200mm unloaded tip (tip of the antenna is highlighted with a pink dot). (The setting is not the test site.) Continue reading AUT – MobileOne M40-1 40m helical