B-52 Bomber Astro Tracker - Part 2: Power up and gyro-stabilization

B-52 Bomber Astro Tracker - Part 2: Power up and gyro-stabilization

Show Video

Hello and welcome back. If you follow the channel,   you know that we opened up  a Kollsman Astrotracker,   with the welcome help from our friend Michel,  from the “Le Labo de Michel” YouTube channel. This astrotracker is but only one part of  the complex Kollsman MD-1 astrocompass,   that was flown on B-52 bombers. It was a Cold War era celestial navigation  system that used analog mechanical computers. In Part 1, I explained how  celestial navigation works,   by sighting the altitude and azimuth of the sun,  moon or stars, using a sextant, then doing some   complicated calculations to correct an approximate  assumed position into a precise true position.

The star tracker we have is an automated  sextant, which is able to sight, center,   and maintain lock on a star while the  bomber is flying, providing an automated   and continuous true heading to the navigation  system, and also a position error estimate. When we cracked it open in the last episode, we  were greeted by a complex arrangement of analog,   electro-mechanical components. The  regular viewers of the channel will   have noted the similarity to the Bendix air  data computer that we previously restored. The many cylindrical thingies that you see  all over the place, are synchros, motors,   generators, and control transformers. They  are the key electrical components of these   analog computers. We explained them in our  previous episodes on the Air Data Computer,  

link in the doodley-doo, and we’ll  come back to them in due time. But this astro-tracker goes one step further:  it adds optics to the mix. And sure enough,   the centerpiece of our freshly opened  astro-tracker is the optical telescope. [Marc] Ah, oui, c''est un prisme. It's  a prism. So, looks from the side here.   So the prism is probably all the way  down. It should be able to move up. Oh, okay. It does spin freely.

[Michel] Normally it's possible  to have a complete turn. [Marc] It's moving when I am  turning it. Do you see that? It's going up, and then it's going  down. Oh, that's interesting. Our astrotracker telescope does not look  like a telescope at all. Fortunately,   Kollsman patent 2,998,529 gives us  some insight into how it might work. The telescope optics are actually pointed  straight up, mostly hidden from view in the   middle of a cylinder. What we just saw was the  movable prism on top of the telescope optics,  

item 71 in the patent drawing.  This prism functions as a mirror,   forming a periscope which allows the telescope to  point to any part of the sky, looking through the   small curved transparent dome, which is the only  part of the system that peeks through the wing. The prism rotates around for azimuth sighting,  and tilts up and down for altitude sighting.   There are two motor-generators, called  MG in the drawing, for controlling the   prism position. Item 77 is the altitude  motor, and item 81 is the azimuth motor.

In addition, each motor is associated  with two Control Transformers,   marked CT in the drawing. These are  the position sensors. There is a x1 CT,   the coarse position sensor, and a x25 CT, the fine  position sensor with 25 times finer resolution. Via internal reflection, the prism directs the  light of the small patch of sky it’s pointing at   into the telescope optics. If our pointing  computer did its job correctly - remember,   that’s the one that Dave teared down on the  EEVblog - this small patch of sky should   contain the star that we want to track.  The star will not be perfectly centered,   but it should be close enough to  be in the narrow field of view.

The light from that patch of sky  is then focused onto detector 110,   which is a Photomultiplier tube, or PMT. PMTs are ultra-sensitive light detectors   that we also had previously encountered, in our  episode about the Eskalab spectrophotometer. You might remember, from that episode, that  the PMT is not an image sensor at all. It   is just a light level detector,  a very sensitive one at that,   but it provides no image information. By itself,  it cannot tell where the star is in the image. It can only measure the total  amount of light in the patch of sky,   just like it measured the total amount of  light going through our spectrometer sample.

