Friday, May 2, 2025

Refurbishing a CIR Astro 200 HF amateur band transceiver

The Astro 200

The CIR Industries Astro 200 is a compact, synthesized 100 watt HF transceiver from the mid-late 1970s that covers the 80, 40, 20, 15 and 10 meter bands.  Intended for both home and mobile use, it is quite small - 9.75" wide, 12.5" deep and 3" tall (24.8 x 31.8 x 7.6cm) - including the rear heat sink.  Back in 1977 - when this unit was made - it seems to have cost around $995 for the version without the CW filter - about $5000 in 2025 dollars!

Figure 1:
The front panel of the CIR Astro 200.  While advanced for
its day, the radio is pretty simple by today's standard.
The lack of a tuning knob seems a bit odd.
Click on the image for a larger version.

I don't know too much about CIR Industries, except that it was around only for a few years, apparently absorbed by Cubic-Swan in about 1978 where it was rebadged with the name of the new company and - with very minor changes - became the "200A".  The history of Cubic-Swan becomes a bit muddy after the early 1980s and appears to have fizzled entirely by the mid-late 1990s.  Much of the design of the Astro 200 - and other Cubic-Swan radios - was apparently done by Don Stoner, W6TNS (who was also the "S" in SGC).

The later version of this radio, the Astro 200A, sported a 6 pin round microphone connector, black knobs, slightly different switches, a lighted meter and very slightly modified scales on the meter itself:  I suspect that the electrical differences - some of which are noted below - may have evolved during the production of the original Astro 200.

The radio's history

This unit was purchased new in 1977, with the extra-cost CW filter option, and owned by a friend of mine, having first resided in his International Scout II - and then his Jeep CJ-7 - until about 2020 (when it was removed during vehicle maintenance) seeing many hours and miles bouncing around rough, 4WD roads.  Despite having banged around for about 40 years in a vehicle, it's in remarkably good physical shape, the case having only a few minor scratches.  Unfortunately, my friend became a silent key in 2022 and the radio ended up in my hands.

A "unique" radio

The advertisements for this radio tout it as being the very first completely synthesized amateur transceiver:  Whether or not it's actually the "first", I can't be sure, and this can vary depending on what you mean by "synthesized" - but in this case the local local oscillators are referenced from a single crystal while the BFOs were independent - a common practice even into the early 2000s.  Being an early synthesized radio, it does have a few interesting quirks:

  • There's no tuning knob.  Tuning is accomplished by a pair of "up/down" momentary toggle switches.  At first, this seems awkward, but one can quickly become adept to tuning a radio this way.  My friend (the one who'd owned this radio) noted that this tuning method was more convenient when bouncing about on a bumpy Jeep road than trying to use a conventional knob.
    • Operating the "fast" switch moves the frequency up/down by about 20 kHz/second after a brief pause.
    • Operating the "slow" switch moves the frequency up/down about 400 Hz/second after a brief pause.
    • A brief up or down push-and-release of either switch moves the frequency by 100 Hz.
  • 100 Hz tuning steps + Fine Tuning.  The radio tunes in 100 Hz steps, but it has a "Fine" tuning knob that moves the frequency up/down by a bit more than +/-65 Hz to allow one to get the frequency as close as you wish.  With the tendency for most amateurs these days to set their radios to an integer number of kHz (and occasionally to "0.5", 100 Hz steps are just fine and this control can be left centered most of the time.
  • The synthesizers are a bit slow to lock.  As one tunes the radio - particularly in the "fast" mode - the synthesizers may take a second or so to catch up as it "swoops" in onto the correct frequency.  This also means that after power-up, the radio is unusable for about 30 seconds, or for up to 15 seconds after changing bands.  As the synthesizers "land" within about a second during normal tuning with the up/down switches, the radio is on frequency by the time normal human reaction time has "locked in" to what is on frequency.
  • The "WWV" mode.  You'll note that the mode switch includes a "WWV" position.  This is actually a completely separate, direct-conversion receiver - with no AGC - that is tuned only to 10 MHz. Since it uses the (doubled) 5 MHz reference as its local oscillator, it provides an easy way to check/set the radio precisely on-frequency.

Despite having a digital readout and a synthesizer, it does not have a computer of any sort.  "Programming" is done using PROMs (Programmable Read-Only Memory)  to look up the synthesizer tuning information and "74LS" type logic as counters for the frequency dividers and tuning - but this also means that when it's first powered up it always defaults to the bottom edge of the band to which it is tuned.  This is a bit of an inconvenience - but in the mid 1970's, prior to inexpensive single-chip microcontrollers with onboard program memory along with affordable development tools there was no real way around this without adding significantly to complexity and cost.  I'm looking into a simple way for the radio to "remember" the last-tuned frequency on each band - perhaps the topic of a later article.

About this radio

Figure 2:
The radio's tag - Serial #8, apparently!
Click on the image for a larger version.
This radio is apparently a very early production unit - somewhat different from that depicted in the manual:

  • The Microphone connector is a standard 1/4" TRS (headphone) jack rather than a 6-pin round connector apparently used later in the production run and in a later revision, the 200A.  The additional pins on the 6 pin connector provide up/down tuning and 11 volts, allowing one to do tuning via the microphone.
  • It was lacking the "ANL Board".  This is a very simple circuit circuit (two pairs of back-to-back diodes and an electrolytic capacitor) that reduces, according to the manual, "excessive popping or AGC pumping".  As this circuit is very simple, it was trivial to add to this radio and this somewhat reduced the tendency for the receiver to be momentarily deafened when changing modes or bands.
  • Upon inspection of the PA (Power Amplifier) module I noted that the driver transistors were Motorola, marked with "604/438 Sample" which further implies an early production radio.  The PA transistors themselves - which are shown as being of type MRF454 in the service manual - were CD3435 made by CTC. 
  • There are a number of doubly-balanced diode-ring mixers used throughout.  Based on the manual and photos of other units, these seem to be implemented with some sort of module.  On this unit these modules are not used as the corresponding areas on the PC boards are populated with a pair of trifilar transformers and individual diodes comprising the mixer.
  • The serial number of this radio is "706008".  Based on other photos that I've seen online, this is apparently serial number 8 - likely having been made in June of 1977.  The date codes on internal components are consistent with the possible June 1977 assembly date.

Figure 3:
The inner synthesizer board - a bunch of counters.  LS-TTL
circuitry is used extensively, along with a few diode-type
PROMs for frequency/display lookup and counter set-up.
Click on the image for a larger version.
Evaluation

As I had other projects in the queue, it was only recently that I pulled this radio off the shelf.   Prior to setting it on my workbench, I blew the dust off it and carefully cleaned the front panel and around controls, throwing the knobs into an ultrasonic cleaner.

Powering it up, the unit worked - sort of:  I could hear noise, but it seemed a bit deaf - but the sensitivity changed wildly with a bit of thumping on the case, an indication of a dirty transmit/receive relay.  Even with a massively strong signal into the antenna connector - which produced a deafeningly-loud tone in the (external) speaker - I got no S-meter reading.  Many years ago, my friend and I used this radio (when it was still in his Jeep) and noticed this same problem and that it was also mitigated by a "percussive repair" and/or clicking the PTT several times, indicating that the Transmit/Receive relay may have problems.

Figure 4:
The main RF/AF board, post repair.  The layout is a bit
crowded, but pretty clean on a two-sided, glass-epoxy board.
This radio includes the optional 400 Hz CW filter.
Click on the image for a larger version.
Popping the top cover I could see that I had some work to do.  While it was remarkably clean inside for having been in a dusty Jeep for decades, I could see evidence of a few problems:  I saw at least one "blowed-up" capacitor near the audio amplifier.

Fortunately, the synthesizer itself seemed to be OK:  The tuning controls did their jobs properly, the tone in the speaker indicating that the radio was landing on the same frequency as the display.  The only "digital" problem seems to be that one of the segments of each digit on the display was constantly illuminated, weakly, possibly indicative of a problem with a segment driver.

Refurbishing

The first order of business was to replace the electrolytic capacitors.  As a few of them had clearly failed as evidenced by inspection, they all had to go - particularly since the radio had spent many summers in a closed vehicle during hot, Utah summers - plus, this radio is nearly a half-century old (which seems amazing when you consider that it's "digitally synthesized") so time would saved to simply "shotgun" them all.  Furthermore, many of the boards are "tethered" with soldered cables:  There is just enough slack to pull them out and work on the boards unsoldering only a wire or two, but doing so many, many times would not only be tedious, but risk fatiguing and breaking them - another reason to replace the capacitors in just one session.

Figure 5:
VCO/Synthesizer board.  There are two synthesizers - one
for them provides the 100Hz tuning steps.  Again, LS-TTL
logic is used, along with a few op-amps.
Click on the image for a larger version.
Capacitors, and more capacitors!

I took inventory, inspecting the entire radio and come up with the following list of capacitors - including those found in the PA module and places other than on the PC boards:

  • (5) 470uf, 10 volt
  • (2) 330uF, 16 volt (axial) 
  • (2) 220uF, 16 volt
  • (14) 100uF, 16 volt
  • (13) 33uF, 16 volt
  • (2) 10uF, 25 volt
  • (4) 10uF, 16 volt
  • (8) 4.7uF, 25 volt
  • 1) 4.7uF, 16 volt
  • (9) 1uF, 25 volt
  • (4) 1uF, 50 volt
  • (3) 1uF, 50 volt (axial)
  • There are several dipped tantalum capacitors in low-level voltage and signal filtering lines that seem to be OK for now.   As none of these are on power rails there's no chance of a catastrophic failure (e.g. flames) should one short out.  These capacitors will be replaced in the future.

I suspect that the differing voltage ratings of some of the same-value capacitors was likely to save space (lower-voltage capacitors are generally smaller) and allow the use of less-expensive capacitors, but these days, capacitors are much smaller (and cheaper, in equivalent money) than their decades-old counterparts.  When ordering replacement capacitors I simply got same value rated for at least the voltage of the highest in the list above, but the new capacitors also had a temperature rating of 105C rather than the 85C of the original - and since modern capacitors are smaller than those from about 50 years ago, even a higher-voltage new capacitor was smaller than the lower voltage devices of the same value.  Since the electrolytic capacitors were pretty inexpensive - typically less than US$0.10/each for the smaller values - I ordered more than just the number above (in some cases, many more) in the event that I missed something.

Figure 6:
The pile of electrolytics removed from the radio.
Replacing every capacitor was the right choice!
Click on the image for a larger version.

Removing capacitors en masse is best done with the appropriate tools - particularly on an older circuit board.  Fortunately, I have a Hakko FR-300 desoldering iron/pump which made removal much easier and I was able to avoid damaging any traces on the board.

When replacing a bunch of capacitors, I prefer to do so methodically, moving from section to section on the circuit board - noting the polarity orientation of the capacitor before removing it and if there was any doubt as to which way it went, referring to the board layout diagram in the service manual - particularly since the circuit boards have neither solder mask or silkscreen as a visual reference.  Once a capacitor is replaced, I typically mark the top of the can with a colored permanent marker to help make sure that I don't miss any.

One possible "gotcha" was that unlike modern electrolytic capacitors which are typically marked only on the negative lead, many (but not all) of the original capacitors in this radio had only their positive side marked - which was the custom of some manufacturers of the day - so I had to be particularly careful to identify the polarity correctly as I replaced each capacitor.

When I was done, the receiver seemed to be more "alive" than before, but it was still a bit deaf - and the synthesizer seemed to be a bit "wobbly", being very sensitive to slight changes in power supply voltage.  The biggest change was the WWV receiver which was profoundly deaf prior to the capacitor change-out, but "normal" afterwards.

Capacitor brand implies longevity

After replacing the capacitors I went through the pile and found that most of them were "OK" - or at good enough that their respective circuits would have worked.  The brand seemed to be a pretty good indicator of which was likely bad:  The Japanese blue-label Nichicon and gray "Sun" and "Elna" brands were generally OK, the silver and gray Taiwanese "T.I." brand were all over the map, the "Sam Hwa" and "Towa" capacitors were marginal, but  all of the "Temple" branded capacitors (which seemed to have 1970 date codes - apparently already a few years old when the radio was made) were extremely bad.

After doing this I still believe that replacing all of the electrolytics was, in fact, the correct choice as I would have probably spent more time finding and diagnosing capacitors individually - and possibly suffered near-term failures - than simply swapping them all out.

