Kurt's Tektronix Page

I like tools. Good tools go hand in hand with the desire to build things and fix things. When it comes to building and fixing electronic things, some of the most important tools are the measurement instruments. Measurement instruments let you know what's going on with your circuit. My favorite type of measurement equipment is the oscilloscope. A good oscilloscope provides a lot of insight into what is happening in a circuit. My favorite oscilloscopes are the analog scopes made by Tektronix. I own several Tektronix service manuals which contain complete schematics. Most of what I know about electronics comes from studying Tektronix schematics and trying to understand exactly what the designers did and why they did it.

Many Tek manuals can be downloaded for free from various websites including BAMA. However, I recently was fixing a Tek 464 and could not find the schematic online. Eventually I found it. Here's my copy: Tektronix 464 Service Manual I would like to point out, however, that there is a DC voltage annotation on the high voltage power supply schematic seems questionable. On the left side of page 267, the voltage on C1455 is marked as 0.4 volts, but it seems unlikely to be correct. I recommend ignoring that annotation.

Here is a nice circuit that is used for overload protection at the input of the Tek 7A29 vertical plugin.

This is a 50-ohm input section with DC-1GHz frequency range. The four diodes at the front limit the current that can flow in or out of the amplifier. Since the current sources are set to 17.4ma and the input impedance is about 50 ohms (terminated), the base voltage of the input transistor is prevented from swinging beyond +/- 870mV. The circuit is very simple, yet it does exactly what is called for. It has very low resistance when it is not being overloaded, but becomes an open circuit when the input is too high. The diodes can be small since they will never have much current passing through them. Therefore they do not introduce a lot of parasitic capacitance to ground in normal operation. The circuit behaves a lot like a fuse, but a magic fuse that automatically recovers after the big input is removed.

Tek 7704 power supply
Tek 7704 right side

It is nice to be able to see a waveform in the time and frequency domains together.
I used to work at a chip company and I was spoiled by using an HP 4566B spectrum analyzer. The 7L12 spectrum analyzer plugin for the Tektronix 7000 series is a toy compared to the HP 4566B, but it is still quite useful, particularly when playing with oscillators.

I have a Tektronix 661 scope. The manual for the mainframe is on BAMA. The manuals for the plugins are on Tek Wiki


Oct 25, 2007: I got a Tektronix 7D20 digitizer plugin. It doesn't work. It has at least one problem. The self-test gives "FAIL 41" on power up. (Huge thanks to all of the people who have contributed to BAMA, Shannon Hill in the case of the 7D20.) According to the service manual, that means "BAD EAROM". From what I can tell, the EAROM is something like what we currently call an EEPROM. It seems like the purpose of the EAROM is to make settings persist across power cycling. It seems like there might be an additional problem. The display is shifted down by about half of a screen. Furthermore, everything is smeared vertically, so a dot appears as a 4mm vertical bar. Horizontally there is no such spreading. The 7D20 uses the host mainframe as an X-Y display. Here is a summary of the architecture:
analog_input -> analog_shift_register -> CPU -> DACs -> X-Y_display
The X and Y signals that are sent to the mainframe are generated by MC3410F DACs, one for X, one for Y. Although they are 10-bit DACs, only 8 bits are used. The unused inputs are grounded. Since the vertical spreading affects everything on the screen, not just the signal trace, I feel that it is pretty safe to assume that the problem is somewhere between the microprocessor and the connector that interfaces with the Y input of the mainframe. I have confirmed that my 7000-series mainframe performs flawlessly with other 7000-series plugins. The Y output circuitry and X output circuitry are very similar. Hopefully the chips are in sockets in those sections. I'd like to swap the horizontal and vertical DACs to see whether the smearing becomes horizontal. Otherwise, maybe it is a bad opamp. Also, I think I'll look at the output of the opamps in the vertical output circuit to see if they are oscillating. They are 5532 opamps, which are compensated, so it shouldn't have too much of a tendency to oscillate. But, of course, there are all sorts of ways to make a compensated opamp oscillate. Also, the MC3410F's are multiplying DACs, which is used to scale the output to match the sensitivity of the mainframe. If there is garbage at the reference inputs of the DAC, that will also corrupt the output. I'll check that. Also, there is a phase splitter that generates the differential low-impedance signal for the mainframe. Maybe the second amp in the phase splitter is bad. That would wreck the symmetry. We'll see. I made some 7D20 repair notes since the manual isn't hypertext. More later...

Oct 28, 2007: The problem with the 7D20 is confusing me. It exhibits the same symptom in my 7704 mainframe and in my 7603 mainframe, with the screen being shifted down and compressed and fuzzy. But once in a while (about 1 out of 10 times), when I turn the scope on, the image is perfect and the 7D20 works perfectly, except for the bad EAROM, which doesn't affect normal use. It will continue working perfectly until I turn the scope off. Turning the scope off for a second and then back on puts it in the non-working state. Bumping the machine when it is in the working state will not put it into the non-working state. Bumping the machine when it is in the non-working state will not put it into the working state. Since the signals that are being corrupted are the X-Y voltages that are used to paint the display with trace and on-screen text, I used another scope in X-Y mode to monitor the X and Y voltages in the 7D20 as they go from the X and Y DACs toward the scope mainframe. When the scope is in the corrupted, non-working state, the other scope still shows a nice clear image on its screen. Only the 7D20's host mainframe shows the corrupted image. As I moved the probe points closer and closer to the mainframe connector, I found that the probed signal remained good. Now here is the crazy part. When I probe the signal in the mainframe, where the plugin connector meets the scope's interface board, the signal still looks good! This is really hard to understand how this can be. I confirmed that the vertical signals (A11 and B11) are operating in proper differential mode. v(A11) + v(B11) = approximately zero. v(A11) - v(B11) = 2 * v(A11). So it looks like a good signal is being fed to the scope but the scope is displaying a distorted image. We could easily infer that the mainframe is not working. However, the 7D20 does the same thing in two different mainframes. And both of those mainframes work correctly with other plugins that go into the same connectors.

