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Hi Michaeli think your setup is causing you a lot of issues, specifically your calibration steps seem off, and you are guiding at 1/2 a second (whereas you typically want 3-5 second range)if you look at your guiding assistant run, you can see the insane amount of instability in your DEC axis (red) *and* in your RA - this is without the motors moving at allmy suggestion is to do a baseline guiding with reasonable guiding numbers and see how it goes:Brian
On Sun, May 17, 2020 at 2:55 PM Michael Borland <michael...@gmail.com> wrote:
I see a 0.6" peak-to-peak oscillation with a 5.6-s period on my CEM40EC. This is with the guide camera (ASI290MM mini) looking directly through my OTA (8" LX90-ACF, FL=2000mm) (even the OAG is out of the way to eliminate any possible confusion). A guide log is attached. The 15-minute-long record is perhaps the most interesting, since I adjusted the RA rate to more or less remove the slow drift.--It seems this oscillation is too fast to correct, since by the time PHD2 sees it, it's probably too late (I get ~1 update rates even with short exposures). For now, I've settled on using a 6-s guide camera exposure time average the oscillation essentially to zero, so PHD2 doesn't chase it. I also found the LowPass2 method seems to work pretty well. However, I still see slightly oblong stars because I'm usually imaging at about 0.5"/pixel. The star shape doesn't depend much on the main camera exposure time, except when it is very short, in which case it oscillates with half 5.6-s period, as I'd expect.Because the oscillation is very narrow in the frequency domain, it should have constant phase for a significant period of time. In light of this, I wonder if it can be countered by a simple preset series of alternating pushes at the position of the predicted zero crossings. Using a short exposure time on the guide camera, I should see the 5.6-s period showing up if the phase and amplitude of these kicks is not right. Hence, a slow adaptive loop could perform an FFT the last, say, 60s of star positions and use that to adjust the phase and amplitude of the kicks. Is there any way to try this in PHD2?Thanks in advance for any comments or advice.--Michael
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>>>> I set the guiding interval at 0.5-s deliberately in order to understand the mount behavior.Hi Michaelit would be interesting to see your guide log from the longer exposuresI mentioned before, if you look at unguided results during your GA run of your DEC axis, you can see the significant instability. and the DEC motor isn't running at all. So that suggests to me the instability is your seeing conditions, and not a function of the mount performance.your RA oscillation of 5.6s is a very small amplitude, and a very fast time period. I doubt you could effectively guide that out predictively, but you could try PPEC with a fixed 5.6sec period with high predictive and low reactive values, and guide at 500ms, but there's so much that could go off the rails there. Might be worth a shot. I did something similar but it was for a 41 sec intervalanother possibility is using an AO unit which can guide at that kind of rate fairly well
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Hi Michael. I think Brian has you on the right track here. It would help if you could also post one or two raw, full-resolution, unprocessed main camera images from this session including the timestamps when they were taken. Those will let us evaluate the star elongation quantitatively while matching it against the guiding performance.
Thanks,
Bruce
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Hi Michael. The zip file is giant and I don’t want to get tangled up with the Google tools for unzipping it before downloading. Trying to download the whole zip file seems to get wedged after Google complains it can’t do a virus scan. Could you just post one representative FITs file so I can look at that?
Thanks, sorry to bother you with this sort of stuff,
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Thanks, Michael. I think this confirms what we suspected, that your star-shape problems are not caused by guiding. Here are the average aspect ratios of the stars in these two images:

The aspect ratio is the percentage difference between the lengths of the major and minor axes of the Airy star disks in the image. By most standards, a value of 10% or less is excellent, generally not noticeable to the human eye. This corresponds to an ellipticity of 0.4 if you’re more accustomed to that measure. Taking it a step further, we can see most of the elongation in your images occurs with stars that are nearer the margins of the image, and there is significant variation among the stars in the field. This points to optical effects of one sort or another because guiding/tracking errors are going to affect all the stars equally.
As Brian said, your tracking/guiding performance is quite good with little difference between RA and Dec RMS. That tells us you should be getting round stars, and I think you essentially are subject to the optical limitations. So I think that fiddling around with your guiding operations would be at best a waste of time at this point, and you can probably focus your attention on other parts of imaging – post-processing and probably better optical performance.
To come back to your original questions – which we never answered – there really isn’t any way in PHD2 to direct a particular guide command at a particular time. It could be done, I suppose, if you wanted to write your own guide algorithm or develop a companion application that would control the mount itself. It would be a challenging project because usually there is no way to learn the gear angle at the time you start guiding. The mount firmware often knows that number but it isn’t reported through any standard interface. So each time you slew the scope, you would have to repeat the process of deducing where you are in the RA gear phase. The PPEC algorithm does that but it isn’t an easy problem and it becomes more difficult as the target period gets smaller. That’s because the signal you’re looking for is increasingly lost in the seeing noise. You mentioned a couple of times that you were concerned about drift rates. For guiding, drift is typically a non-problem because it is the easiest thing to correct for and rarely has any effect on the final results.