A wobbly power supply

With all of the electrolytic capacitors replaced, I systematically went through the adjustment steps found in the user and service manual (which can be found online) - more or less.  Knowing that before you make ANY adjustments that you must make sure that the power supply is correct, I probed about with a volt meter noticing that the 11 volt supply was actually just below eight volts, likely accounting for its seeming deafness.  Locating the 11 volt regulator on the synthesizer board, I noted that the act of slightly adjusting the potentiometer resulted the voltage jumping, indicating that it was somewhat "stratchy", with the wiper likely not making good contact.  A bit of cleaning spray and exercising of this control resolved the issue and I reset the voltage to precisely 11.0 volts.

Figure 7:
Original S-meter coil.  It would seem that the coil winding
was broken in several places - hence, unsalvagable.
Click on the image for a larger version.
With the correct voltages now applied to the circuits in the radio, its sensitivity seemed to be much better and the synthesizer was no longer sensitive to fluctuations in the power supply, being able to tolerate a drop to about 11.25 volts at the radio's DC input before the synthesizer "wobbled".  

No S-meter!

Going through the alignment steps I applied a signal from my generator and noted that while the sensitivity seemed to be about right - and the AGC was now working as it should - the S-meter did not move.  It's worth noting that the S-meter on this radio works ONLY when the meter switch is set to the "ALC" position - but I was getting no reading on any setting.  Using a voltmeter, I could see that the voltage across the S-meter's movement was increasing with the signal strength indicating that the AGC was working (which was also obvious by listening to off-air signals) but a quick check with an ohmmeter - after disconnecting one of the meter's leads - indicated that it was open circuit.

This was bad news, particularly since it was likely that I would never find a meter of the same, exact physical size - and even if I did find a replacement, I'd probably have to re-create the scale in the meter.  This wasn't impossible to do, but I took another path.

Figure 8:
The meter with its rewound meter coil using #30 wire.
As many turns were wound as would fit - the coil shaped to
prevent mechanical interference and then covered with
varnish to hold it in place.
Click on the image for a larger version.

Carefully disassembling the meter and inspecting it I noted that it was of the inexpensive "moving vane" type, the coil wound with very fine wire - probably around 46 AWGIn probing very carefully I noted that one of these hair-thin wires was disconnected at the base of the coil.  Further probing showed that the wire itself was frayed where it was wound onto the phenolic paper stator - probably a victim of both temperature cycling and (possibly) some corrosion.  A bit of later inspection of the wire showed that it seemed "brittle" - something that I've seen on older gear:  I don't know if it's the copper hardening in some way or some sort of reaction between the wire, enamel and its environment that causes this.

Since the meter's coil was a total loss I decided to do something a bit drastic:  Rewind it.  Rather than trying to use #46 wire, I chose, instead, to use less-fragile wire - #30, which is about 10 times larger diameter:  I'd have used a smaller - but not overly fragile - wire (likely #36) if I'd had it on hand to get more turns and better sensitivity.  Of course, I was not going to get nearly as many turns on the stator as the original - which meant that it wasn't going to be as sensitive as it had been originally and would be unlikely to work properly in the circuit - but I had a plan for this.

Carefully winding the #30 wire into the phenolic stator until it was "full", I scrunched the coil down to reduce its height and then pushed it sideways to clear both the meter's axle and the moving magnets on the rotor before covering all of the windings with urethane varnish.  With the varnish dry, I reassembled the meter and using a variable bench supply with a series resistor to vary the current through it I found that it operated nonlinearly, particularly near the upper and lower ends of meter travel.

I quickly realized that the screwdriver that I'd used was slightly magnetic - and the two screws used to hold down the phenolic stator had become magnetized as well from using that screwdriver.  Using a TV picture tube degaussing coil (I could have used a soldering gun's magnetic field instead) I demagnetized the two screws and the screwdriver, solving this nonlinearity problem.

Re-zeroing the meter and using a series 470 ohm resistor and a variable bench power supply I found that the meter's full-scale sensitivity was about 23 milliamps - very much higher than the 500-ish microamp sensitivity that I'd calculated it to be originally.  In looking at the circuitry I noted that the negative side of the meter was grounded in all three of the front panel meter switch settings which meant that all I needed was to come up with a circuit to multiply the current linearly - and with one end of the meter being connected to circuit ground, that task was greatly simplified:  Here's the circuit to do this:

Figure 9:
Schematic of the circuit used to drive the re-wound meter on the CIR Astro 200.

The circuit shown in Figure 9 is the classic "precision current source" using an op  amp to drive a transistor and then the meter.  The input voltage is scaled with the trimmer potentiometer (R3) and applied to the non-inverting (+) input of the op amp with R4 in parallel to set an input resistance of about 250 ohms - which is my guess of the resistance of the original meter movement.  By its nature, the op amp will attempt to adjust its output to make the voltage on the inverting (-) input the same as the non-inverting (+) input and to do this, it turns on the transistor, causing current to flow through the meter and the current sense resistor, R2.  Resistor R1 is there to limit the maximum current to a "sane" value to prevent the meter from being slammed too hard in the case of an "oops".

Figure 10:
The as-built circuit from Figure 9 constructed on some
prototyping board.  This circuit is adhered to the top of the
meter itself.
Click on the image for a larger version.

The result of this is that this circuit will happily convert the voltage through R2 into a proportional current, the magnitude set by the adjustment of R3, allowing our now-rebuilt meter movement of arbitrary sensitivity to be used.

As the schematic shows, this circuit was built using the venerable LM324.  This device was chosen mainly because I have plenty of them, and it's one of the most common op amps that has an input and output voltage range that includes "ground" (V-):  Many "standard" op amps don't work near one or the other power supply rail and will work incorrectly if the input voltage is the same as the "V-" lead (ground, in our case) and about as many cannot output voltage down to the negative rail, either.

Since I needed only one of the four LM324's op amps, the other three were simply strapped to the power supply to keep them from floating and possibly causing noise issues:  It's possible that I could have used one or more of the op amp sections to directly drive the meter, but the single transistor was cheap and easy.  The circuit was built onto a small piece of glass-epoxy perfboard and attached to the top of the meter movement - the power supply from this circuit stolen from a trace containing the +11 volt supply found on the front-panel circuit board - but even the 13 volt, unregulated supply would have been fine.

Setting up the "new" meter

While the actual sensitivity of the original meter - which is believed to be around 500 microamps - is not known for certain, there is one step in the manual that is revealing in that it has no actual circuit adjustment, relying on the sensitivity of the meter itself and fixed components for accuracy and calibration.  Because of this, we must do this step first and calibrate the sensitivity of our new meter circuit.

In the section of the manual about "Power Meter, Reflected Power Meter Adjustment" it describes connecting a 2:1 VSWR load (25 ohms using two 50 ohm dummy loads in parallel) and using an external power meter connected between the radio and the load:  The radio should be set for 40 meters for this step.  Switching to "CWW" (CW Wide - using the SSB filter) mode, set the Mic Gain to maximum (fully clockwise), key the radio and then increase the power (turning the Mic gain counter-clockwise to increase power) and adjusting R312 to limit the maximum power to 90 watts even when the Mic gain control is fully counter-clockwise (maximum power): These adjustments should be done quickly to avoid overheating the power amplifier.  The manual notes that with the meter set to the "REF" position, the meter should read "2" (for 2:1 VSWR) - and we quickly adjust R3 in Figure 9 for a reading of "2" on the meter.  Again, the key point here is that the REF meter gets its output from the reverse power detector amplifier - but since its threshold is fixed, when the power is being reduced by this circuit, it will always output the correct voltage/current to make the meter read "2".  In other words, this is fixed reference and we can use it to calibrate the meter for all other modes.

After this, the procedures for adjusting the S-meter, ALC and forward power readings outlined in the manual should be applied without further adjustment of R3, the 10 turn trimmer potentiometer on our meter-driver circuit from Figure 9.

It's worth reiterating the point that as the AGC, ALC, FWD and REF signals feeding the meter are ground-referenced, the circuit design was simple.  If the meter was driven by a "floating" circuit - one in which the negative side of the meter was at some potential other than ground - I would likely have used several sections of the LM324 configured as an "instrumentation amplifier" - one that measured the voltage drop across a fixed resistor (in lieu of current through the original meter coil) regardless of the actual voltages.  This circuit would have been somewhat more complex, but not overly so.

Radio alignment

With the capacitors replaced and the meter working, I went through the alignment steps outlined in the manual.  Fortunately, I had reviewed the manual in its entirety and noted a few "inconsistencies", notably:

  • The listing of the carrier oscillator frequencies in the alignment steps shows the same frequency for LSB and USB.  The correct frequencies are shown on the previous page.
  • When adjusting the ALC using potentiometer R296, the manual says to do so at mid-rotation in one place and and fully CW (clockwise) in another:  I presume that they meant fully CW.

Additionally, I would suggest the following additions to the procedure at the beginning of the procedure.

  • Verify/adjust the setting of the 11.0 volt regulator on the synthesizer board (R92).
  • Verify/adjust the 5.0 MHz oscillator on the synthesizer board using C52.
  • If you had to re-wind the meter and add the circuit described above, I would do the reverse power meter calibration (described above) before the other meter calibration steps:  This is noted in the procedure at the end of this article.

After this, proceed with the alignment/calibration as described in the manual.  There is a revised/annotated alignment procedure at the end of this article.

Power cable

As I was unable to find the original power cable (it may still be in the Jeep) I needed to find the mating power connector.  Recognizing it as a "Jones" connector, I did a bit of research and found that I needed to get a Cinch-Jones S-306-CCT, which is a 6 pin female connector.  Unfortunately, this line of connectors was discontinued by the manufacturer several years ago, but EvilBay came to the rescue and I found a "new" one with the inline cable shroud and strain relief.

Using 12 AWG wire and an inline holder with a 30 amp blade fuse I put together a power cable with an Anderson power pole connector on the far end.  This allowed me to connect it to a high-current power supply so that I could get on with testing the radio's final power amplifier.

"Final" problems

With the radio otherwise aligned, I noted that I was unable to get anywhere near full power out of the power amplifier - about 35 watts on 80 meters, nearly 50 watts on 40 meters and 10-15 watts on 10 meters.  Checking the output on the main RF/AF board, I noted that the voltages were equal to or higher than noted in the manual so I removed the PA module from the back via its ten screws.

I immediately noticed something that further indicated that this was an "early" unit:  The PA driver transistors were Motorola, but marked as "604/438 Sample" and rather than using MRF454 outputs, they were CTC CD3435.  In poking around with an oscilloscope with about 10 watts of output on 40 meters I noticed that the waveforms on the collectors of the driver transistors were not equal - and neither were the corresponding waveforms on the output transistors:  This indicated that in each stage, at least one of the transistors had failed - or was badly degraded.

While annoying (the transistors aren't cheap!) it didn't surprise me.  It is (apparently) common for RF transistors from the 70s and, perhaps, into the early 80s to fail - even when not being used - due to internal defects that seem to "grow" over time.

Figure 11:
The repaired PA board with the new driver and output
transistors.
Click on the image for a larger version.
For the driver transistors, the originals were 2N6367, but the equivalent is the MRF433 or the 2SC2395 - but the MRF455 may work OK.  Rummaging around my bin of RF transistors I found a pair of pulled 2SC2395s (I don't recall where I got them) and put them in, saving me from spending about $100 for them.  Greeted with only about 80 watts on 40 meters - and much lower power than that on 10 meters - I could still see from the waveform on the 'scope - probing the collector leads - that one of the output transistors was still an issue.

While I could get a pair of MRF454 transistors from RF Parts, I noted that they were available from Mouser Electronics for a lower price (about $55 each at the time of writing) and when they arrived, I saw that they sported a recent date code.  Plopping them in I saw that the PA was now capable of well over 125 watts on 80 and 40 meters - working as it should - allowing me to complete the adjustment procedures related to the ALC and power metering.

In testing the two original PA transistors out of circuit I noted that both their beta and "diode drop" voltage were radically different.  I suspect that at least one of these devices had lost some "emitter sites" or tiny bond wires on the die, making it "less of a transistor" than it once had been.

With the final board now repaired, the radio met the specifications outlined in the manual:  100+ watts on all bands except 10 meters where the output was a bit over 85 watts.

A few loose ends...

The "stuck" LED segment

I also noted that the "stuck" segment on the LED display seemed to have fixed itself during a toggle of the "bright/dim" switch:  In looking at a YouTube video reviewing this radio I noted that it, too, had this exact problem with the same segment being stuck - but I have no idea if it's common (e.g. happened on at least two different radios) or why it fixed itself - nor is there an obvious clue from the schematic diagram why that one particular segment would be affected on my radio and the one in the video.