A guy on the TekScopes mailing list told me how to get rid of the EAROM problem. One just needs to store anything to each of the memory locations and then the contents will be valid and no error will be reported.


I was given a non-working Tek 130 L/C Meter a couple of years ago and never got around to fixing it until today. I have been building oscillators and I wanted to measure the capacitors and inductors in my junk drawer to find stuff I can use. The problem with the Tek 130 was the power supply capacitor. It was exhibiting low capacitance and/or high ESR. There was about 80 volts rms AC on high voltage rail and 6 or 7 volts rms AC on the regulated 150-volt rail. I temporarily shunted the power supply cap with an off-board 47uF 500-volt electrolytic. The instrument suddenly became usable. Actually it is pretty accurate. It is an elegant instrument. As I was appreciating the meter's schematic and thinking about the sensitive heterodyning, I realized that I could make a Tek 130 Theremin. Update: I replaced the capacitor properly. After removing the old metal can capacitor, I removed the bottom flange from it. Then I epoxied the new 47uF 500-volt capacitor to the flange. Minor nibbling of the flange was required to get proper clearance for the pins of the new cap. The result can be seen here.
Jan 2008: Recently I repaired a 180A time mark generator. The output pulse rate was unstable. The 5ms output would jump from 5ms between pulses to 6ms, and sometimes to 4ms. I suspected a bad/noisy tube. Swapping all three tubes in the 5ms divider with known good tubes failed to improve the output. So I suspected the timing capacitor, the one that cross-couples the two triodes of the multivibrator. The capacitor turned out to have drifted upward and had also become extremely temperature-sensitive. I replaced it with two cheap little metal film capacitors in parallel. This completely fixed the problem. I would like to use a good capacitor but my good caps (polypropylene, for example) cannot take the voltage in this circuit. Anyway, the circuit is designed to work correctly as long as the time constant (charging rate) stays within about +/- 20% from the value during calibration. This is the nice part of making a pulse frequency divider out of many cascaded sections of low division ratio. The 180A is a very nice piece of equipment. If I were designing it (if I had been born), I would have made it an option to have a built-in receiver for injection locking the oscillator to WWV. It wouldn't need to be a full radio. It doesn't need to demodulate and it doesn't need to be tunable. Hey, this might be fun to build...
February 17th, 2008: I got a TM504 containing, among other things, a PS503A. It wasn't working. The 4500uF filter capacitor for the positive rail (C10) had failed, becoming a high impedance to AC. (Was it a high real impedance or a high imaginary impedance? Who cares?) After replacing that, the symptoms changed. The positive variable supply would work at low voltages but would shut off when the voltage was raised. Also, when it would go into current limiting mode, it would never come out, even when the load was removed. The load I was using was a 300-ohm power resistor. Interestingly, at moderate voltages (5 to 10 volts), disconnecting the load would cause the positive supply to shut off. This indicated stability problems. The crowbar SCR (Q65) was triggering. I suspected that 4.7uF capacitor (C64) that filters the gate line for SCR was bad, and that inductive kick was triggering the SCR, so I checked the cap, but it was exactly 4.7uF. I grounded the gate of the SCR so it wouldn't trigger (The crowbar circuit is mainly to protect the load.), and observed that the output voltage was oscillating from rail to rail at about 200KHz with some ugly sawtooth-like waveform. I suspected the 50uF output capacitor (C60), since it is supposed to serve some kind of compensation role. Indeed, C60 was bad, a high impedance to AC. So I replaced it and re-enabled the crowbar circuit, and the power supply works perfectly now. The failure of C60 left the power supply in a marginally stable state. When it would ring or oscillate, the crowbar would trigger, and then the power supply would cut off. Clearly I should also replace the capacitors in the negative half of the PS503A, since the circuit is just a mirror image of the positive half. Capacitors are remarkably problematic components, particularly as they age.
Feb 20, 2008: I recently bought a Tektronix 519. I wanted one for years. There were two if them at my undergrad college in the storage room on their way to the trash. I asked their owner (a professor) to please notify me before throwing them away. He threw them away without notifying me: two Tektronix 519 oscilloscopes in fine condition with carts. I had a sinking feeling when I heard about it.

Anyway, I bought a 519 from a nice guy in St. Louis. Before he sold it, he powered it up and posted pictures of it working. When I got it, I fired it up on a variac. It worked for a couple of minutes and then the high-voltage supply died. I am in the process of troubleshooting it. It is full of black beauty capacitors which are, of course, prime suspects. The transformer looks good, but it's hard to tell. The power oscillator isn't oscillating. It seems unlikely to me that problems on the secondary side of the transformer would cause it to stop oscillating. My guess at the moment is that the cause of the problem is the failure of one of the capacitors in the oscillator. I checked them for small-signal capacitance and low-voltage leakage and they are all fine, except for the expected horrendous drift in capacitance, upwards usually. Still, there are many ways that a capacitor can be bad, while still having the correct capacitance and low DC leakage.