Obviously, so more trickery  is needed to derive the star   position. That’s when the rotating  disks 106 and 107 come into play. We could spy both of them after we removed  the PMT. One disk has radial slots,   and is called the raster. The other one has a  round aperture and is called the shutter. They   rotate continuously at precise speeds. It’s going  to take a whole video to explain how this devilish   analog star position encoding scheme  works, but for now, just know it’s there,   and that it needs a motor M to rotate the  disks, and an associated position sensor P.

So this is what our star tracker really is,  if we ignore the many motors and sensors that   automate it. A fixed telescope with a movable  prism on top, a rotating shutter and raster   disks to encode the position of the star in the  field of view, a few filters for viewing the sun   or masking out auroras, and a photomultiplier.  And lots of motors and control transformers. The various motors and control transformers are  the cylindrical thingies that you see at the base   of the telescope, surrounding the PMT. So far,  we have identified 2 Motor Generators, 4 Control  

Transformers, one Motor and one Position sensor.  That should be 8 cylindrical thingies. But you can   count 10 of them here, so there are two more - a  sure hint that the actual implementation is more   complicated than what’s disclosed in the patent.  We’ll get to discover what they are in due time. But we are not quite done. There is additional  stuff at the bottom. We can see two more Motor  

Generators, and their associated Control  Transformers. It turns out that the entire   telescope platform is mounted on a two  axis gimbal mount. This is used to keep   the telescope platform level while the plane  is flying, using a gyroscope. This system will   keep the telescope perfectly vertical through  +/- 15 degrees of movement in pitch and roll. We already demonstrated the movement of the gimbal  platform in the previous episode. For that, we   first had to release the gimbal’s electro-magnetic  brake, and then move the platform manually so   we could access a hidden screw. You can spy  the gimbal motors and control transformers.

So we’re now talking about a grand total of  4 motor generators, 8 control transformers,   1 motor, 1 position sensor and 2 mysterious  extras. That’s 16 cylindrical thingies,   total. Each of them has many wires: a  control transformer has 4 coils and 5 wires. As we’ll see later, our motors are  more than simple AC servo motors,   they are motor-generator combos,  for a total of 4 coils and 8 wires. And there is a brake, a few solenoids, the PMT  control, and extra electrical stuff not talked   about in the patent. That’s a lot of wires,  none of which we know how it is hooked up. Undaunted, Michel got right to work  on reverse engineering the wiring. I soon learned that Michel is a reverse  engineering beast. He must be Master Ken’s  

forgotten French cousin. For days on end, he  would be in the lab from 7 am to midnight,   beeping connections tirelessly, which, by the  way, you can only do by piercing the wires,   as there is no other place to probe them.  He then carefully wrote his findings in   his notebook. After a few days of this, he  had reverse engineered the entire wiring. Thanks to Michel’s drawings,   we can start to make sense of what we see  at the back of the telescope platform.

There is the photomultiplier tube of course. The first cylinder is the shutter position sensor,   which is implemented with a  permanent magnet generator. Then we have the shutter synchronous motor,   which should be driven at 250 Hz to rotate  the shutter disks at a precise speed.

Then we have the prism altitude  angle coarse position sensor,   implemented by a control transformer. Here is our first mystery item. It  happens to be a potentiometer which   serves as another altitude angle sensor for  the star position detection electronics. Then comes the prism altitude motor generator.

Then the fine control transformer  for the prism altitude angle. It is followed by our second mystery  item, which this time is a resolver,   an animal that we have already encountered. This  time, it is coupled to the azimuth angle. We’ll   see later that it is used as a coordinate rotator  for the star position detection electronics. Then we have the coarse control  transformer for the prism azimuth angle,   the corresponding motor generator, and the  fine control transformer for that axis. There you go. This complicated  contraption is starting to make  

sense, assuming you are still with me. I think we are ready to start experimenting with   the star tracker. But before we do  that, we need to build a test stand. [Marc] All right, so let's try to put in  a mount, see if we can take it from there. So, we've made a couple of rails here.