Adding the clipper/limiter

As for the receiver, the sensitivity is good - but I decided to make a modification that apparently became standard in production just after this unit was produced.  I noted that when changing modes and bands, the S-meter would "pin" with the very loud "pop" that occurred, the AGC taking 5-10 seconds to recover

Figure 12:
The clipper circuit in tubing, installed in the radio.  One end
is connected to a leg of R290 - the other end to ground.
Click on the image for a larger version.
Noting that the manual included the description of a "Limiter" board - and that the radio in the YouTube channel - which had a serial number of about a dozen units higher - also had this board, I figured that this might be one of the reasons why it was added.

The circuit itself is simple:  Two pairs of diodes - one silicon and one germanium in series (for a clipping voltage of about 0.9 volts) - were placed in anti-parallel configuration and AC-coupled with a 10uF capacitor.  This circuit was placed between ground and input of the AGC detector.  Rather than make a small circuit board as was done in the production units I simply wired the components in free space and covered them with PTFE and heat-shrink tubing, connecting the assembly between the AGC circuit and a handy ground pin as can be seen in Figure 12.

My suspicion about its later addition was confirmed:  While there is still a loud "click" when changing modes, the AGC now recovers much more quickly and the radio's AGC is also very much less prone to being badly deflected with a long recovery time when there is a loud static crash.

The T/R relay and filter module

Mentioned briefly, there was the problem with the intermittent T/R relay.  This is contained within a module that sits along the right edge, inside the radio that extends from the front panel to the back of the radio along with the band switch.

This module - in addition to the T/R relay - contains the receiver pre-selector filters, the transmit mixer filters and the transmit low-pass filters on a compact, shielded assembly.  To pull this assembly out of the radio would be quite a job, requiring the partial removal of the front panel, disconnecting (mostly unsoldering!) a number of wires, connectors and signal cables and pulling it out of the radio - something that I have not attempted to do.

Fortunately, the designers provided an access hole near the back panel of the radio (on the bottom side) that is covered with tape where one can burnish the relay's contacts and apply contact cleaner.  After both burnishing and the application of cleaner, the T/R relay is now working perfectly.

Using the radio

Tuning with switches

With the use of toggle switches instead of a round, "spinny" tuning knob, operating the Astro 200 is decidedly different than using a conventional radio.  As mentioned before, the previous owner told me that he thought using toggle switches was a bit better for tuning while bouncing along bumpy roads than a large knob - and in the days of analog radios, this was likely the case.

In perusing online references to this same radio, the users also noted that one quickly becomes accustomed to this method of tuning - but everyone had the same comment:  It's slow to tune across the band.  When powered up, this radio always starts at the bottom of the selected amateur band - and on 10 meters, this particular radio starts at 27.0000 MHz (transmit is inhibited below 28 MHz) which means that it takes about a minute to even get into the 10 meter band!

The AGC

The radio's AGC is not adjustable and the time constant is fine for CW, but a bit fast for SSB in my opinion.  As is common with many analog radios, the apparent AGC time constant gets shorter with more AGC action (e.g. higher S-meter reading).  This is a result of the "dB per Volts" curve getting steeper with many gain reduction schemes (e.g. more dB gain reduction per volt of change) effectively shortening the time constants.

Since this radio has a front panel RF attenuator control, switching this in to reduce the signal level helps with this effect somewhat.

Noise blanker

The noise blanker (enabled by pulling the "Squelch" control knob out) seems to work pretty well, operating in the wideband IF prior to the crystal filters.  As is typical with noise blankers in analog receivers - and some modern digital radios - its efficacy is somewhat affected by very strong, adjacent signals which "desense" the noise detector - a difficult problem to overcome.

CW usage

As is common for radios of that era, the sidetone frequency in the CW mode has little to do with the frequency offset.  This radio uses USB and a positive transmit frequency shift when in CW which means that neither the display or the tuned frequency changes when going from USB to CW mode.  This was pretty common in the era (many makers - including Drake - did it this way) which meant that if the operator wanted to know the actual frequency of their transmitted signal that they would have to do some mental math.

One "quirk" that I need to investigate is that if this radio's heterodyne oscillator is set precisely according to the manual, the receive (and transmit) frequencies do not match the display, being offset by a bit more than 100 Hz.  This is easily corrected by setting the display to a known frequency, inputting a signal 1 kHz above and below (for USB and LSB, respectively) and adjusting for an audio tone of 1 kHz, but doing so shifts the passband of the crystal filters audibly - and in CW mode, it puts the center of the passband at about 1200 Hz.  This slight shift does not result in either "tinny" or "muffled" audio when using SSB on either sideband, and the radio sounds quite good on air!

As this offset - which is mentioned in the manual as being around 1000 Hz - appears to be programmed into PROMs, it does not seem possible to shift the local oscillator to overcome this issue - and while there's a difference between the USB and LSB passband, it is not a "show stopper" but a 1200 Hz-centered passband for CW is too high in my opinion.  I suspect that this being a very early production radio may have something to do with this issue and I'll have to think about possible ways to address it.

When a "Mic Gain" control isn't really "Mic Gain"

Another unusual design feature of this radio is the transmit audio path.  From the microphone input the signal path goes directly to the amplifier (there's no level adjustment preceding it) and into the clipper/compressor stage.  Interestingly, the clipper/compressor takes the form of a logarithmic amplifier which has less of a sharp "knee" than a typical clipper, making it quite effective in functioning very much like a compressor-type speech processor.

The designers made an interesting choice here:  The control marked "Mic Gain" is placed in the signal path after the clipper/compressor - but this has some important implications.  In testing, I used an old Sure 440SL high impedance dynamic microphone which has a fairly high output level, but this caused the clipper/compressor to be "hit" very hard:  On-air reports indicated that that I was readable, but that my speech processing was very "heavy" and off-air recordings from a remote WebSDR verified this.  Since the "Mic Gain" control is between the clipper/compressor and the radio's balanced modulator, it affects only the RF output power and how hard one is "hitting" the ALC and doesn't affect the amount of audio compression at all.

What should really have been done was to include a means of adjusting the microphone level into the clipper/compressor stage and this could take the form of having a level control on the microphone itself or in a box between the microphone and the radio, or, if the same microphone will always be used with the radio, put such a control inside the radio.

To accommodate this need, I rummaged around my parts box and found a 500k vertical chassis-mount trimmer potentiometer. This potentiometer was wired such that the "CCW" (counter-clockwise) end was grounded and the opposite end connected to the microphone jack with the audio to the radio on the wiper.

Figure 13:
A 500k potentiometer - reachable using a long, thin blade
screwdriver is accessible through the 1/4" TRS MIC/KEY
connector on this radio.  See text for more details.
Click on the image.

As depicted in Figure 13, behind the 1/4" MIC/KEY jack is a 5 volt regulator in a TO-3 case - but this doesn't line up with the connector, so I glued the potentiometer to a small piece of circuit board to allow it to be offset.  When I glued the pot to this board, I took care to avoid fouling the adjustment knob and after curing.

I then glued the small piece of circuit board to the top of the 5 volt regulator, taking care to offset it so that the potentiometer was aligned such that a long, thin blade screwdriver through the MIC connector could be used to adjust the level from the microphone being applied to the MIC amplifier.  

The adhesive that I used was "Shoe Goo" which remains flexible:  I would not recommend epoxy, cyanoacrylate ("super") glue or hot-melt glue as none of these are a good choice in this application (e.g. the bonds will fail with temperature cycling and/or mechanical stress.)

Adjusting this new "MIC Level" control is an iterative process:  Plug in the mic - check the ALC deflection and output power, unplugging, and then making the necessary adjustments and doing it again.  The goal here is to have enough audio to activate the compressor, but not so much that it sounds very "heavy" on-air.

As noted earlier, THIS radio uses a 1/4" TRS connector rather than the round, multi-pin connector used on later production models:  If this radio had this latter connector, blocking access to an adjustment behind it, I would have mounted the potentiometer facing down and drilled an access hole in the bottom of the chassis, probably making a right-angle bracket on which it could be mounted.

Carrier balance

One interesting omission by the designers is the lack of a "carrier balance" control.  When SSB is generated, the "balanced modulator" - which literally mixes the audio with RF - this carrier is nulled on most radios via one or two adjustments to minimize the amplitude of the original carrier - but not on this radio.  This radio uses a diode-ring type of doubly-balanced mixer and by themselves these typically have a "bleedthrough" of between 25 and 35 dB- much less than the 40-50dB of a typical balanced modulator in an analog SSB transmitter after it has been carefully nulled.

What this means is that on 40 meters there is a carrier bleedthrough of about 200 milliwatts (which varies depending on whether you are using USB or LSB, with band and operating temperature) when keyed down with no transmit audio.  Compared with a 100 watt output level, this represents a level that is 25-30 dB below peak power that cannot be adjusted.  This is nowhere near enough to impair efficiency of the transmitter by "wasting" power in the carrier but it is enough to be easily visible to the "waterfall police" using a modern digital radio with a spectral display if the conditions are good.

Frequency (in)stability

When it came out, this radio was remarkable compared to its contemporaries in that it didn't really drift:  You set the frequency and it just stayed there, within a few Hz.  Unlike most radios of the day, it moved only a few Hertz from the instant that it was turned on while most others at the time would change by hundreds of Hz in the first half hour or so - particularly if operated in a cold environment.

Compared to today's radios, the synthesizer is a bit crude - it has large (100 Hz) tuning steps and a bit slow to lock.  As the radio uses rather low reference frequencies (100 and 163 Hz) for its two synthesizers, their oscillators are rather slow to respond - but this also means that they are easily disturbed by slight changes in power supply voltage, mechanical vibration and just the physics of electronic circuits.

What this means is that the frequency can easily "wobble" a few Hz - or even 10s of Hz - around the nominal frequency in the short term.  This is generally unnoticeable for SSB usage or even RTTY - and most people will likely not even notice this when running CW - but it does make this radio unsuitable for some of the very narrow digital modes that are seen today, like FT-4, FT-8, WSPR, PSK31 or similar - a trait that it shares with some of its non-synthesized (VFO-only) predecessors.  These modern digital modes require that the radio be stable within 1-2 Hz at any given instant over the duration of the transmission/reception window - and this radio simply may not be able to do that.

Mechanical work

If you look very closely at Figure 1, you'll see aluminum brackets on either side of the front panel that were used to screw it to the underside of the dash on the CJ-7 in which it was mounted.  During my refurbishment, I drilled out the pop rivets on these brackets and filled the holes - and a few scratches - with metal-filled epoxy and sanded them down.

Even though the exterior of the case was in reasonable shape, it did show a bit of the wear of having been in a vehicle or two for over 40 years, so I decided to repaint it.  Having been in the vehicle for so long, the original light blue color was varied, depending on how much sun had faded it, but inside the top cover - out of sight - was a "virgin" section of paint to which I was able to find a very close match at the store:  Rustoleum satin "French Blue".  Just in case I - or someone else - wanted to match the original color, exactly, I masked off and left a patch of the original paint inside the lid.

Aside from a bit of wear on the knobs and slight yellowing of the panel meter's clear plastic - most of which was removed with the application of a bit of elbow grease and Novus plastic polish - the radio looks almost brand new.

On the air

I've made several contacts on the air with this radio and and have gotten good reports.  Even with the prevalence of waterfall displays these days, few people mention the slight carrier leakage - but I also wonder how many people actually look at their waterfall not to mention how many others would immediately recognize carrier leakage, anyway?

The addition of the "MIC Level" potentiometer was a good one.  When properly adjusted, the radio now sounds "normal" rather than very heavily "compressed" as before.

I haven't used the radio enough to become very adept at quickly tuning across the band using the UP/DOWN toggle switches, constantly overshooting signals - but I'd guess that this would be a skill that could be readily acquired.  At the risk of sacrilege, I'm considering the addition of a small, PIC-based microcontroller board that will track the button presses and the current band selection to "pre-set" the frequency when the unit is powered up and band is changed, making it a bit more convenient to use:  Such a modification would be completely reversible

Final comments

One should treat this radio in a way similar to "vintage" radios of decades gone by.  It's remarkable in its capability and design considering that it's nearly a half-century old and it needed relatively little repair - and even more remarkable in that most of the parts that it uses are still available from electronics suppliers at the end of the first quarter of the 21st century - not something that is likely to be true of today's radios in 50 years!.

As a general-purpose radio for SSB, CW and even RTTY operation, it's still very usable:  Its small size belies its capabilities, particularly in context with its vintage.  Being made prior to 1980, it obviously lacks the WARC bands (30, 17 and 12 meters) - but so do other radios of that time period.  Once the radio was restored - mostly a matter of replacing electrolytic capacitors - it operates pretty much as it did when it was new and it would not seem out of place on the air among modern radios on the air.