Feb 22, 2008: OK, I got the 519 to work. I replaced all of the black beauty capacitors in the HV power oscillator and it still wasn't oscillating. Finally, even though the 6AU5 tube in the oscillator had a working filament and had reasonable plate current, I decided to steal a 6AU5 from my 545B and try swapping it. Yes! The original 6AU5 was bad. After swapping it, the HV power supply came to life, the neon bulbs lit, and there was a nice trace on the screen. However, the trace didn't respond to the input signal. How could it be? There is no vertical amplifier to go bad. Eventually I determined that my BNC-to-GR adapter was getting a bad connection with the GR plug in the front panel of the 519. When I fed the signal to the center pin of the input connector, it worked. As I looked at the input connector, I noticed that it looks different... Knowledgeable people informed me that there are 125-ohm GR connectors and the 519 uses them, not the standard 50-ohm GR connectors. I had no idea. It makes sense, though. A 50-ohm connector in a 125-ohm system would be a very bad idea. It is great news that the 519 works now. The only thing to do now is to figure out why the triggering is a bit jittery. It does trigger, but there is about 1mm of jitter.

May 16, 2008 I ran across a Nelson-Ross 002 spectrum analyzer plugin for 500-series scopes. Here are some pictures: front, bottom, bottom. I put it in my 547 and fired it up and it does not appear to work. I have used various other spectrum analyzers, so I don't think that the problem is merely my own stupidity. Among other things, it does not generate a sweep signal. It has a wire coming out of the front panel that ends in a banana plug that seems like it should go to the external horizontal input so the spectrum analyzer can use the scope in X-Y mode. I probed that signal with another scope and saw nothing. I'm guessing that there is a ramp generator inside the plugin and that ramp drives a VCO. I'm guessing that the ramp generator is not working. Unfortunately the manual is not on BAMA. Most likely I'll either have to trace the wires and make my own schematic or buy the manual.

May 18, 2008 The same guy who sold me the Nelson-Ross 002 also sold me a Tektronix 555. I was hesitant to power it up because I feared that the electrolytic capacitors would be shorted from years of not being turned on. I used a 0-500V bench power supply to test each of the large electrolytics. This is not nearly a complete test. I just verified that each capacitor could be maintained at the normal operating voltage without any significant DC current. All capacitors were fine. I tried to power up the power supply without it being connected to the scope. That doesn't work. After I plugged in into the scope and powered it up, I was pleased to see that the 555 was in pretty good shape. The lower beam wouldn't do anything, which I traced to a bad black beauty capacitor in its high voltage supply. I replaced it with a 1kV ceramic capacitor from my junk drawer. The lower beam works now. But I smell something hot after the scope runs for a couple of minutes. Each time I smell it, I power down immediately. I will do a high voltage test on all of the capacitors in the lower beam HV supply, including the ceramic cap that I put in there. My current hypothesis is that some capacitor is passing DC and the smell is either coming from the heat dissipated in the capacitor or the heat dissipated in some series-connected resistor that is not designed to have standing current flowing through it. The post-deflection accelerating voltage in a 555 is generated by the lower-beam supply. So the brightness of the upper beam really suffers without this supply working. Interestingly, you can still sort of use the top beam without the lower-beam supply working. It's just dim. Removing V900 (a 6CZ5 beam power tube forming a power oscillator) effectively shuts down the lower-beam supply and the scope runs without the burning smell.

May 19, 2008 The lower beam HV problem remains, but in the meantime, I noticed 2.7 volts of ripple on the 500 volt supply. The problem is that C760, a dual 40uF capacitor, has lost most of its capacitance. I left the capacitor in place, but electrically disconnected it, and mounted two 50uF electrolytics on a little piece of plexiglass using hot glue and screwed the plexiglass to the chassis of the 555 power supply using an existing screw. Now the ripple is below 3mV. There was time-domain blur before and now it is gone. I can't remember if the blur got worse from left to right across the screen. Maybe the ripple on the 500 volt supply was affecting the triggering somehow, which would cause uniform blur across the screen, or maybe it was affecting the Miller runup circuit, which would cause increasing blur from left to right. The ripple was full-wave rectified 60Hz power line. It is interesting to think about the manifestation of a "modulating" signal on the sweep rate.

By the way, I have a Tek 155-0147-02 chip from a 1470 NTSC generator. If anybody needs it, it's yours for the cost of shipping, or zero if you're in NYC.

May 20, 2008 I played with the 555 for a little while this morning. The lower-beam supply acts strange. For one thing, the HV pot has no effect on the cathode voltage. The upper-beam supply behaves normally. However, the lower-beam cathode voltage is in the right neighborhood, around -1380V. And the post-deflection acceleration voltage is around +6000V, which seems reasonable. But there's no lower-beam trace. I verified that the lower-beam filament is good, and I swapped the horizontal plugins. My guess is that there is a problem with blanking. The burning smell has decreased or even stopped. Maybe something in the blanking circuitry was burning and has finally burnt out. Of course there could be a fault in the elaborate distributed vertical or horizontal amplifiers, but if that were the case, I'd expect to see some vague patterns on the screen, not just darkness. So my current hypothesis is that the grid-to-cathode voltage is holding back the electrons. This will be verified with my multimeter, floated to the cathode voltage. This is one reason why I prefer my battery-powered multimeter to my bench multimeter.

May 21, 2008: The 555 HV supply is better now, but still not proper. The HV ADJ control still doesn't have any effect. But at least both beams are working now. It's a bit hard to believe, but it seems that V962, the 5642 high-voltage rectifier tube for the lower-beam cathode failed during the few days that I've had the scope. It must be caused by me but I don't see how. My guess is that C931, C943, C944, or C948 was intermittently passing a bunch of DC current, and this was overloading the little tube. The filament glows and it doesn't look gassy, but it fails to rectify. I borrowed a 5642 from another working scope (I dislike doing this.) and installed it in place of the bad V962, and the cathode voltage came back. But I don't want to kill this good 5642 tube. I will figure out a safe way to continue debugging without endangering the rectifier.