I think that will... Oops, you are already hooked up. That will work. [Michel] Perfect! [Marc] There we go, we have it. So I can either  clamp it, or put some screws. I think clamp it. Then you can put your gyro at the bottom, power  supply, stuff like that. We can adjust the height. There you go. Test stand!

The first step is to get the gyro stabilization  working, so we can erect the telescope and   maintain it leveled. The gyro and the servo  electronics are normally contained in a small   cylinder next to the tracker. But we don’t have  that. So, instead, Michel brought his own vertical   reference gyro, and some AC servo amplifiers to  build the electronic servo control loop ourselves. [Marc] We're ready to try something? [Michel] We are ready! [Marc] What have you done? [Michel] I have added the servo amplifier here,   and the synchro transmitter to  simulate the gyroscope output. Normally, we can adjust the pitch  stabilization using this synchro transmitter.

[Marc] So you're trying to control one  of the axis of the platform with this. [Michel] Normally, yes. The pitch is the  inner gimbal. This is this gimbal here,   that position here. [Marc] And it's complicated because  you need 115 volt AC, 26 volt AC,   and 28 volt DC, a synchro, an  AC amplifier, in a control loop. That's a servo loop, right? [Michel] This is a servo loop.

[Marc] The servo loop is not inside this. [Michel] It is outside. [Marc] It's a part of the  electronics we don't have, right? [Michel] Unfortunately, we don't have  everything. We just have the mechanical   part. So we need (to build) all (the) electronics. [Marc] But you brought one, that you know works.

Okay, let's try it! Let me interrupt, yet again, to explain how  a synchro servo loop works. A review of our   previous episode on synchros will probably  help, I’ll put a link in the doodley-doo. As a summary, a transmitting synchro is somewhat  similar to an AC motor used in reverse. It has   3 windings on the stator at 120 degrees of  each other, and one winding on the rotor.

Normally, you power the rotor with 400 Hz AC,   and an AC signal is produced on the three stator  windings, that encodes the position of the shaft. To read that position, the simplest way  is to put another synchro in parallel,   called the receiving synchro.  By virtue of magnetic magic,   the second synchro will align itself on the  first, as we demonstrated in the synchro video. But that only works if the receiving synchro is  moving something light, like the needle of an   instrument. Here, we want to use a transmitting  synchro to move a heavy telescope gimbal. So, we replace the receiving side with a servo  motor loop. The receiving synchro is replaced with  

a Control Transformer. A CT, as it’s called, is  the same as a synchro, but with the rotor winding   off by 90 degrees. This time, its rotor winding  is not powered. It is used as an output instead. If the CT is aligned to the input synchro,   no voltage appears at the output. But if  the two are offset, an AC signal appears,  

that grows larger with the misalignment.  It is called the error signal. We then feed this error signal to a simple  AC power amplifier, and then connect the   amplifier output to the control winding of  an AC servo motor. To complete the loop,   the output shaft of the servo motor  is mechanically connected to the CT,   usually through reduction gears. So the  motor will turn the CT shaft until it   is aligned with the transmit synchro,  and the error signal is back to zero.

This arrangement is very powerful. You  can move entire gun turrets with it. In our case, the control transformer  and motors are already provided in   the astrotracker. All we need is to add  a transmitting synchro and an amplifier,   which Michel has just done.  Let’s see how that works. [Marc] We need the 28 volt first, right? [Michel] Yes. [Marc] So, 'output'. Okay.

And the noise we heard were the thing  being freed, right? Yeah, it's free up. So I have this little super extra control  box here. And I can lock it, or free it. Okay, so, that works. It's  free, it has been freed up. And now, uh, maybe you control it, and I turn it  on and off pretty quickly if something goes bad. [Michel] Yes, it's a good idea. [Marc] So, you're ready? [Michel] I'm ready.