Given its quirks (no tuning knob being the most obvious) it is a bit of curiosity, reminding the user of a time just before completely analog radios gave way to synthesized radios becoming the norm - a revolution not too dissimilar to the more recent trend of "analog" radios giving way to those that are almost entirely digital from the antenna port to the speaker.

* * * * * * * 

Alignment notes

Here are notes related to aligning the Astro 200 (Non "A" version) - although they should be generally correct for the "A" version as well.  These should be used to augment the instructions noted in the operation/maintenance manual.

Power supply check - IMPORTANT!

  • Verify 11.0 volt power supply - adjust R92 on synthesizer board as appropriate.
  • Verify that 11.0 volt supply will remain stable down to a supply voltage of at least 11.5 volts as measured on the radio's voltage input.
  • Verify 8.0 and 5.0 volt supplies (each being +/- 0.25 volts of nominal).  Note that there are two separate 5.0 volt regulated supplies.

Reference (Master) oscillator:

  • Frequency counter to set to 5.000000 MHz or use WWV setting (which listens to 10 MHz via a direct-conversion receiver) and listen for zero beat
  • Set C52 for 5 MHz, exactly.  This is accessible via a small hole in the bottom cover.

Carrier oscillator:

  • USB/LSB
    • MIC Gain CCW
    • RIT and FINE at 12:00 position
    • MODE to USB
    • Key radio and adjust C180 for 5.601650 MHz
    • MODE to LSB
    • Key radio and adjust C174 for 5.598350 MHz
    • MODE to CWN
    • MIC Gain fully CW (for minimum CW TX power) and connect radio to dummy load.
    • Key radio and adjust C204 for 5.60060 MHz

RX Delay adjustment - used to delay time between release of PTT/VOX and RX activation

  • Adjust R239 for desired delay time preference in switching from TX back to RX when PTT is released.

VOX Trip and Anti-Trip

  • Turn on VOX and set volume to desired level using your typical ham shack speaker/audio environment.
  • Adjust R181 for VOX activation level with normal speaking voice.
  • Adjust R158 for anti-VOX level with signals/static present to prevent unwanted triggering.

Meter adjustments.  Be sure to view meter "straight on" and consistently to minimize parallax for the readings below.

  • VSWR shutdown/reflected power:  R312 calibrates the VSWR shutdown of power.  DO THIS STEP AS QUICKLY AS POSSIBLE.  Be sure to view the meter "straight on" to avoid parallax in the following steps.
    • NOTE:  As mentioned earlier in this article, I had to "repair" the meter by re-winding its coil and using an external driver circuit.  If you restore the meter in this manner, do THIS step before the other "Meter adjustment" steps.
    • Connect two 50 ohm loads in parallel for 2:1 VSWR (25 ohms) - use the shortest length coaxial cable possible.
    • Set to a mid-band frequency on 20 meters.
    • Set meter switch to REF
    • In CWW mode, turn MIC gain fully CW, key transmitter.
    • Increase power.  Quickly adjust R312 so that the forward power can not be increased to more than 90 watts on the forward meter and unkey.
    • In VSWR mode, the meter should read about 2.
  • Forward power:  R306 calibrates forward power reading.
    • Connect 50 ohm dummy load and power meter.
    • Set the radio to a mid-band 40 meter frequency and pre-set the MIC gain control fully CW to set minimum power.
    • In CWW mode, turn MIC gain CCW, key transmitter and adjust for 100 watts on the power meter.
    • Adjust R306 for full-scale indication indication (to the "Set" marking) on meter.
  • ALC Setting.  Be sure to view the meter "straight on" to avoid parallax in the following steps.
    • Connect 50 ohm dummy load and power meter.
    • Set MIC gain to 12:00 position, meter mode to FWD. (CONFLICT:  Manual says says fully CW in earlier section about adjustment)
      • Note:  Since the transceiver has no actual "Microphone Gain" adjustment prior to the clipper, the fully-CW adjustment setting would make sense as it will maximally drive the ALC (worst-case).
    • Key transmitter and whistle or produce tone into the microphone.
    • Adjust R296 for a reading of an average of 40 watts on the power meter.  This should correspond roughly with a reading of "30 over" on the meter.
  • ALC Meter setting.  Be sure to view the meter "straight on" to avoid parallax in the following steps.
    • Connect to 50 ohm dummy load.
    • Set mode to CWW, meter to ALC and set MIC Gain fully CLOCKWISE
    • Key transmitter:  There should be low/no power.
    • Adjust R291 for FULL SCALE ALC meter deflection.

AGC set-up.  Be sure to view the meter "straight on" to avoid parallax in the following steps.

  • Connect signal generator to antenna input and mode to CWW.
  • Set front attenuator switch to OFF (down)
  • Set for 20 meters and tune to a frequency mid-band and adjust the signal generator so that there is a tone of about 1 kHz
  • Set the signal generator for an output of 1.5 microvolts (-103.4dBm)
  • Adjust R280 for an S-meter reading of S3.
  • Increase the signal to 50 microvolts (-73dBm)
  • Adjust R272 for an S-9 meter reading
  • Re-check the steps above for 1.5 and 50 microvolts and adjust as necessary.

Sidetone Level set

  • Connect to 50 ohm dummy load, set to CWN and adjust MIC gain control fully CLOCKWISE (minimum power)
  • Key transmitter and adjust R257 for desired sidetone level in speaker.

In-depth alignment:

Carrier oscillator peaking

  • Using and oscilloscope or high-impedance RF voltmeter, measure the amplitude at the base of Q60
    • Adjust L11 for maximum amplitude.  Use only a plastic adjustment tool to avoid breaking the core.
    • Check carrier oscillator frequencies as noted above - adjust as appropriate.

TX mixer and ALC attenuator

  • Connect 50 ohm dummy load.
  • Set to CWN and adjust fully CCW (max power)
  • Key down and adjust L6 for maximum signal on collector of Q20 using an oscilloscope or RF voltmeter.  Use only a plastic adjustment tool to avoid breaking the core.

WWV receiver adjustment

  • Set MODE switch to WWV and turn AF gain all of the way down.
  • Apply signal generator at 50uV (e.g. -73dBm - equivalent to S9) to antenna, offset from 10 MHz by about 1 kHz so that a tone will be heard.
  • Connect AC voltmeter to speaker and adjust level to indicate on meter, but keep it well below clipping.
  • Tune L15 for maximum speaker output.  Use only a plastic adjustment tool to avoid breaking the core.
  • Remove input signal.
  • Using a high-impedance RF voltmeter or oscilloscope, adjust L16 for maximum 10 MHz at collector of Q77.  Use only a plastic adjustment tool to avoid breaking the core.
  • A signal of 5uV (-93dBm) should be audible.

Noise blanker adjustment

  • Connect a signal generator to the antenna input.
  • Adjust receiver and signal generator for a mid-band 20 meter frequency and adjust for a level of 100uV (-67dBm) and an approx. 1 kHz tone in the speaker.
  • Adjust L9 and L10 for maximum voltage on D30.  Use only a plastic adjustment tool to avoid breaking the core.breaking the core.

SWR Bridge adjustment

  • Connect two 50 ohm loads in parallel for 2:1 VSWR (25 ohms) - use the shortest length coaxial cable possible.
  • Set MODE switch to CWW and set MIC Gain control fully CW (minimum power) and set to mid-band on 20 meters.
  • NOTE:  Do the following measurements as quickly as possible to minimize stress on power amplifier.
  • Key down.  Increase power (MIC gain turned CCW) and note that SWR protection limits to 90 watts as adjusted in SWR protection steps noted above.
  • Note power reading on front panel meter and external wattmeter (if used) and then un-key.
  • In the same manner, check the maximum power into the same 2:1 VSWR on 80, 40 and 15 meters.
  • Adjust C3 as necessary for flattest (most consistent) power reduction on all bands:  Power should be between 80 and 105 watts.
  • On 10 meters, power into a 2:1 VSWR may be in the 70-80 watt range.

RF Tuning assembly

This is the unit inline with the BAND switch.  The coils noted below correspond with the frequency range and should be adjust for best response across that noted below.

NOTE: 

As the receive and transmit filter inductors are not normally accessible, it is necessary to remove the band switch module to perform these adjustments - a laborious task which requires unsoldering a lot of different cables and removal of the front panel.  It should be done ONLY if problems are suspected.  These adjustments should only be done with a spectrum analyzer and tracking generator OR a VNA/SNA.

If the sensitivity of the receiver is adequate and the transmit drive is within specifications, there is probably little need to even touch these adjustments.  As my radio was "up to spec" in terms of sensitivity and TX drive, I did not pull the module and make any adjustments.

Use only a plastic adjustment tool to avoid breaking the cores.

Receive filters

  • 80 Meters:  L101, L102 - 3.5-4.5 MHz
  • 40 Meters:  L103, L104 - 7.0-7.5 MHz
  • 20 Meters:  L105, L106 - 14.0-14.5 MHz
  • 15 Meters:  L107, L108 - 21.0-21.5 MHz
  • 10 Meters:  L109, L110 - 28.0-30 MHz
  • WWV:  L111, peaked at 10.0 MHz.

Transmit mixer band-pass filters

  • 80 Meters:  L201, L202 - 3.5-4.5 MHz
  • 40 Meters:  L203, L204 - 7.0-7.5 MHz
  • 20 Meters:  L205, L206 - 14.0-14.5 MHz
  • 15 Meters:  L207, L208 - 21.0-21.5 MHz
  • 10 Meters:  L209, L210 - 28.0-30.0 MHz

Synthesizer adjustments

Unless the synthesizer has difficulty locking - particularly at the upper or lower edge of one or more bands - there's probably no need to make these adjustments.

Major Loop VCO

  • Adjustments should be made at low edge of the respective band.
  • Coil should be set for a voltage of 2.5 +/- 0.25 volts on R18
    • Exception:  For units that can tune to 27.0 MHz, the voltage should be 3.0 +/- 0.25 volts when tuned to 28.0 MHz.
    • Start with the highest band first.  For the progressively-lower bands, the following inductors are in series meaning that a higher-band coil's adjustment will affect all lower bands.
    • 10M:  L9
    • 15M:  L8
    • 20M:  L7
    • 40M:  L6
    • 80M:  L12
  • Notch filter:  Adjust R11 and R15 for minimum amplitude of 100 Hz signal on the output (pin 6) of IC21 (0.035Vpp or lower)

Minor Loop VCO

  • Adjustments should be made on low edge of the respective band.  (Manual isn't clear about this)
  • If adjustment is needed, it will be necessary to remove the brass shield by unsoldering its three corners.  Note that the presence of the shield may affect tuning, so it may be necessary to iteratively replace it during the process.
  • Coils should be set for a voltage of 1.6 +/- 0.2 volts as measured on R21.
    • Start with the highest band first.  For the progressively-lower bands, the following inductors are in series meaning that a higher-band coil's adjustment will affect all lower bands.
    • 10M:  L5
    • 15M:  L4
    • 20M:  L3
    • 40M:  L2
    • 80M:  L1
  • Notch filter:  Adjust R25 and R27 for minimum 165 Hz signal (0.025Vpp or lower) on the output (pin 6) of IC20.
* * * * * * *

This page stolen from ka7oei.blogspot.com

[END]



Tuesday, April 8, 2025

Using a PIR to reduce wear and tear on a Nixie clock

"Does a lit-up Nixie tube in a forest wear out even if there's no-one to see it?"

Figure 1:
The "Black'n'wood" Nixie Clock (blue back-light turned on)
with the PIR (Passive InfraRed) sensor to the right.
With no detected movement in the room, the high voltage
supply turns off, reducing wear on the tubes.
Click on the image for a larger version.
This millenia-old riddle has a simple answer:  Yes.  Yes, it does.

This article has not so much to do with this specific model of Nixie clock, but rather adding a PIR (Passive InfraRed) sensor to turn off the display when there is no-one in the room to look at it.

They wear out!

Nixie clocks and other neon-glow displays (e.g. Panaplex), along with VFD (Vacuum Florescent), Numitron and CRTs have a "wear out" mechanism when they are operating:  In other words, when they are on, they are slowly degrading.

By limiting the "on" time of such displays only to when someone is likely able to see it one can prolong its overall useful life in many cases.  As many of these devices are no longer made, the supply of "new, old stock" tubes is very limited and what there is still available is becoming more expensive year upon year.

* * *

A few years ago - at a swapmeet - I picked up a "Nixie" 1 clock - the "Black'n'wood" by Nocrotec.  It was in a plastic bag with loose parts, but for only $20 I couldn't resist!