By the way, note what happens if V962, V914, or any of the associated circuitry is not working. The HV supply will be out of regulation and will run at full-throttle.

I replaced some more bad components and got things closer to how they should be. Still, the CRT cathode voltage is a bit weak. Here are some notes about the feedback that controls the HV supply.

V914 is a 12AU7 dual triode used as a feedback amplifier for the HV supply. The grid of V914B is compared with the cathode of V914B, which is -150V. A voltage difference near zero will result in about 200uA of plate current, which will pull the grid of V914A down to about -14V, which will cause 3mA of plate current and will put the plate at +260V. This is the second grid voltage for V900, the 6CZ5 power tube that forms the HV power oscillator with transformer T901. So, for the same reason that one makes the "virtual ground" assumption when analyzing op-amp circuits, the analysis (and troubleshooting) of the 555 HV supply can start at the grid of V914B. If the system is operating in the proper closed-loop mode, we expect to see -150V on the grid of V914B. This is a fork in the road. If there isn't a constant -150 volts on the grid of V914B, we have to ask whether the HV oscillator is oscillating at all, or trying to start. Relevant issues will be whether the HV transformer is good, whether the oscillator tube is good, whether the tube is getting the right DC voltages to start oscillating, and whether there are bad passive components, particularly capacitors in the circuit. In the case of the HV supply of my 555, the grid of V914B is a constant -150 volts. So the question is why CRT voltage is wrong while the feedback system is in a steady state equilibrium. The design of the HV supply uses something like a 9:1 voltage divider on the CRT cathode voltage to get the grid voltage for V914B. If the resistances in the divider drift, the divider might be 10:1 or 8:1, and one would expect to see 10*(-150V) or 8*(-150V) on the CRT cathode.

Indeed, drift in the resistors in the voltage divider was responsible for the error. R950, an 820K resistor, had drifted to 920K. I replaced this, but it didn't completely fix the problem. R952, a 1Meg pot, had drifted to 1.26Meg. I shunted the pot with a 5Meg resistance to correct this. R956, a 2Meg pot, had drifted to 2.5Meg. I shunted it with 10Meg to correct it. The result of this sort of shunting is not quite the same as if the pot were correct, but if the wiper current is very low, the difference will be small. After making these three changes, the HV ADJ control works correctly and I set the CRT cathode to -1350 volts, as it should be.

May 22, 2008: I traded a DEC PDP11/23 for a non-working Tektronix 310A. The 310A would blow the fuse at power-up. I suspected shorted filter capacitors in the power supply, but this was not the problem. The problem was a bad 6AQ5 tube in the HV power supply. I happened to have a 6005 in a box of old tubes, and it works well in place of the 6AQ5. The CRT cathode voltage is correct now, without any adjustment necessary. Now the 310A works perfectly except for the calibrator which puts out a low-amplitude, high-frequency waveform instead of a low-frequency square wave.

June 1, 2008: I fixed the calibrator in the 310A. It was a bad tube. The circuit calls for a 12AU7 and the closest I had was a 12AT7. It works fine.

June 2, 2008: I never was able to get my Tektronix 661 sampling scope to work. (Update: It works.) Recently, I bought another 661, not working and missing its timing plug-in. My hope is that from the two non-working 661's, a single working 661 can be built. Just today, I put the new 661 on my bench to take a look. It is certainly dirty. So far, I have confirmed that the main power supply works correctly, the cathode voltage is good (no PDA), and the CRT works. There appears to be a problem with triggering, timing, and/or blanking. The screen is completely dark in what should be normal operation.
June 3, 2008: I got the "new" 661 to work. There was a bad tube in the 4S1 sampling plug-in. Debugging the 4S1 is not easy, but fortunately nothing was wrong with any of the exotic components. Here are some photos of the 4S1 schematics. I feel that the best way to debug the 4S1 is to leave it in the 661 and lay the 661 on its side with the bottom cover removed. That way you can easily probe the inputs and outputs of each module on the 4S1's interconnection network. The manual provides examples of what the signals are supposed to look like. I have a 5T1A and a 5T3. The 5T3 works only at high sweep rates. The 5T1A doesn't work at all. I'm glad I have a working configuration to start from. Next I'd like to get the 5T1A working. I'm not intimidated by a half-dozen tunnel diodes.

June 4, 2008: The Tektronix 661 is really a nice machine. It appears to have been designed in 1961. The scope takes two plug-ins, one for the time base ("timing") and the other for the vertical inputs ("sampling"). It is a high speed sampling scope, so it is somewhat more complex than the average scope. The external styling and internal construction resemble the 500-series scopes like the 545 and 547. The mainframe provides regulated DC voltages to the plug-ins, and provides them with a low-speed X-Y display. Unlike most Tek scopes, there is nothing tricky about the CRT. Basically the scope works as follows. The signal comes into the sampling plug-in. There is a trigger pick-off that sends some of the input signal to the timing plug-in through a coaxial cable that is part of the mainframe. The timing plug-in has triggering circuitry and sends a signal back to the sampling plug-in, telling it when to sample. The sampling plug-in does some signal conditioning to the output of the sampler and sends this to the Y amp of the display. The timing plug-in sends a slow ramp signal to the X amp of the display.