[Marc] 'Enable'. Oh, it works! [Michel] Okay, it is expected because I didn't   connect the generator. So the  loop isn't stable, probably. [Marc] Oh, can I take picture of that? Well, you you're doing something. The average position is... Well,  that's success if you ask me. That's a lot of wires, just to do that. Because  you have the five wires of the synchros,  

the control transformer, you had to find which  capacitor to put for the motor to work correctly. So, you want to try to put the, um... [Michel] ...the generator? [Marc] ...the generator. [Michel] In order to stabilize the loop? [Marc] Yeah. [Michel] Normally, it should work.

[Marc] Alright, well done Michel! The old  astro compass is coming back to life, but it   is overshooting the position and being unstable.  This was a known problem with direct servo loops.   But fear not, there was also a known solution! We  add a new device, called a tachometer generator.   That’s an AC motor in reverse, essentially, that  generates an AC voltage proportional to the speed   of the motor. It is subtracted to the motor  control voltage at the input of the amplifier,   and should prevent the overshoot. This arrangement  was so common, that the generator is an integral   part of our motor, hence called a Motor Generator,  or MG in the drawings. Here is one that Master   Ken took apart and explained on his blog, link in  the doodley-doo, and you can see the two rotors,   the squirrel cage one for the motor section,  and the copper one for the generator.

At this point, Michel and I had given up on  English, so let me self-dub my own video. Warning, I am a pretty poor voice actor. [Marc] So you added the rate transducer? [Michel] Yes, somewhat at random.

[Marc] So, maybe you still need to lower  the gain. There's some progress at least. [Michel] Yes, now it's dampening. Maybe  I don't have enough rate feedback. Or it's wired in reverse? Oh yes, it's dampening out. (Moments later) [Marc] So, you found out what wasn't working? [Michel] Yes. The problem was that  the phase of the motor was inverted,   the reference coil. Oh no, the other one.  I inverted the phase of the control coil.

[Marc] So, it was an anti-servo loop? [Michel] Exactly. But somehow it  still managed to stabilize itself. But now it stabilizes without any overshoot. [Marc] Nice! [Michel] So, the next step is to do  the same thing on the other axis,   the roll axis. Then we'll connect  everything to the gyro underneath. [Marc] See if we can stabilize the platform.  And then it's onto the optical part.

Alright, we have our roll servo loop working!  We just had the feedback wired in reverse,   but once Michel rectified that, it became  stable. We just need to do this again,   in the right direction  hopefully, on the pitch axis. [Marc] Okay, so we have one more amplifier? [Michel] We have one more amplifier, here, and one  more synchro transmitter. And some more wiring. [Marc] Okay, but we don't know in  which direction it's going to turn.

[Michel] Yes. It could oscillate.  We don't know in which direction. [Marc] All right. It either smokes, or it doesn't. Looks like it didn't move. [Michel] Nope. The other one still works.

(More moments later...) [Marc] You found the issue? [Michel] Yes, the issue was the de-phasing  capacitor, which is necessary for an AC motor.   You need 90° between the control and the reference  coils. It's done with a series capacitor. [Marc] Ah, the de-phasing capacitor. We  hadn’t talked about that one and left  

it as a mystery on the schematics until  it decided to bite us in the butt. See,   in our dual coil AC servo motor, we need  to create a rotating magnetic field.   For that, you need one of the coils to be out  of phase by about 90 degrees. This is usually  

done by adding a capacitor in series with  one of the coils. The capacitor is usually   adjusted to give about 90 degrees of phase  lag. You could calculate it, but in our   case we just used trial and error. Looks like  we ended up with error. We need more trial.

[Michel] So, I added one, a bit of a blind guess,  because the motor is much larger for the roll.   There is a much larger moving mass. So, I had put a 0.39 microfarad  cap, which is not enough. So if I put one, a little bigger, I'll add two,   that will be about 1.2 microfarads. Now I  can make it move, but it's not yet optimal. [Marc] But it's moving, it's moving! [Michel] Yes, it's servoed, nonetheless.