Getting it home I found the problem:  One of the elements of the "10s of hours" tube was shorted internally and very visual close inspection revealed that two internal wires were touching each other.  A bit of "percussive repair" (banging it on the table) moved the two wires away from each other and the tube was once again usable.  I suspect that the problem was originally caused by the tube experiencing mechanical shock.

The current limiting resistor associated with this same element was burned, so replacing it returned the clock to full operation.

"Could I use one of those microwave motion sensor boards instead of a PIR module?"
 
Motion sensor boards that use low-level microwave energy are cheap and available.  These work in a manner similar to the old "Proximity Fuse" - an electronic sensor used to detonate bombs a certain height above ground.  By detecting interference to its own oscillator by the disturbance of standing waves in a room caused by movement, they can also be used to turn on lights, open doors, etc.

While the use of radio waves instead of (infrared) light means that they can sense movement through walls or behind many non-conductive materials like plastic or wood - albeit with some diminution in sensitivity - this property may make them less desirable in this application:  If you want to turn off the clock when no-one is there to see it, you likely don't want it to turn on when it detects movement at a farther distant - even in the next room.

One advantage of a PIR sensor is that it may be placed to limit its range of sensitivity to reduce false triggering - including from pets:  If you can't see it, it probably can't see you!

Over the next year or two the clock has continued to work fine - although the display got "glitchy" and began to dim - but the biggest clue was that the flashing colon neon lights were flickering but this was quickly traced to the failure of the main high voltage filter capacitor on the 180 volt supply:  These problems went away with the replacement of that capacitor - but I digress.

* * *

All of this brings me to the main topic of this article:  Reducing the wear and tear of the neon tubes.  

Sitting unused, in a box, many "vacuum" devices (I'll include neon indicators and other cold-cathode tubes in this category even though they are not strictly "vacuum" devices) have the property that laying on the shelf, they (usually) have little/no degradation over time.  There are many (now) century-old devices that have been sitting around that work just as well as they did when they were made - the caveat that they haven't been compromised in some manner (e.g. broken, corrosion, failure of a seal, etc.)

Like most "vacuum bulb" devices - which include thermionic tubes/valves (with a filament) and those without a filament - like neon indicators - there is a definite lifetime related to acceptable performance when they are operating.  For normal tubes/valves, the emission from the filament/cathode will inevitably drop over time - often due to gradual degradation of emissivity and the "work function" of the cathode.  "Cold cathode" devices (e.g. those without a filament) like neon indicators also suffer degradation - and the causes are broadly similar:  Degradation of the materials and subsequent contamination.

In the case of the neon indicators, one major cause of degradation is the inevitable "blasting" of atoms from the electrodes' surfaces (called "sputtering") where the metal gets liberated - only to redeposit elsewhere.  The most obvious result of this is that the inside of the of the glass envelope darkens, reducing the brightness of the display - but even if the glass were to remain clear, this and other effects conspire to reduce the brightness overall.

Running neon indicators such as these "Nixies" at lower than maximum current will reduce these effects - but what about not running them at all?

Nixies are meant to be seen!

The entire point of a "Nixie" clock is that it is cool to look at - but what if no-one is there to see it?  As the conceit at the top of the page states, if we operate a Nixie tube in a forest and no-one is there to see it, it still wears out!

The goal, therefore, is to turn off the display when no-one is in the room.

Turning off the display

First, we need to figure out how to turn off the display, presuming that the clock or other device has no obvious means of doing so (e.g. there is no "turn of the display" switch or pin).  Two options came to mind:

Approach #1:  Removing the power

Figure 2:
Interface with HV converter.  PNP transistor "Qa", when
its base is pulled low, injects current into Pin 5 of the
HV converter chip, effectively turning it off.
Click on the image for a larger version.
As the "Black'n'Wood" clock has a battery back-up, I first tried the most obvious thing:  Interrupt the power to the clock if no motion was detected.  This worked - in theory - but I soon noted that the clock was losing almost a minute every day.

After I'd first repaired the clock, I applied correction factors via its menu and got it to stay within a fraction of a second per day - but I had assumed that this was done in the clock module itself (as some Dallas/Maxim devices are equipped) but this was not so:  While the timekeeping module continued to run on the battery, the firmware on the clock itself - being powered down - was obviously not and the calibration that I'd applied was missing, explaining why it was keeping time so badly.

To be sure, I could have likely done something to "fix" this (e.g. trim the oscillator with a tuning capacitor, added a GPS module to auto-set the clock, etc.) but since the clock - while it was running normally - was very stable, I decided to try another approach.

Approach #2:  Turning off the high voltage

Figure 3:
A top-down view of the components added to the high
voltage switching converter IC to produce the circuit depicted
in Figure 2, above.
Click on the image for a larger version.
The clock itself runs on 12 volts DC and to get the 150-180 volts needed to drive the neon displays, there is an onboard voltage converter.  While no schematic seems to be publicly available for this particular clock, the various sections of its circuitry are easily identified by visual inspection:  A large-ish inductor adjacent to a high voltage capacitor flagged the location of the voltage converter and the chip next to those components.  

This clock uses two switching supplies - the first one converts the nominal 12 volts down to 5 volts for the logic, but the second one - near the high-voltage capacitors - is the one that produces the (approximately) 180 volts for the Nixies.  Both of these use a common type of switching supply controller chip - the MC34063 - and since the implementation of these chips is spelled out in the data sheets, we have some insight as to how they work and a schematic isn't necessary to complete our task.

Fooling the voltage converter into shutting down

Like most any voltage regulator or converter, it monitors its own output voltage - typically through a pair of resistors ("Rdiv" is one of them, depicted in Figure 2 - the other, not shown, would go between the chip and ground) that are chosen to divide the desired output voltage down something close to the chip's on-board reference voltage - in the case of the MC34063, 1.25 volts, which is applied to its pin #5:  If the voltage on this pin is lower than 1.25 volts, the switching converter adjusts the voltage higher but if the voltage is higher, it reduces the voltage.

Figure 4:
A side view of the high voltage switching converter IC
showing the components added to it to allow the
180 volt supply feeding the Nixie tubes to be turned off.
Click on the image for a larger version.

As can be seen from the diagram in Figure 2, I tacked a PNP transistor ("Qa") - and three resistors - across several of the pins of the MC34063 high voltage converter.  "Pre-forming" the shape of the components to match the locations of the needed IC pins along with using a hot soldering iron to pre-tin the leads of these components and the IC itself it's possible to attach this simple circuit directly to pins 5 and 6 of the high voltage switching converter IC without risk of damage to the chip or other, nearby components.

If the base of Qa, the PNP transistor (I used a 2N3906) is pulled to ground (via the 10k resistor, Rc), it will turn on - and with its emitter connected to Pin 6 of the MC34063 - its power supply pin - it will apply current, via the 3.3k resistor (Ra), to Pin 5 of the MC34063, dragging the voltage on this pin up.  When this happens, the MC34063 will "think" that the voltage is too high and effectively turn off.  If the base of Qa is allowed to float (nothing connected to it), this transistor is biased off by the 100k resistor (Rb) between the emitter and base and the high voltage converter will run normally (e.g. the display will be on).

Any converter will do

While this article shows the example using the MC34063, this sort of technique could be applied to about any switching-type of voltage converter.  Determining a bit about the circuit itself could be done simply by referring to the data sheet of the chip that was used - as was done here - but it could also be done with a bit of reverse-engineering.

It would have also been possible to find the power supply lead feeding the voltage converter - in this case, about 12 volts from the external power supply - and interrupt it, perhaps with a relay, a PNP transistor or a P-channel FET.

If you are using an "old-school" power supply that does NOT have some sort of switching converter, perhaps consisting of a high-voltage winding, rectifier and capacitor to develop the high voltage for the tubes, your best option may be to use a relay to open the supply - preferably interrupting the pre-rectified AC side, directly.   At such voltages switching DC is best avoided due to the possibility of contact-damaging arcs:  Switching on the AC side (or between the rectifier and the first filter capacitor) is better in that the voltage falls to zero twice per cycle of the AC waveform and any arcing that does occur will extinguish at that time.

Getting the connection outside the clock

In perusing the manual for this clock I noticed that the 6 pin mini-DIN connector - intended for connection to an external GPS or DCF77 radio receiver - not only had ground (Pin 1) and power (Pin 2 for 5 volts), but also an unused pin (#4) that I verified to be floating - and to this I connected the end of the 10k resistor (Rc) to this pin with a flying lead inside the clock.  With the three needed signals (power, ground and the "disable" line) on the mini-DIN connector, I was ready to connect it to a sensor.

A PIR sensor to turn it off and on

A PIR (Passive InfraRed) sensor fits the bill for this task quite well - and they are inexpensive.  These devices use pyroelectric detectors to detect heat from warm, moving objects - which includes us humans - by focusing deep infrared energy onto a pair of sensing surfaces from an array of Fresnel lenses.  A moving object in the field of view will cause a difference in the pair that can reliably indicate that an object in view is in motion.

Figure 5:
This circuit was added to the output of the PIR to present
an open-collector to allow transistor Qa in Figure 2
to properly turn off when the HV was to be turned on.
Click on the image for a larger version.
The PIR sensor that I chose was found on Amazon - three of them for under US$10 - and it has exactly three connections:
  • Power.  This particular PIR sensor was happy to operate from between 5 and 12 volts, having an onboard 3.3 volt regulator.
  • Ground.  This is the negative supply and the reference to the output signal.
  • Output.  This output pin goes "high" (to 3.3 volts) when motion is detected.

This sensor also has two potentiometer adjustments:

  • Delay - Which is the amount of time the output will go "high" when motion is detected.
  • Sensitivity - As the name implies, this sets the degree to which the device reacts to movement.

There's also a jumper:  The piece of paper that came with the PIR sensor implies that this determines if the output is "re-triggerable" (the default setting) or not.  Being re-triggerable means that motion will reset the delay timer whenever it's detected:  If it were not re-triggerable, the delay time would be reset only after the delay had expired and the output had turned off.  Clearly, we want to use the "re-triggerable" setting so that any movement simply extends the timer.

It turns out that moving the jumper on this board from its factory position stopped the unit from working at all and a quick bit of reverse engineering revealed that whoever designed this board simply connected it to the wrong place - probably due to poor reverse-engineering on the part of the "designer" of this (likely cloned) circuit board.  Fortunately, the wiring of the circuit is such that it is already wired as being re-triggerable, so we can leave it alone.

Figure 6:
Perhaps a bit messy, but this is the two-transistor circuit
depicted in Figure 5, tacked to the pins of the PIR module's
circuit board.  The three-conductor cable that connects to the
clock via the mini-DIN connector can just be seen.
Click on the image for a larger version.

One problem with the 3.3 volt output is that it is a logic output that is limited to 3.3 volts because it has both pull-down and pull-up transistors, internally.  As we discussed in the previous section, we need to ground the base of transistor "Qa" through the resistor to disable the high voltage and let it float to an unknown voltage to allow it to turn on.  

Because the output is not an open collector or open drain, it cannot be pulled higher than approximately one diode drop above the 3.3 volt supply on the PIR chip:  This voltage is lower than the emitter voltage of the transistor that we added ("Qa") which means that Qa will always be turned on, always disabling the high voltage converter!

To fix this we need to provide an open-collector output - but preserving the polarity of the output - which is to say that we want it to be an open collector to allow the base of "Qa" to float high when movement is detected, but go to ground and turn on "Qa" when it is not.  To accomplish this, transistor "Qb" takes the "high-active" pulse from the PIR and inverts it - and then transistor "Qc" will invert it yet again, but this time with the needed open collector.  "Qb" and "Qc" can be practically any NPN transistor - I used 2N3904 types in this cicruit.

In experimenting with this PIR sensor module, I noted that when set to "maximum" the "on" time from the output was about 150 seconds - about 2.5 minutes.  I was able to iteratively adjust the "sensitivity" control incrementally upwards until I found a setting that reliably detected even slight motion in the room - but seemed not to randomly "false" trigger, the result being that even when I was in the room and not moving much - say watching TV - it would stay on most of the time, but be easily (re)triggered by even slight movements.

Figure 1 shows the clock with the PIR sensor next to it, sitting on the shelf below my TV.  I purposely set the PIR sensor back from the edge of the shelf - not just to line up with the front of the clock, but to obscure part of the view of the floor to reduce the probability that a cat would trigger it:  Since cats sleep most of the time, anyway, their occasionally triggering the PIR sensor isn't a big deal and the display remains off most of the tim.

Reducing "wear-out"

For a "cold cathode" tube like a Nixie, turning the high voltage on and off is not a stress on the tube:  After all, simply changing the segments to show the time is also turning on/off parts of the tube.  With no voltage present, there is no electron bombardment on the elements within the tube and thus, it will not experience wear.