The mainframe is actually quite a bit simpler than a 545 or 547. Failures, therefore, tend to be in the plug-ins. Tek made extensive use of fancy diodes to do the high-speed work. These fancy diodes seem to be the most common cause of a 661 not working. At first, it seems like the sampling plug-in and the timing plug-in are in a very intimate embrace, and it seems like it would be hard to determine which one is at fault. However, this is not the case. As I mentioned before, probing the sampling plug-in from the bottom gives you access to many of its internal signals while it is running. It is possible to probe most of the timing plug-in's signals by removing the side cover of the 661. So, for example you can determine whether the sampling plug-in is sending the timing plug-in a signal. If it is, you can check whether the output tunnel diode in the timing plug-in is firing. If not, you have restricted the problem to the front end of the timing plug-in. If so, you can check the signal that the timing plug-in is sending back to the sampling plug-in.

A common cause of failures of sampling plug-ins is the sampling diodes. They are small and have low capacitance, so they are vulnerable to overload and ESD. Their forward voltage should be around 400mV. Blown diodes may show higher voltage on a diode tester. Also, there are Nuvistors in the sampling plug-in. Nuvistors sometimes fail. Fortunately, many of the components can be swapped back and forth. So if you have one working channel, you can swap parts to figure out what's wrong with the second channel. Keeping notes is recommended. If all of your sampling diodes are dead, don't worry, there are modern replacements. Dead tunnel diodes are a more serious problem.

June 12th, 2008: I ordered some HP Schottky diodes to replace the blown GaAs sampling diodes in my 4S1 and other blown samplers that I have. They come in pairs, and HP says that each pair is well matched. I am a bit unclear on the matching criteria for sampling bridges. It is clear that the left half and right half should be matched, but it isn't obvious to me why top-to-bottom matching is required.

I scanned some manuals. They are on my manuals page.

June 17, 2008: The Schottky diodes for the 4S1/661 haven't come yet, so I've been playing with other things. I've been trying to get my HP-85 computer to communicate with my Tektronix 7912AD via GPIB. Let's see, I'm not sure whether the 7912AD's GPIB works. I'm also not sure whether the HP-85's GPIB works. And I don't know anything about GPIB. I am able to get the 7912AD to switch back and forth from local to remote mode via GPIB, but when I try to read data from it, nothing happens, and my I/O procedure times out. The HP-85 works by itself, and the 7912AD works in TV mode. Most likely the problems is that I don't know anything about GPIB.

June 28, 2008: I am fortunate enough to own a Tektronix 519. Here is a photo of the delay line in my Tektronix 519. For the purpose of comparison, here is a photo of an automobile supercharger.

Oct 24, 2008: I've been using my 547 lately as my main bench scope. From the time I bought it until today, it had a blanking problem with the A timebase. The cause of the problem was a bad PNP germanium transistor, a 2N2207. I replaced it with a 2N3906 and it works fine now. Other than that, my 547 is in pretty good shape. One of the triggers is a bit fussy. I'll see what I can do about that.

Oct 26, 2008: I calibrated the triggers and sweeps and my 547 is really working well now. The cause of the fussy trigger was actually a dirty switch. I used contact cleaner on all of the switches and worked them back and forth. After that, the trigger adjustments helped a bit more. Finally, I used my time mark generator to calibrate the sweeps. They were running a bit fast on some sweep rates.

Dec 6, 2008: I started a wiki for classic Tektronix equipment.

Oct 8, 2009: Today, I fixed a Telequipment D54. The scope was making arcing noises and the brightness control wasn't doing anything. The 100V zener diode in the CRT cathode supply was shorted. I replaced it and the scope works. The construction of the D54 is not friendly to a person making repairs. Removing the PCB requires removing controls from the front panel. An alternative is to cut the wires of the old component and to solder the new component to the stubs that remain. The D54 uses an unregulated power supply. They play some games with voltage-controlled amplifiers to keep the gain stable across supply voltage variations. It doesn't really work. When I play with my variac, I see significant changes on the screen. That doesn't happen with, for example, my 547.

Oct 9, 2009: Due to lack of participation, I consider my Tektronix wiki a failure. I will move back to a non-wiki webpage.
Update (April 2010): Things have gotten more active on the Tektronix Wiki so I will continue to post to that.

Jan 27, 2010: Recently I have been fixing up a Tektronix 567. The original electrolytic capacitors in the power supply failed due to excessive ESR. I replaced them with new capacitors. This affected the low voltage supplies the most. Some ripple in the pre-regulator capacitors is normal. The regulators handle this variation at their input without allowing it to affect the output voltage. But there is a limit, and certainly if the voltage at the input of the regulator dips down to (or below) the assigned output voltage, there is nothing the regulator can do. That is what was happening in the 567 before I replaced the capacitors.

After replacing them, I could look at the finer details of the situation. I found one dead tunnel diode in the 3T77 sampling sweep. They symptom was that it would never really trigger on the input signal. Depending on the position of the trigger level control, it would either not generate trigger pulses or it would free-run. For debugging sampling scopes, I like to look at signals that pass back and forth between the plug-ins. And I like to start with an external trigger signal since it is simpler than internal triggering. The 567 is working well now except for one small problem with the 6R1A digital unit.