Hope this helps,
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If you get some time, it would be interesting to see a few frames in a heavy starfield (think milky way), maybe 3 images of about the same exposure 180s as I recallthat could shed more light on star shape detailsBrian
On Mon, May 18, 2020 at 6:04 PM Michael Borland <michael...@gmail.com> wrote:
Bruce and Brian,--Many thanks for the analysis. I had myself convinced that it was a mount problem, but your analysis has me doubting that conclusion. I analyzed some images of M57, which have somewhat more stars, and these showed similar results. I am still puzzled by the fact that the stars are all elongated in the RA direction, which could be just coincidence of course. Presumably, if it was field curvature, all the ellipses of stars should point toward the center of the FOV. Does that indicate a tilt in the optical system?A few more observations:1. I checked for a tilt in the imaging train by rotating the entire imaging train by 90 degrees about the telescope axis. The ellipses kept their orientation relative to the celestial coordinate directions, which means it is in the OTA or mount. (Unfortunately, I can't rotate the OTA relative to the dovetail.)2. I'm pretty sure my backfocus is within 1 mm of the Meade's specified value of 4.57" for the LX90 ACF. I have a variable T extender that I'll use to play with this and see if I can make any improvements.3. Looking at out-of-focus images of stars I concluded that the collimation was quite good, but have an artificial star that I'll try, since that should be more controlled. I guess I can also use this to check the imaging curvature.4. With a non-correcting Antares 0.63 reducer, my star images are very round. (I don't often image that way because I'm interested in galaxies this time of year and want higher magnification.) I had concluded that this was just because with a 0.63 reduction factor, my guiding issues were invisible.5. Some time ago I acquired a series of short exposures (1s I think) in rapid succession using the imaging camera, then analyzed their eccentricity using PixInsight. It showed a sinusoidal variation, which I interpreted as variation in the spot sizes with phase during the 5.6-s oscillation (the effect is expected to be worst at the zero crossings and least at the crests). This still seems convincing to me but I need to repeat the experiment since I've made other improvements since then and I deleted the original images.Thanks again! I'm relatively new to the on-line astronomy community and I'm very impressed by how helpful people are.--Michael
On Sunday, May 17, 2020 at 4:54:58 PM UTC-5, Michael Borland wrote:I see a 0.6" peak-to-peak oscillation with a 5.6-s period on my CEM40EC. This is with the guide camera (ASI290MM mini) looking directly through my OTA (8" LX90-ACF, FL=2000mm) (even the OAG is out of the way to eliminate any possible confusion). A guide log is attached. The 15-minute-long record is perhaps the most interesting, since I adjusted the RA rate to more or less remove the slow drift.It seems this oscillation is too fast to correct, since by the time PHD2 sees it, it's probably too late (I get ~1 update rates even with short exposures). For now, I've settled on using a 6-s guide camera exposure time average the oscillation essentially to zero, so PHD2 doesn't chase it. I also found the LowPass2 method seems to work pretty well. However, I still see slightly oblong stars because I'm usually imaging at about 0.5"/pixel. The star shape doesn't depend much on the main camera exposure time, except when it is very short, in which case it oscillates with half 5.6-s period, as I'd expect.Because the oscillation is very narrow in the frequency domain, it should have constant phase for a significant period of time. In light of this, I wonder if it can be countered by a simple preset series of alternating pushes at the position of the predicted zero crossings. Using a short exposure time on the guide camera, I should see the 5.6-s period showing up if the phase and amplitude of these kicks is not right. Hence, a slow adaptive loop could perform an FFT the last, say, 60s of star positions and use that to adjust the phase and amplitude of the kicks. Is there any way to try this in PHD2?Thanks in advance for any comments or advice.--Michael
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Michael
Michael
I think you'll find their offer not appealing. Use it if you can't see star elongated.
Michael
Yes, 26 lbs is a bit intimidating for me when it's a precision component and not, say, a box of kitty litter. Maybe they'll throw in a robotic exoskeleton to make it a good trade? ;)
Michael
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--Tom Sargent
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--Tom Sargent
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I'm also using an OAG on a 2000mm FL SCT. I tried what you suggest but found that my seeing was never good enough to make it stable. I got the best results by using a 6s exposure, which averages out the oscillation almost completely and at least allows guiding out any other problems. (My mount also exhibits linear RA drift that varies with pointing direction. I've seen it as bad as 2" per minute.)
Michael
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I have the same problem on my CEM40ec..about 10 cycles/minute. I’ve fiddled with Phd2 parameters and tightened the RA belt but to avail. Please keep us posted as to your success. I Really don’t want to send my mount back to MA!
Ray
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Ray:I think most cem40 owners are very happy with their mount. A few of us get the ones with the oscillation problem. I don't know of any one who has had the problem fixed (maybe there are some, but I haven't run across them). So you should hope that sending it back will work. I think it's your only hope of having a working mount.
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