Powering down other devices in the absence of "viewers"

There are other types of "antique" displays that may benefit from having some sort of "human presence detector".  For example, a VFD (Vacuum Fluorescent Display) has a wear-out mechanism similar to a Nixie in that electron bombardment will gradually degrade the phosphors - and the cathode (filament) may also lose emission.

Similarly, if one has a "Scope Clock" - a vector-graphics clock that uses an oscilloscope tube to show the time - it, too, will wear out over time, the emission of the from the cathode will drop over time - not to mention possible burning of the phosphor.

Figure 7:
An example of a "Scope Clock" - a vector-graphic clock
display shown on an oscilloscope using a cathode-ray tube
(CRT).  In this photo, the CRT in a Cushman CE-50A
communications monitor is being used to demonstrate, but
an old, analog oscilloscope would work as a "permanent"
fixture and blanking it when no-one is looking would
extend the life of increasingly-rare CRTs.
Click on the image for a larger version

For these two examples, a bit of care should be taken in that while removing the high voltage source may partially remove the wear-out mechanism (e.g. degradation of phosphors) other steps would be required to mitigate the diminution of filament emission over time.  This could include turning off the filament - or at the very least, reducing its voltage, perhaps in steps, in the absence of the anode voltage.  If grid voltages happen to be present, those, too, should be carefully considered to see if they should be removed when the high voltage is turned off - but since these often share the same power supply, this problem may take care of itself.

In so-doing - and depending on the nature of the display tube - other precautions may also be required (e.g. removing all other voltage prior to powering down the filament) to avoid damage - and frequent power-cycling of the filament itself may be an issue:  These are potential issues that should be considered - but are beyond the purview of this article.

Footnote:

  1. The name "Nixie" is a trademark of Burroughs Corp. to describe certain types of neon-glow indicators.  Like many trademarks, it's become "genericized".  As done in this article, nowadays it's commonly used to denote all types of similar cold-cathode glow devices in which each digit is indicated by a separate element within the tube in the shape of the desired numeral or symbol - whether they were made by the original trademark holder or not.

 * * * * * * *

This article stolen from ka7oei.blogspot.com


[END]

 

Friday, March 14, 2025

Repairing a NanoVNA "V2" with nonsensical readings ("Blown up" input)

Figure 1:
The SAA-2N, a variant of the Version 2.  As noted in the text
I chose this version as it had N connectors and was suited
for my specific needs and has served well for several years.
Click on the image for a larger version.
The NanoVNA has become a ubiquitous device for the RF toolbox:  For less than US$200 you can get a device that is reasonably capable, accurate and covers a usefully-wide frequency range - from a few 10s of kHz into the GHz range, depending on the model.

The original NanoVNA - sometimes found for less than US$50 - works reasonably well up to about 250-ish MHz - the limit of the frequency range of its RF synthesizer (typically an Si5131).  Using harmonics for the higher ranges allows the unit to "work" higher than this, but with the dropping gain of the mixers and lower power of the higher-order harmonics diminish its usefulness and it pretty much "runs out of steam" by the time one gets to around 1 GHz.

The "Version 2" of the NanoVNA (which includes many variants, such as the "H2") improved on this using a different detector (often the Analog Devices AD8342 which is rated to work above 3 GHz) and two RF synthesizers - the original Si5351 and another device (usually the Analog Devices ADF4350 or similar) that takes over from the '5351 at the higher frequencies (usually above around 140 MHz) up through 3+ GHz.  The different architecture of the Version 2 necessitates greater complexity - which also implies increased vulnerability as we'll see.

Note:  This article will generically refer to the units thus-constructed as "V2" NanoVNAs - regardless of who actually makes/sells them.

Background

When I looked for an "upgrade" to the original NanoVNA I was looking for a device that would have durable connectors that would withstand hundreds of connect/disconnect cycles and be able to hang the unit from the interconnect cables themselves to measure gear "in situ".  This "need" was due to its expected use:  Being dragged around in the equipment box to repeater and radio sites, the houses of other amateurs, and being used on the workbench - and almost never above about 1.5 GHz - a frequency range for which I have other gear, anyway.  Having friends with other NanoVNA V2 variants, I've heard how physically fragile these devices are - mostly related to the supplied cables and the SMA connectors themselves, and how they may be physically attached to the circuit board.  All of this ruled out anything with SMA connectors.

For this reason I got the SAA-2N (metal case with "N" connectors) and have used it enough that the nickle plating is starting to wear off the threads of the N connectors, indicative of a number of connect/disconnect cycles (now in the hundreds) that would have trashed even the best-quality SMA connectors:  Had anyone else made a device as physically rugged as this, I'd have considered it - but as of the time of this writing, no-one else has done so!  (Why not?)

The problem

One issue that can befall users of all NanoVNA "V2" variants is that of static sensitivity - particularly on the S11 port (e.g. "Port 1" or "CH0").  While some users on the forums suggest that this is due to "inferior" components of some of the clones, this is simply false:  It's a result of the way that the unit is designed - and the components necessary to execute it which are intrinsically more vulnerable to ESD (ElectroStatic Discharge) than simpler versions.  

Additionally - and speaking for myself -  I'm much more likely to use this unit - with its "N" connectors - "out in the field" where it may be exposed to hazards (ESD) than someone who gently rests their NanoVNA on their workbench for its entire life.  At least for me, this increases the probability that a unit that is more likely to be used out in the field - away from the "safe" workbench - will be damaged in some way, electrically or mechanically.

Specifically, the problem is the Maxscend MXD8641 RF switch found in several places on the "Version 2" NanoVNA variants (e.g. those that work past 3 GHz).  This is a SP4T (4-way) RF switch used to route the signals that, among other things, is used to switch between the Si5351 oscillator and the ADF4350 (or similar) - but one of these devices may also be found right on the S11 port - and that's where the problem lies.  (This device is not on the original NanoVNA, which seems to be more rugged in this respect.)  As the list price of the MXD8641 is well under US$0.07 in any sort of production quantity, it's unlikely that so-called "cheap counterfeits" are being used.

While the data sheet for this device indicates that it has good ESD protection, it's clear from the NanoVNA forums - and my personal experience and that of friends who also have a V2 NanoVNA - that this protection is NOT necessarily adequate for in-the-field, casual use.  If your NanoVNA V2 never leaves your static-free workbench, you may never have this sort of problem - but if you drag it out in the field like I do, you may well have run across situations where the NanoVNA becomes damaged.

Figure 2:
If the RF switch chip is has a "dead" short to ground,
you may end up with chaos of lines like this after you do a
"short-open-load" recalibration.
Click on the image for a larger version.

As it happens, a good-quality coaxial cable is capable of storing quite a bit of energy, stored as voltage.  With a typical 50 ohm coax having around 30pF per foot (100pF/meter) this, coupled with triboelectric effects - not to mention static on your person or on the antenna to which you might connect it - pose a hazard to sensitive electronics, and this is device is no exception.

Considering that the specifications for this part note that it should withstand 1kV from the "human body model" (100pF discharged through a 1.5k resistor) it's easy to see that discharging even a hundred or so volts from 3000pF of capacitance - represented by about 100 feet (28 meters) of coaxial cable - and not having any series resistance - could easily damage this part.  One can trivially develop hundreds of volts across a piece of coaxial cable just from handling - not to mention that which might be developed across an antenna from wind static!

When a NanoVNA V2 goes bad

On the NanoVNA forums I've seen people commenting on how they are suddenly getting nonsensical readings on their V2 (see Figure 2) or the apparent inability of the unit to maintain calibration - and this is indicative of possible damage to the MXD8641 found on the S11 port, likely caused by voltage discharge:  With a 0.047uF series coupling capacitor, it would not take much accidentally inject enough energy to damage that part!

My own NanoVNA V2 was, itself, damaged through discharge after having used it for several years without incident, apparently when connected to a fairly long length of coaxial cable - despite reasonable effort and care.  I have also encountered others with V2 NanoVNA variants that have also experienced similar issues and in all of the cases where I have been able to get the unit into my hands, it's been due to damage of the MXD8641.  One thing in common with these other failures is that these folks often - but not always - use their NanoVNA V2 places other than just on the workbench - to test antennas, cables, etc. out in the field:  I don't know about you, but I can detect a common thread here!

Comment:  

As can be seen in Figure 3, there is a 0.047uF monolithic ceramic coupling capacitor.  Ideally, a capacitor tester would be used to verify its integrity, as would an ohmmeter to assure that it's not shorted - even intermittently.

It is possible - particularly if the NanoVNA V2 has board-mounted SMA connectors - that if the things are flexed repeatedly (tightening of the connectors or other mechanical stress) that this capacitor and/or the solder joints in the signal path have broken or become intermittent.  It would be a good idea to use an ohmmeter to "buzz" out continuity from the end of the cable to the "connector" side of the coupling capacitor, and also between the other (circuit-side) lead of the capacitor and the trace.

Sometimes, reflowing both ends (allowing time in between for the two solder connections to cool) will restore connectivity if the solder joint has cracked - but note that the capacitor itself may be mechanically intermittent and thus require replacement, anyway.

Diagnosis:

Having corresponded with several others who have had the misfortune of damaging their V2 NanoVNAs, there are several ways that the damage will manifest itself that may appear to be totally different, but are actually the caused by the same problem.

  • Sudden high return loss everywhere.  Sometimes the discharge will cause the '8641 to simply fail dead-shorted and the user will see a very high VSWR on everything and if one configures the unit for an S21 (e.g. "through") reading, the apparent insertion loss is extremely high - indicated by a very high noise floor (after attempted recalibration) as compared to what it was when working.  If one attempts to recalibrate (Open/Short/Load) a completely nonsensical display like that in Figure 2 is likely to result after doing so.
  • Unit will not seem to "hold" calibration well.  This seems to be the more common failure:  The user will suddenly find that the unit is out of calibration for no obvious reason - and this is often worse at higher (VHF/UHF) frequencies than at HF (30 MHz or lower).  Using the Open/Short/Load, the unit will seem to calibrate, but the noise floor in "S21" measurements will likely be higher - and the calibration will seem to drift all over the place over time and with temperature.

This second failure mode is a bit more sinister in that the user may, at first, presume that the loss of calibration was a result of user error.  What has actually happened was that rather than fail shorted, the '8641 will be damaged, often putting between 30 and 80 ohms of resistance between the input port and ground  - a value that will vary significantly with temperature and over time.  This is insidious in that the unit may "seem" to be working - but it will likely give incorrect readings, even if it seems to calibrate properly.  This causes two problems:

  • Calibration drift.  The NanoVNA's source impedance is nominally 50 ohms - but placing a varying resistance across this - possibly in the 30-80 ohm range - will lower this, causing calibration to seem to vary despite frequent recalibrations.  As noted above, if an "S21" measurement is done (e.g. a "through insertion loss"), the shunting of the source signal (on CH0/Port 1) will reduce its amplitude - possibly significantly - and you may notice that the noise floor is higher than expected as the signal levels have been reduced.
  • Misleading results.  What's worse is that even though the unit will seem to calibrate correctly using the Open/Short/Load, the fact that it is no longer sourcing or loading 50 ohms on the Ch0 port can cause misleading readings if you are trying to sweep a filter, antenna, cable or other device that is expecting a source impedance in the area of 50 ohms.  This may be proven by using a known-good 50 ohm cable of significant length (10s of feet/meters long) and terminating it with a known good 50 ohm load:  Ideally, it should remain "flat"(low VSWR/return loss) but if the unit itself no longer sources/loads 50 ohms, this test will reveal something other than a flat response.
    Figure 3:
    The screwdriver tip is touching the "circuit" side of the
    0.047 uF coupling cap.  It is between this point and ground
    that one would test with a digital Ohmmeter to determine if
    the RF switch chip has been damaged.
    Click on the image for a larger version.

A quick check with an Ohmmeter will reveal the problem and figure 3 shows where a measurement may be made, on the "circuit" side of the blocking capacitor on the CH0/Port1 terminal. This photo shows the SAA-2N, but your model may have a slightly different layout, but it should be pretty easy to locate this capacitor and do a similar test on other variants.

If all is well, a typical digital Ohmmeter will likely read around 10k or higher with the unit powered down - but if you get anything lower - specially if it is in the hundreds of Ohms or lower (it is likely to be in the 10s of ohms if you have noticed a problem) - the MXD8641 is likely blown.  (Do NOT use the "diode test" function of your Ohmmeter.  Be sure to check your Ohmmeter in both directions to rule out a reading a protection diode on the chip.)