Feb 1, 2010: I bought a Tektronix 454A on Ebay. It was sold as not working. It arrived, indeed, not working. The main problem was that the A trigger was not triggering. It would free-run when in the AUTO mode, and not trigger when in the NORMAL mode. I found abnormal DC voltages on the terminals of Q623, which is a JFET source-follower at the input of the trigger circuit. Current was leaking out from the gate of the JFET, a bad sign. I removed Q823 (a similar JFET) from the B trigger board and inserted it in the Q623 socket. It worked. With Q823 missing, the scope still works, including the B sweep. Q823 is only needed for the "triggerable after delay" mode, not the "sweep after delay" mode. I will find a JFET to replace Q823. Q623 is in a vulnerable position. When the trigger input is set to EXT, if a big pulse (e.g., electrostatic discharge) is applied to the external trigger input, it goes more or less directly into Q623, killing it.

Another problem with my 454A was that the horizontal position knob was pushed in, cracking the knob and breaking open the potentiometer. To fix this I had to remove the structural aluminum piece on the side of the scope. The rear panel of the scope must be loose to remove the structural piece. I was able to push the potentiometer back together and bend its metal retaining tabs back in place. It works fine now.

Feb 1, 2010 (continued): I replaced Q823 with a 2N3819 FET. It works well. The pinout of the 2N3819 is different from the pinout of the original 2N4416. After changing the transistors, I recalibrated the DC levels of the triggers and checked them for stability at low input levels.

Feb 3, 2010: Nose-to-nose measurements are common for high-speed sampling scopes. Today I wanted to measure the risetime of 454A that I recently got, which is specified to be about 2.4ns. Lacking a subnanosecond risetime pulse generator, the first thought that came to mind was to use the kickout pulse from one of my sampling scopes. The 567 was convenient, so I connected the output of the 3S1 sampling vertical plug-in to the input of the 454A. I drove the 3T77A sampling sweep horizontal plug-in with an external trigger signal from my HP pulse generator (7ns minimum risetime). The sampling pulses were visible on the 454A, but I was disappointed by how low in amplitude they were. They had a more or less gaussian shape, with a 10% to 90% time of about 2ns. Later, I thought about it and it makes perfect sense. The tall skinny sampling kickout pulses become lower and wider due to the bandwidth limitation of the 454A. This is, in fact, exactly what one should expect. And the 454A is behaving as it should.

Feb 4, 2010: I found that the amplitude of the kickout pulse from the 3S1 sampler is strongly dependent on the mV/div setting on the 3S1. By choosing a setting that gives a strong kickout pulse, I was able to get a better trace of the impulse response of the 454A. This photo was taken with the 454A set to 2ns/div (0.02us/div and 10x horizontal magnification).


June 4, 2010: I bought a 564. It had a problem with HV arcing (photo 1, photo 2) The scope was very dirty when I got it. It was arcing from one position in the porcelain strip to a the silver cup of the adjacent position, and then to the next position to complete the path. Corrosion or etching of the porcelain strip can be seen in the photos. One end of the arc path is the junction of a resistor with a wire. I lifted that junction off the porcelain strip and the arcing stopped. I tried to clean the porcelain strip but it is permanently discolored from the arcing and I don't trust it not to leak current at high voltage. For now, it seems fine to let the junction float. It is mechanically stable because of the stiffness of the resistor and the wire with which it joins.

It is an interesting 564. It has been modified with the addition of a module labeled "MODIFIED FOR SPECIAL LINC DATA TERMINAL BOX". It has four relays added. These relays are in sockets. The relays are controlled by signals brought in through an added connector on the rear panel of the 564. The relays appear to provide remote control of the storage circuit.

June 5, 2010: A few weeks ago, I found an early 535 being discarded. It is the type with the chassis that slides out from the case, which is brown. Before powering up the scope, I did a few things. First, the scope was filthy so I washed the entire scope with warm water from a hose. After letting it dry for two weeks, I remounted the fan, which was originally mounted on rubber anti-vibration blocks, which predictably had become brittle and disintegrated. Next, there was a HV rectifier tube that had a broken plate lead. Based on the appearance of the inside suface of the metal box that encloses the HV circuit, it seems like the plate had been arcing for a while before it eventually weakened the wire enough for it to break. I would guess that this is the failure that ended the scope's previous phase of service. I reconstructed the plate wire by soldering a thin wire to the 1mm stub remaining of the 5642's plate wire. Next problem, there were arcs forming between two of the secondary leads on the HV transformer, T801 and the core of the transformer. These cracks in the insulation/potting can be seen in this photo. The blue lines drawn on this photo show the path of the arcing. I cleaned the area of the arcing with contact cleaner and a toothbrush and then dripped hot candle wax on the area. This completely stopped the arcing.

The -150V supply was quite far off, -142. I adjusted it to -150. If the scope was calibrated while the supply was wrong, then setting it to the correct voltage will mess everything up. But I doubt that anybody would calibrate a scope without checking the -150 supply. A couple of volts off is not a problem, but 8 volts is too much. After that, I checked the other supplies. The +225V supply was +195V. It it was in regulation, and not noisy, just the DC voltage was wrong. Here is the schematic of the +225V section of the power supply circuit, annotated with what I think was happening. R772 and R771 are not too far from their specified resistance values. The 12AX7 has normal emission and no grid shorts. The problem was DC leakage through C770. Let I_leak refer to the DC leakage current through C770. By my calculations the output voltage of the +225V section of the 535 power supply is 225 - 5.8*10^6 * I_leak. So the the output voltage drops by 5.8 volts for every microampere of I_leak. Based on this, it seems like C770 (an original bumblebee capacitor) in my 535 was leaking 5.17uA with 195V across it. I replaced C770 with a good capacitor of the same ratings and now the output voltage of the +225V power supply measures +227V, close enough. The reason it is 227 and not 225 is that R772, a 333K 1% resistor, has drifted up a bit. I will measure the DC leakage of the original C770 on a voltage source set to 195V.