[Marc] You were telling me that  the servo loop was a bit saturated? [Michel] Yeah. So, if you look at the scope,   the output signal of the amp is the  yellow trace. It's square, it's saturated. The signal after the cap is the green  trace. So, if we add a capacitor,   it's going to look a little bit  better. But it's still not optimum.

However, it's working somewhat. [Marc] We are so lucky to have you here.  Because, this de-phasing cap business,   we might have found it eventually,  but it could have taken us forever! Not bad, it works better now! [Michel] I can move it in two  directions simultaneously. [Marc] Okay, we're getting closer! [Michel] Yep, getting closer! [Marc] You said, what surprised you, is that there  are coils at 115 volts, and coils at 26 volts? [Michel] Yes. The motor reference coils are at 115   volts, but the tach generators are at 26 volts.  That is really strange, two reference voltages.

[Marc] So, motor reference coils are 115 volts? [Michel] Yes, the motor reference coils  are 115 volts, and the control coils   are standard 26 volt ones. But for the tach  generators, the reference coil is 26 volts. [Marc] I'm impressed that you  were able to figure this out! [Michel] Yes, servo control  loops are my specialty! [Marc] Great, now we have two axes. [Michel] Now we'll be able  to hook up the gyroscope. [Marc] That's all there is to do! [Michel] I'll just prepare it and wire it up. [Marc] Alright, we have two axis servo  control of our gimbal. In the real system,  

the roll and pitch input synchros come from  a vertical gyro assembly, so the telescope   should be servoed to the gyro movements. It’s  finally time to spin up Michel’s beautiful gyro. So, Michel, you brought another item? [Michel] Right. This is a vertical  gyro, to provide a vertical reference. [Marc] So, the idea is that the vertical  gyroscope, well, is always vertical,   regardless of the aircraft attitude.  And it moves the platform accordingly. That's a pretty one! [Michel] So here's a synchro.  There is a synchro on each side. [Marc] Can you spin it up for the camera? [Michel] You want to spin it, to power it up? [Marc] Yes, to see it erect. [Michel] Yes I can, I just need  to connect it to 115 volts.

[Marc] And a one and a two, here we go! [Michel] At first it wiggles all around... [Marc] It makes very little noise  compared to mine. This is a good one. (sound of gyro spinning up) [Michel]   It's at operating speed. [Marc] We can move it a bit? It's magic! So, the idea is to connect this to this. So,  when we wiggle one, the other one wiggles too. [Michel] It will replace those two synchros here. [Marc] Okay! Good work! [Michel] We're making progress.

[Marc] I saw it move! Wait, let me do it, so you're  not in front of the camera. In which direction? [Michel] Try pitch. [Marc] Oh, yeah! Pitch, around this direction. Impressive, very impressive! Even better, with two axes! [Michel] So the roll and the pitch [Marc] OK, Michel rules again, our gyro  is controlling the astrotracker gimbal.   In the real system though, , the  gyro should be attached to the same   frame as the tracker. So let’s move  the gyro on the astrotracker stand.

(Soon after...) [Marc] Go for it. Did it start or not? What's happening? It's connected, it's fine. Do we have a short circuit somewhere? Wires that touch? Yeah! They  touch there. Is it on purpose? No, that's not good here. That's not good.

[Michel] Ah yes, that's not good at all! Not  done on purpose. The 115 volts was shorted out! [Marc] Okay, works better  when there are no shorts! [Michel] It should work already now. [Marc] Ah yes, absolutely! In the other direction, it's harder. Yeah, yeah, it works! Yay, thanks to Michel, we have a gyro stabilized  telescope platform, . Pretty cool! In the next   episode, we’ll turn our attention to  the star tracking optics. See you then!

2025-01-08 21:33

Show Video

Other news

Nanotechnology: The Future of Everything 2025-01-14 14:03
Panasonic CES 2025 Opening Keynote 2025-01-14 03:10
3: Threat Hunting with Microsoft Defender Threat Intelligence 2025-01-13 07:34