As mentioned earlier, the MXD8641 is a very inexpensive part - but it's difficult to find from U.S. suppliers - and for this reason I sourced a strip of the MXD8641 on EvilBay with each part costing well under US$1.00, including shipping.  Replacing this part, however, is another matter as we'll see shortly.

A promising equivalent part would seem to be the Skyworks 13414-485LF (available from DigiKey) which is also a SP4T switch - in the same package and with the same pin-out - but despite what look like identical specifications, parameters and truth tables in the data sheet, the units that I got from DigiKey did not work in the 'V2 for reasons still unknown.

Figure 4:
Highlighted section shows the installed TVS - the 30 volt
0603-package part mentioned in the text.  It is laying on its
side, which was the easiest orientation for mounting.
Click on the image for a larger version.
Input protection

If one makes it standard practice to always place a resistive attenuator (say, 6-10 dB) on CH0/Port1 of their VNA - and does calibrations with it in place - this may reduce the probability of damage, but doing such may complicate certain types of measurements due to the added loss and reduction of signal levels.

Unfortunately, none of the V2 variants that I've seen have included overt protection in addition to that intrinsic to the MXD8641 - and this would likely be in the form of a low-capacitance TVS diode.  As it happens, there are a number of TVS diodes that have very low capacitance (0.5pF or less) that are specifically intended for protection of GHz-range devices (HDMI, USB3 and RF/antenna) which make the suitable candidates for use with a NanoVNA.

The device that I chose was the Inpaq EGA10603V12B0DG - a 12/30 volt, 0.2pF part in a 0603 SMD package (DigiKey P/N:  3526-EGA10603V12B0DGCT-ND).  There are other devices with low capacitance with even lower voltages (which would have been preferred) but these were available only in 0402 (or smaller!) packages, making their handling very difficult:  As it is, a 0603 package is about 1/4th of the size of a grain of rice!

With a fine tip and small-diameter solder, it's possible to add the TVS diode.  Figure 4 shows how this might be done on the SAA-2N:  Adjacent to the blocking capacitor, the green coating is scraped off the board to bare the ground plane and the TVS diode is installed.  I find it a bit easier to set the TVS on its side, but your mileage may vary.

You will note that the TVS is placed on the "circuit" side of the blocking capacitor rather than on the antenna terminals.  The reason for this is that if there is a voltage across the input (and thus across the capacitor) that is then shorted, the energy of the 0.047uF capacitor (plus any "ringing" from inductance/resonance) will be dumped into the circuitry.  By placing the TVS on the "circuit" side, it will be able to dissipate at least some of the energy dumped by the capacitor, placing an absolute limit on the voltage peak applied to the '8641.

How much effect does this TVS have on the readings?  I've added one to a perfectly-functioning Version 2 NanoVNA and then re-checked the calibration:  Below several hundred MHz, there was no detectable effect of the device's small amount of capacitance - and even well into the 2+ GHz range, the effect was very minor.

As I rarely use my NanoVNA above about 1.5 GHz, this effect was acceptable - and the added protection against damage (that is, finding your NanoVNA non-functional at a radio site - possibly disrupting the planned activities - perhaps resulting in a wasted trip unless you have a spare VNA or equivalent!) is worth it. The 0.2pF capacitance of this device is probably less than stray capacitances in the circuit/layout, anyway.

Figure 5:
Location of the failed chip (U551) - the first active component
in the signal path on CH0/Port 1 of the VNA - and the one
most likely to be damaged.  The SAA-2N is shown above.
Click on the image for a larger version.

Note:  I haven't put similar protection on CH1/Port 2 as it's less-commonly used - and it's typically used in conjunction with a device under test that is less likely to produce ESD.  If you are measuring the loss of coaxial cable, however, it would be a good idea to dissipate any stored charge on it (shorting the center to the shield - or even touching across the two with your fingers) prior to connecting it to either terminal of the NanoVNA.

Replacing the MXD8641

If your 'VNA has already been damaged, it may be too late unless you have the equipment to do small surface-mount work.  For such work, it's not so much skill that is needed - but the right gear (hot-air rework, ceramic tweezers, etc.) and good magnification is required:  None of this is particularly expensive as a suitable hot-air rework station can be had new for well under US$100.

Using the hot air rework wand with a small-diameter blower tip (Figure 6) the chip is carefully heated and using ceramic tweezers (which are fairly heat-insulative and non-conductive) the old, blown-up chip is lifted off - noting the orientation of the small dot on the original chip - which, on this board, corresponds with the "arrow" symbol seen at about the 7 o'clock position on U551 in Figure 5.  This image shows the location of this chip on the SAA-2N, but it will be located near the connector itself on other models - you may need to trace the signal path for other models.

Figure 6:
Heating the failed chip with a hot-air rework tool.
Be sure to note the orientation of the tiny dot on the chip
before you remove it!
Click on the image for a larger version.
Flooding the area with a drop of "no clean" solder flux from a pen, the replacement chip is dropped onto the spot where the original was - taking care to orient its dot properly - and the area is re-heated with the rework tool.  Gently nudging it back and forth, when the solder melts it will "stick" in place as surface tension does its work - but it may be necessary to make sure that it's centered on the pad - or even push down on it slightly.  If it seems to not be centering itself, let it cool a bit and apply a bit more flux and re-heat it:  The trick here is to let the flux and surface tension do the work!  It is unlikely that more solder will need to be added as the new chip was pre-tinned at the factory and there will likely be plenty still on the pads.

Letting the unit cool - and verifying that its dot is oriented in the same manner as the original part - the unit may be reassembled and tested:  I've had extremely good luck with this method and have never had a failure - and having replaced '8641's in several Version 2 NanoVNAs, I've been 100% successful - but then, I've been doing surface-mount work for quite some time.

Figure 7:
The repaired NanoVNA, recalibrated.  The flatness and level
of the noise floor (<=-70dBm) indicate that it's well matched
and that the losses are low between 100kHz and 1.5 GHz.
Click on the image for a larger version.
Conclusion

Without careful examination of your Version 2 NanoVNA it may not be possible to determine if it has the added protection of the TVS diode - although this may be noted in its documentation.  If it does not - and you regularly take it out in the field rather than having it sit comfortably on your workbench - it's worth considering adding it.

Note:  As much as I would like to help, I'm not going to get into the business of repairing/modifying NanoVNAs in the manner described, so please don't ask - sorry.  If you have a "blowed up" NanoVNA and don't have the gear/skill to do SMD rework, find someone who can.  At the very least, you now know why this issue might happen and this may prevent you from damaging other devices in the future.

 * * * * * * *

This page stolen from ka7oei.blogspot.com 

[END]

Sunday, February 16, 2025

Ali Express "SDR TX/RX Switch" - A design NOT well thought out...

Figure 1: 
Front panel of the SDR TX/RX antenna switch showing the
the 3.5mm audio connectors and the red/green RX/TX LED -
which have been swapped to be in their proper location.
Click on the image for a larger version.

        IMPORTANT:        

If you have one of these devices, DO NOT connect it to your transceiver and second receiver (SDR) UNTIL you have read and understood the issues described here. 

Failure to understand how this device works may result in you blowing up your SDR when you transmit! 

If you wish to use it ONLY as an audio muting switch when you transmit (e.g. when using a remote receiver) see the section labeled "Audio Muting" near the bottom of the page.

I've you've been following this blog you'll note that I've used SDRs (Software Defined Radios) quite a bit - particularly for reception.  Transmitting in the vicinity of any receiver - or trying to use an outboard receiver in conjunction with a transmitter on the same antenna - is a bit problematic for several reasons:

  • If the transmitter and receiver are in close proximity and on very nearby frequencies (e.g. on the same band) then it is (nearly) inevitable that the receiver WILL be overloaded when the transmitter is active.
  • Unless the frequencies (transmit and receive) are very well separated AND both the receiver and transmitter have adequate filtering, the receiver will be overloaded by the transmitter.
  • It is possible that even if you have a separate receive antenna, it may intercept enough energy from the transmitter to damage/destroy the receiver.  If the two are on the same band, this is more likely - but even if the receiver is being operated on a very different frequency range than the nearby transmitter and there is insufficient filtering at the receiver the receiver could sustain damage.
  • It is often the case that one might have a single antenna on which there are two receivers (e.g. the receiver built into the transceiver and an outboard SDR receiver).  In this case one clearly must protect (e.g. disconnect) the outboard receiver when transmitting.

It's worth noting that most SDR receivers do NOT have particularly strong filtering in them:  Unlike an amateur transceiver - which may have separate filtering for each amateur band (or groups of bands) - this is rarely the case for wide frequency-range software-defined radios:  RTL-SDRs, SDRPlay, Funcube and others have either no band-specific filtering or rather broad (e.g. covering about an octave or even wider) filtering in them.

What this unit does

Some modern radios actually have external receive ports on them to allow you to "share" the RF while protecting the external receiver.  If your radio doesn't have that, there are/were several devices to allow this that may be found on the market (e.g. the MFJ-1708) but my attention was brought to an inexpensive unit (pictured above) that has appeared on the various seller web sites (Amazon, EvilBay, Ali Express, etc.) so I obtained one via a U.S. seller.

The description of this device is typical of those found on at the stores of Chinese sellers, curiously being both under and over-descriptive at the same time:  "160MHz 100W Portable SDR Transceivers Aluminum Alloy Box Device Radio Switch Antenna Sharer Practical Signal Equipment Accessory"

By the description, with this device it should be possible to connect your transceiver and SDR (receiver) to the same antenna, perhaps receiving using both (e.g. the addition of a waterfall to an older radio) without fear of damaging the SDR or the transceiver.

This device also has another feature:  To re-route audio when transmitting - which is probably the most usable feature of this device as it comes out of the box as we'll see.

As we'll see, this device doesn't quite work as you might think that it should.

"Documentation?  What documentation?!" 

This unit arrived in a package with (surprise!) no documentation at all - which was somewhat disappointing:  Sometimes one gets a (badly!) translated half-sheet of paper that hurts one's brain to parse - or even a URL to a page with... something... but not the case here.

From a practical standpoint, it's somewhat "self documenting" in the sense that if you ordered this device in the first place, you already had an idea as to what it was supposed to do, so it's possible to figure things out.  Referring to Figures 1 and 2 (the front and back panels) we have:

Front panel (Figure 1):

  • LED on the left-hand side.  This LED is illuminated when the unit is in "Receive" mode - that is, the "SDR" rear-panel RF connector is connected to the "ANT" rear-panel connector.  (The PC board shows this as a green LED, but on mine the red and green were interchanged during assembly:  I swapped them back.)
  • 3.5mm jack labeled "SDR".  This is a stereo (2-channel) audio jack and, during receive, both channels are connected to the "Audio Out" connector.  It is disconnected during transmit.
  • 3.5mm jack labeled "AUDIO OUT".  This is a stereo (2-channel) audio jack that is intended to be connected to speakers.
  • 3.5mm jack labeled "TRX".  This is a stereo (2-channel) audio jack that is intended to be connected to the transceiver during transmit.  Is is disconnected during receive.
  • LED on the right-hand side.  This LED is illuminated when the unit is in "Transmit" mode - that is, the "TRX" RF rear-panel connector is connected to the "ANT" rear-panel connector.  (As noted, this should have been a red LED according to the marking on the PC board but mine was populated with a green LED, which I swapped.)

Figure 2:
Back panel of the SDR antenna switch.  SO-239 connectors
are for the radio (transceiver) and antenna with the SMA for
the SDR.  The 3.5mm PTT and power connectors are visible.
Click on the image for a larger version.

Rear panel (Figure 2):

  • RADIO connector.  This is an SO-239 (female) UHF connector to which the transmitter/transceiver is to be connected.
  • ANTENNA connector.  This is an SO-239 (female) UHF connector to which the antenna is to be connected.
  •  PTT ("Push To Talk") connector.  This is a 3.5mm connector in which the center pin (tip), when grounded, will switch the unit from"Receive" to "Transmit" mode.  It's likely that a 3 or 4 wire 3.5mm cable was provided in which case only the tip (PTT) and sleeve (outer-most ring - ground) are needed.
  • SDR connector.  This is an SMA connector to which the SDR (or other auxiliary receiver) is to be connected.
  • 13.8 VDC connector.  This is a 2.1x5.5mm coaxial power connector (center positive) through which DC power is supplied.  This voltage is not critical and could be anywhere from 11.5 through 15 volts.