Update, June 5, 2010: I measured the leakage of the original C770. It leaks 1.5uA with 195V across it. Although 1.5uA is a totally unacceptable amount of leakage for a 0.01uF capacitor, I was expecting more like 5uA. I have no explanation for the discrepancy at the moment. In any case, C770 is clearly bad.

June 6, 2010: I found that the leakage current through the bumblebee C770 of the 535 is extremely temperature sensitive. At 195V, the leakage varies from 1.5uA at cool room temperature to 20uA when warmed so the body of the capacitor is warm to the touch. I tested a 0.047uF 600V Orange Drop (polypropylene film) capacitor at 195V. The leakage is 100nA cool, 200nA warm. Normalizing for the difference in capacitance, at room temperature the bumblebee's leakage is 70x worse than the Orange Drop's. Warm, this becomes 465x.

The 535 works now. All supply rails meet their voltage and ripple specs. I was seeing some strange erratic nonlinearity in the sweep, but it went away after I used the scope for a while. I think it was a dirty contact in one of the switches, most likely the horizontal mode switch. The triggers for both sweeps work, but are very tempermental, only triggering correctly in a narrow range of stability settings.

July 10, 2010: I bought a 230 Digital Unit. It was not working at all. All of the DC voltages at the test points on the regulator board were close to 0V. One of the low voltage electrolytics has failed (high ESR). I connected another capacitor in parallel with the failed capacitor using clip leads. That fixed the ripple on the post-rectifier capacitor, but the outputs of all of the regulated voltages were still all dead. There are interdependencies between the regulator subcircuits. For example the -50V output is used by the error amplifier for the +50V regulator. And the +50V output is used by the -50V regulator.

There is a 1-ohm sense resistor used by the +50V regulator for overcurrent protection. This resistor had failed, open-circuit. I replaced it and then the whole power supply came to life, pretty close to the specified voltages for all outputs, and less than 2mVrms ripple on all of them. But the 230 is still not working in other ways. Some Nixies don't light up at all and others have multiple digits lit apparently simultaneously. None of the three limit lights illuminates.

August 7, 2011: I collect old Tektronix instruments not because they are useful to me. I collect them because they are interesting, inspiring, beautiful, and challenging to understand completely. I collect them to preserve the instruments and their heritage. It isn't about utility. A lot of people, including Stan Griffiths in his authoritative book, Oscilloscopes: Selecting and Restoring a Classic, discuss classic oscilloscopes as though their value derives solely from their utility. The scopes I find most intriguing and cherish the most in my collection are not the most practical and useful ones. Amazing engineering has to do with what the engineer does with what is available at a given time, on a given budget. Tektronix scopes are examples of amazing engineering because of what they did given the constraints of the day.

August 20, 2011: Recently, I bought a Tektronix 106 square wave generator. The 106 uses diode clipping circuits to make a 500mV square wave with rated risetime under 1ns. I powered it up and checked its output on the first scope I could find, which happened to be my Tek 2235, a 100MHz portable scope (3.5ns specified risetime. The observed risetime of the Tek 106 was about 3.5ns. I assumed that the actual risetime of the 2235 is somewhat less than 3.5ns, and the 106 is contributing just a little to the observed risetime. To get more detail, I fired up my Tektronix 567 with a 3S2 with S-4 samplers and a 3T77A timing unit. It was not easy to view the rising edge of the pulse. A common technique is to trigger on one cycle and view the leading edge of the next cycle. This works well if the period-to-risetime ratio is small (e.g., 20). Otherwise there is a jitter problem. Unfortunately, the maximum repetition frequency of the Tek 106 is 1MHz. So the period-to-risetime ratio is around 1000. The solution is either to use a pretrigger or a random sampling timing plug-in. I replaced the 3T77A with my 3T2 random sampling plug-in. Random sampling is great for viewing the leading edge of low repetition rate signals like the 1MHz output of the 106. With the 3T2 I was able to view the leading edge easily. The Tek 106 with 1m of RG/58 seems to be about 650ps risetime. The cable and connectors probably has a risetime of around 100ps. Backcalculating the 2235's risetime, we get 3.44ns.

August 25, 2011: I bought a Type 181 Time Mark Generator on Ebay. 8 out of 20 of the tubes were bad, mostly gassy. That is too high of a percentage to be attributed to natural failure. I should start a list of the parts I need for my various Tek restoration projects.

Oct 8, 2011: When a Tek 284 isn't working, one might wonder whether the tunnel diode is dead. One way of testing the tunnel diode is to open the airline, remove the tunnel diode, and perform direct testing on it, (e.g., measuring the I-V curve). This is very risky because the tunnel diode is delicate and new ones haven't been available for many years. Minimizing the risk is a good idea. Furthermore, measuring the tunnel diode in isolation still doesn't tell you whether the parts inside the airline are getting a good electrical connection.