Also in the box my unit came with an SMA-SMA jumper, SMA-BNC adapter to adapt the SDR connector to BNC, three "audio" cables with 3-conductor 3.5mm connectors on each end, and a 12 volt switching supply (with a European "pin" plug) and a universal plug adapter:  The 12 volt switching supply seems to be the cheapest, meanest possible unit with no brand name and should NOT be trusted or used - but at least its DC cord is useful!  (In other words, do not use this power supply - particularly as it is unfiltered from an RF standpoint and it would be a really bad idea to use it on an RF receive device of any type.) 

How it actually works

As you would expect, the antenna is to be connected to the "ANTENNA" port.  When in receive mode, the "SDR" connector is also connected to the "ANTENNA" port - but the "RADIO" port is not!

What this means is that as shipped from the factory, if you connect your transceiver, antenna and SDR to the unit, when it's in receive mode, you will get no receive signals on your transceiver.  This is by design, apparently.

It is expected that the PTT connection on the back should be grounded when the transceiver is in transmit mode - and when this happens, the RADIO and ANTENNA ports will be connected to each other.  There is also an RF sensing circuit that is supposed to detect when the transmitter is producing RF, but this has its own issues as will be discussed later.

There is a jumper...

If you take the unit apart (via the four screws on the back panel) you'll see a jumper (J5 - see the schematic of Figure 3 and the photo of the board in Figure 4) and some awkwardly-worded text indicating that if you remove the jumper that you'll have "dual receive" - which means that the Radio's receiver and the SDR will be connected to the antenna at the same time.

This is technically true - but there are a number of "gotchas" here

First, let's take a look at a reverse-engineered schematic of the unit, below:

Figure 3:
Reverse-engineered schematic diagram of the unit.
The parts designators are those shown on the silkscreen of the circuit board.
Click on the image for a larger version.

Circuit description:

DC power

The DC input power via J4 is protected with F1, a 500mA self-resetting fuse and D10, a diode for reverse polarity protection while L2, a 220uH inductor, isolates the connection at RF.  Capacitors C6 bypasses RF while C7, a 220uF electrolytic, provides smoothing/filtering - likely enough to even allow an AC power source (from a 12-ish volt transformer) to be used. 

It's worth noting that there are two "grounds" on this device:  The "antenna ground" of the rear panel and RF connectors and the "shack ground" of the DC power and audio which are isolated by L1, a 220uH inductor.  On paper, this isn't a bad idea - but on this unit there's a flaw:

The back panel being used to mount the connectors and it - and the entire case - is at "RF" ground - which would be fine as that would be the same "ground" as your radio.  The problem is that the circuit board's ground planes are not set back from the edges of the board meaning that it's possible that the green insulating coating could scrape off the board and contact the case it the mounting slot, connecting the two "grounds" together - perhaps intermittently.  (Practically speaking, most people would not be likely to ever have a problem.)

Oops.

Keying

J6 is the PTT input, activated by grounding the tip of the 3.5mm connection with the outermost sleeve being the "shack" (not antenna) ground.  Diode D6 blocks positive voltage and when the PTT is keyed, the gate of Q3, an N-channel MOSFET, goes low, de-energizing all of the relays.  When the PTT line is "un-grounded" capacitor C3 and R9 charge, preventing Q3 from re-activating the relays instantly, providing about 100msec or so of delay through the charging by R3.

Comments about the keying via the PTT port

This relay keying scheme assumes that there is either NO voltage, or that there is a POSITIVE voltage on the keying line from the radio when in receive that is greater than a few volts.  There are several caveats to this:

When powered up, the relays are energized whenever it's in "Receive" mode (PTT ungrounded or no transmit RF)  What this means is that if power is removed, it's as if it's in "transmit" mode.
  • This connects the ANT to the RADIO port and the SDR port is grounded when in TX mode or powered down.
  • Additionally, the front-panel AUDIO jack gets connected to the TRX jack. when in TX mode or powered down.

The keying line from the radio must go to GROUND when keyed.  If the keying line is shared with an amplifier, that amplifier CANNOT put a negative voltage on the keying line as that will hold the SDR switch in "Transmit" mode at best, damage the SDR switch in worst case - and in either case it would hold the amplifier in a "keyed" state.


If there IS a positive voltage on the keying line when "unkeyed" it must be at least 5 volts just to assure that Q3 will turn on reliably when the radio is un-keyed - and this lower voltage may affect the duration of the "un-key" delay.  If the voltage is less than 10 volts, the full delay caused by C3 and R3 may not occur.  The 100msec or so of "un-key"delay afforded by R3 and C3 is insufficient to prevent the relays from "chattering" during SSB and CW transmissions if RF sensing is used!

  • If you are a CW operator, the unit will not switch back to receive mode as quickly as your radio might.  If you are a CW operator that prefers QSK (full break-in) you probably don't want to have this unit inline.

There is also an RF-sensing keying circuit:  Transmit RF is tapped from the RADIO RF line (from the transmitter) by C1, a 47pF capacitor and rectified by D1 and D2 and used to turn on Q1 - grounding it in the same way that grounding the PTT line does - which in turn keys the transmitter.  There is a fatal flaw in the design of this device exacerbated by RF sensing which I will discuss shortly.

Audio switching

Figure 4:
The circuit board, showing J5 in the center.
The power supply filtering is in the upper-right with the audio
relay (K3) on the left.
Click on the image for a larger version.

Relay K3 may be used to switch audio based on keying.  Let's assume that you are using a separate SDR with a computer to receive audio:  By connecting the computer speakers to the "Audio Out" connector and the computer audio output to the front-panel 3.5mm "SDR" jack the SDR audio will be muted when transmitting at which any audio from the radio connected to the front-panel 3.5mm "TRX" jack will be passed through to the speakers.

Practically speaking, you would probably never use the "TRX" jack to mute your radio's audio, but a more likely scenario is that if you are using an online WebSDR (see the WebSDR.org web site for a list) to listen on the air, you could use this to mute your speakers when you transmit to prevent your own transmitted audio from coming back with a delay and causing an echo.

RF Switching

This is where it gets a bit scary.  First, consider the configuration - from the factory - with jumper "J5" in place.

Remembering that when powered up, the relays are energized, you can see that when in "Receive" mode, the ANT port is connected directly to the SDR port - but you'll also note that the RADIO port is not connected to anything (e.g. floating).  When you transmit, the relays de-energize, connecting the RADIO port to the antenna and grounding the SDR port.  This means two things:

  • There is no receive RF at the transceiver.  Most people that I know don't use their transceiver's receiver instead of the SDR, but use them at the same time - perhaps turning down the volume on the one not being used or, more likely, using their transceiver for audio and the SDR to display a waterfall.  Not having antenna RF to be able to receive anything on the transceiver is likely not what you really want to do.
  • When using the RF sensing, the transmitter is connected to an open circuit before the relay switches.  This has several implications:
    • If you don't have the PTT line wired to your radio, there will be a split second when RF first appears that the radio will see an infinite VSWR before the relays de-energize and the contacts close, connecting the radio to the antenna.  This repeated burst of infinite SWR can progressively damage a transmitter's finals, despite the SWR protection circuitry within the radio.
    • When relay K1 does de-energize and connect to the antenna, it will be "hot switching" the relay contacts, which is to say that they will be carrying RF power at the instant that the antenna is connected.  This tends to burn contacts and shorten the life of the relay.
    • The RF sensing circuit doesn't have adequate "hang time" to ride through word pauses and CW elements meaning that it will likely "chatter", repeatedly causing the hazards noted above.

As can be seen from the picture of the circuit board in Figure 4 there's a jumper, J5, on the board with the following somewhat confusing text:

J5 Usage
Open = Dual receive wheh [sic] RX ("wheh" was probably intended to be "when")
Short = Normal Operation

By removing J5, relay K1 is never energized meaning that it is always connected to the antenna:  This helps to mitigate the problem that - when RF sensing is used - that the transmitter is connected to "nothing" as it would be the case with J5 installed - but this also means that in receive mode, the transceiver and the SDR are connected in parallel

Simply paralleling two (nominally) 50 ohm devices (the transceiver operating in receive mode and the SDR) isn't a great idea - but it will generally work "OK", particularly if the SDR and the transceiver are tuned to the same frequency range.  When the transceiver is OFF - or on a band  other than that to which the SDR is tuned - it may cause its filters to "suck out" RF and a loss of signal/sensitivity on the SDR.   

(Note:  A "properly-designed" device that shared the antenna for receive would likely include a built-in 2-way splitter which can reduce such problems, and it will also contain circuitry to protect the second receiver should excessive RF manage to find its way into it.)

The bad part here is that if you transmit - and, for some reason relay K2 doesn't de-energize instantly, as would be the case with RF sensing only - you will transmit directly into your SDR, likely destroying its front end.

Oops, again.

What this means is:

  • If you remove J5, DO NOT operate the unit UNLESS you are using the PTT cable - which is to say DO NOT rely on RF sensing alone as transmit power will briefly enter the SDR's front end before the relay can switch.  The SDR is likely to be damaged due to the lack of RF power protection on that port.
  • If your PTT cable accidentally becomes disconnected - or external keying is turned off in your radio's menu - you will transmit into the SDR and destroy its front end due to the inability of the RF sensing to act instantly and due to the lack of protection to the SDR.

The reason for this as as mentioned above:  Not only are the transceiver and SDR connected together without any protection circuitry, but also the RF sense needs to detect transmit power before it will activate - and by the time that it does, a brief burst of full transmit power may have found its way into your SDR.

A hardware bug

There is also a more subtle bug that I uncovered.  While testing the unit on the bench, I disconnected J5 - but was confused when the ANT and RADIO ports were not connected.  What was happening was that when I removed J5 - while the unit was powered up and in receive mode - enough current was flowing through LED D8 and resistor R4 to hold relay K1 closed.

Simply removing the power temporarily caused K1 to release - and there wasn't enough current to close it again, but if you are messing with the configuration, this "bug" could bite you, too!  I suppose that it's also possible that jarring the unit could cause the armature of K1 to hold in place - but I didn't try this.

The "fix" for this - if you want to bother with it - is to change resistor R4 to a 10k resistor:  This also tones down the TX LED's brightness a bit, too.

Overall comments

I get the sense that whoever designed this thing may have been copying the general idea from other, similar devices - but not really understanding what was being done, and why.  For example, the separate "grounds" implies an understanding that having them separated would be a good idea - but whoever laid out the circuit board made the "rookie mistake" of making it possible for the two "grounds" to be connected, anyway if the green coating on the board and the black anodization of the case wear through.

The description of this unit implies that it's useful up to 160 MHz.  I suspect that this is probably "true-ish", but the VSWR starts to climb when one gets to and above 6 meters (50 MHz) meaning that it's likely most useful at low power at these higher frequencies.

The cardinal - and unforgivable - sin has to do with the fact that if you want to use both your transceiver's receiver and your SDR simultaneously, you WILL want to remove J5 - but if you do - and you don't absolutely have the PTT connection working properly, you WILL blow up your SDR!

Fixing this problem is possible with the addition of some simple protection circuitry to allow the SDR to survive brief bursts of transmit power - perhaps the topic of a later post. 

AS IT IS, I WOULD NOT USE IT FOR ITS INTENDED PURPOSE, AS AN SDR ANTENNA SWITCH - at least not without significant modification.

"Audio Muting"

What it IS useful for, out of the box

What it IS useful for is an audio switch to mute your computer audio when you transmit - as you might do when using a WebSDR or other remote receiver.  For this, I would:

  • Remove internal jumper J5
  • Connect the PTT to your radio's PTT
  • Connect your computer's speakers to the "AUDIO OUT" jack
  • Connect your computer audio output to the "SDR" jack

If you are hell-bent on not using the PTT cable, the RF sense may be useful, but you would also need to:

  • Be sure that you have removed internal jumper J5
  • Connect the transceiver to the "RADIO" port
  • Connect the antenna to the "ANTENNA" port 
  • DO NOT connect anything to the SDR port

As noted before, the "hang time" imposed by the time constant of C3 and R3 may not be enough and the relay may "chatter" - in which case R3 could be replaced with a higher-value resistor of, say, 330k - or with a 1 Meg potentiometer in series with a 47k resistor to allow "hang time" adjustment.  (Adjustment of R3 is preferable to increasing the value of C3 much as the latter could also slow the activation time when RF is detected.)

Final comments

Other than to switch audio as described above, I wouldn't use this device as it is shipped for any other purpose without appropriate modification.  This makes this device a possible  "starting point" for another project (e.g. there are already some relays and a metal box!) - one to provide proper RF protection for the SDR and make the RF sensing more useful when using modes that have variable power levels (e.g. CW, SSB) which can cause the current design to "chatter".

* * * * * * *

This page stolen from ka7oei.blogspot.com

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