For a 284 that doesn't make its high-speed pulse, the tunnel diode should in fact be the last thing that is checked. First check the 50kHz oscillator on the "PULSE GENERATOR" schematic page (p.103), and work your way across. On my 284, the waveforms very closely match the example waveforms on the schematic. My 284 came from Ebay, having been sold as "Square-wave and sine-wave outputs test good. No further testing done." It arrived promptly, well packed, and indeed, the sine and square wave outputs worked. The pulse output did not work. The setup I used for checking to connect to trigger pulse output of the 284 to the external 50-ohm trigger input of my Tek 3T2, and the pulse output of the 284 to the input of my Tek 3S2 with S-4 sampling heads. I could see that the 3T2 was triggering, but the trace was mostly flat. There was a small (50mV) pulse when the bias current turned on and off, but it was slow (20ns rise time) and badly formed. I probed the primary of T160, the input to the "TD tripper" and saw no signal. The switch and/or wiring associated with "lead time" switch SW158 had failed. I made an SMA-to-SMA jumper and used it to connect J158 to J160, bypassing the lead time switch. After that, the pulse tripper circuit worked, but the output pulse was unchanged, still weak and slow. I checked the waveforms at all inputs to the airline assembly: J181, J185, J186, and J184, and all seemed fine. I feared that the tunnel diode might be bad, but I wanted to exhaust all other options before opening the airline assembly. At that point I decided to leave it alone for a couple of days and come back to it fresh.

I measured the tunnel diode by connecting my multimeter in diode test mode between the center pin of J181 and the airline shell. In diode test mode, my Fluke multimeter applies about 500uA and observes the voltage. It read around 60mV, the exact value I can't remember. That was an encouraging sign, indicating that at least the tunnel diode wasn't blown open. Note that there is a 54 ohm resistor in series with the diode while this measurement is being made, but the resistor doesn't introduce much uncertainty since the multimeter drives a constant current. 500uA through 54 ohms results in 27mV voltage drop. So a reading of 60mV on the multimeter means that 500uA through the tunnel diode results in a 33mV voltage drop across the diode. This seems reasonable. A very rough approximation of the effective resistance of the tunnel diode in the region below Vp is Vp/Ip. For the diode in the 284, this is 65mV/21mA, about 3 ohms. 500uA through 3 ohms results in 1.5mV. This is quite different from the 33mV calculated above. I should go back and measure it again.

Measuring the forward voltage of the tunnel diode at low currents doesn't tell us what we really need to know. We need to know Ip. We also need to know the Ip:Iv ratio. If those two parameters are good, the diode is probably in good condition. I'm not aware of failure modes that degrade other aspects of the tunnel diode's performance without affecting either of those parameters. For example, I'm not aware of failure modes that cause the diode's capacitance to increase.

If the diode is good, we definitely don't want to damage it while measuring it, which can happen if the tunnel diode is treated like a regular diode. Tunnel diodes are notoriously sensitive to electrostatic discharge, high temperature, and excessive current. Furthermore, for minimizing package parasitics, the packages tend to be small and easy to misplace. The tunnel diode in the Tektronix 284 can be adequately tested without removing it from the airline. Connect a variable voltage source that can output between 0V and 1.5V at 30mA with fine control of the voltage and less than 5mVpp of noise. I have a Power Designs model 2010 power supply that is good for this sort of thing. Power Designs power supplies are like Tektronix equipment: well designed, well documented, and well constructed. Whatever power supply you use, make sure it doesn't put out glitches when you change the voltage, because a major glitch could kill the diode we are trying to test.


To test the diode, disconnect all four SMB connectors from the airline assembly. Turn on the power supply and set it to 0V. If the power supply has a current limiting control, set it to about 40mA. Connect the positive lead of the power supply to the center pin of J181 on the 284. Connect the negative lead of the power supply to the airline housing (i.e., the ground of the airline). Put a high-impedance voltmeter between the center pin of J184 and the airline housing. The voltmeter measures the diode current, which is passes entirely through R184A. Since no current flows through R184B and R184C (high-impedance voltmeter), the voltage at the center pin of J184 is equal to the cathode voltage of D180. Raise the power supply voltage to 50mV. At this point, there should be about 50mV at J184, and we can infer a diode current of about 1mA. Raise the power supply voltage slowly while recording the power supply voltage and J184 voltage. If the diode is working as specified, the J184 voltage should get up to about 1V when the power supply is around 1.065V. Assuming that R184A is within tolerance, when you observe 1V on J184, there should be about 18mA flowing through the diode. When you increase the power supply to somewhere around 1.2V, the J184 voltage should suddenly decrease. Record the voltage. The downward step in J184 voltage should be at least 500mV. The diode is a short circuit, it there will be no downward step in voltage. If the diode is an open circuit, the J184 voltage will not follow the J181 voltage. If the diode works but has a shifted Ip, that will be shown as a shift in the maximum J184 voltage that can be seen before the downward step happens. If the Ip:Iv ratio is degraded, the size of the downward step will be reduced.

My 284 turned out to have dirty contacts in SW158, the "lead time" switch. After spraying some contact cleaner into the switch and working it back and forth, it was completely functionally restored. I readjusted the tunnel diode bias and bias balance and got a nice clean pulse with an displayed risetime 50ps, as observed using my Tektronix 567 with 3S2, S-4, and 3T2.


The risetime of the 284, can be approximately inferred from the displayed risetime and knowledge of the risetime of the S-4 sampling head, which is about 20ps. sqrt(50ps^ - 20ps^2) = 46ps. This is similar to the observations by Ralf Ohmberger on his excellent amplifier.cd page.

Oct 9, 2011: I recently got a 067-0596-00 Chopped Voltage Reference. It is a precision rectangular waveform generator. It uses a chopper to switch the output between two user-selected voltages. It was designed in 1968 or earlier. Mine was probably made in late 1981 and has serial number 000234, indicating that it was a low-volume product. It is an unusually elegant instrument. The word "chopped" in the name aligns with the fact that it contains a chopper. The layout of the front panel aligns with the layout of the circuit, which also aligns with the layout of the schematic, all of which align with the conceptual function of the instrument: to switch back and forth between two selectable voltages.

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