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kens

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Posts posted by kens

  1. When using ST4 select "on camera". It is also useful, but optional, when using ST4 to also select as Aux Mount "Ask for coordinates". If selected then every time you start guiding you are prmpted for your declination. This lets you reuse your calibration. Otherwise you need to calibrate every time you start guiding, or at least when you change declination.

    The declination does not need to be entered precisely, within a few degrees is sufficient. It allows PHD2 to adjust its RA guiding to suit the declination.

    https://openphdguiding.org/manual/?section=Tools.htm#Ask_for_coordinates_aux_mount

    • Like 1
  2. @gregk01I just did an experiment that might help you. I started up PHD2 and connected to the StarGo driver without any USB connection to the  mount. The StarGo driver popped up a window asking for the COM port so I clicked OK. It was happy with this even though the selected COM port did not even exist. The connection went ahead as though everything was OK and the guide log shows pretty much the same as yours.

    So make sure that (a) Your USB cable is correctly connected to the mount and (b) that you have selected the correct COM port

  3. 36 minutes ago, alacant said:

    Hi

    Increase the mount guide speeds from zero to at least 0.5 a-s/s for both axes. Then go for a calibration.

    HTH

    The data is showing RA Guide speed =0; Dec guide speed =0; RA=0; Dec=0, PierSide =Unknown. The non-reporting of RA and Dec suggests something more fundamental. With the Avalon mounts you need to set up the StarGo application by loading up a configuration file for the type of mount being used or it just wont work. Seeing as it is a new mount for the OP it is possible that this step has been omitted.

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  4. I usually disbale Star Mass detection:

    https://openphdguiding.org/man-dev/Advanced_settings.htm#Guiding_Tab

    Quote

    'Star mass detection' - tells PHD2 to monitor the brightness and size of the guide star compared to the sky background.   You may need to disable this feature or set the tolerance to a higher number if you're using a fine image scale and are getting too many lost-star events because of  this feature.

    Or it could be a camera or USB problem? PHD2 has an option to save lost star images as well. It is normally enabled to some level so you may be able to view/post one or more of those.

    Not related but your guide rate is very low at 0.1x sidereal. You should increase it to 0.5 to 0.9

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  5. I've been dealing with a similar issue. I had my ASI1600MM-C and AS1120MM-S plugged into a powered USB3 hub (so not using the ASI1600 USB) and that plugged into an Aaeon UP Core computer. All powered from the same 12V source. A lot of the time the ASI1600 would not get connected so I would have to unplug the USB cable and replug it. Never had a problem connecting to the ASI120. At first I thought I would need to delay sending power to the ASI1600 till after the computer had booted but that didn't help. So I'm now trying with a delay in sending powerto the computer so it boots after power has been applied to all the other devices. So far this has been working reliably for a few days. I suspect the issue may be due to the powered USB3 hub needing some time to register the ASI1600 before the computer boots and searches for attached USB devices.

  6. 6 hours ago, Gina said:

    Is this saying that the optimum gain is unity (139)?

    There is nothing magical or optimal about unity gain. It is just a value of amplification that causes one ADU to rcorrespond to one electron captured by the sensor. 

    The charge on the sensor is converted to a voltage which is then amplified before being converted to a digital value in the ADC. Collectively, the errors introduced are quantified as read noise.

    If you are aiming for maximum dynamic range then try zero gain. But if you find that for a given integration time you have only a small number of subs then quantization error could be manifested in the result. If so the using a higher gain and more subs may be beneficial - but at the expense of saturation of brighter parts of the image.

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  7. Its more the case that CMOS sensors generally have lower read noise so shorter subs are possible. You want the subs to be long enough on any sensor type, that the shot noise dominates the read noise. That way, stacking more shorter subs approaches the efficiency of longer subs in terms of getting a given SNR versus integration time.

    The length of the subs needed for shot noise to dominate read noise depends on gain and sky background. You want to expose so that the sky background equates to somewhere in the order of 3 to 10 times the read noise squared. When you can control the gain, lower gain gives more dynamic range but higher read noise. Once you get beyond 10 x read-noise squared you are getting more saturation with little gain in stacking efficiency. Below 3xRN squared you need more integration time to get SNR equivalent to longer subs.

    For the ASI1600, the optimal minimum gain is around 76. If your sub lengths at that gain are workable then use that. For NB you may need a higher gain to get workable sub lengths but with higher gain you lose dynamic range. A maximum gain of 200 gives a reasonable dynamic range - 10.5 stops; which gives some room for stretching. If you want something in between then unity (139) is a good choice. You don't need gain to be more precise than those three values and you don't need  to be too precise with the actual values. I tend to use 70, 140 and 200 as they are easy to remember.

    Another factor with the ASI1600 is that it has a 12bit ADC so quantization noise is a consideration, especially at low gain. That can be overcome with more subs - say 40 or more. You are talking 50 to 100 subs so that is not really an issue for you.

     

     

     

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  8. According to the log you were trying to calibrate at the celestial pole (Dec 90). Try calibrating closer to the celestial equator (Dec 0). 

    Near the pole, any movement in RA makes only a small movement on the camera. 

    Also, alter your step size back to 1000ms (or use the calculator) to give around 12 steps.

  9. 10 hours ago, R26 oldtimer said:

    If I am getting James question right, it's about more about setting the mount in an accurate home position (weights down-scope pointing North), rather than polar aligning (which comes next).

    If that's the case I've found this tutorial quite helpful: https://www.myastroscience.com/homeposition

    I assume you are commenting on my post. Whilst it is easy enough to get a weights down position with a spirit level it is harder to get the declination aligned to the pole. The tutorial I linked shows how to use the SPA Tool to help point the OTA at the pole rather than for polar alignment. Any tool that calculates the centre of rotation could be used. Indeed, one could set a longish exposure time and rotate the mount to get an arc and eyeball the centre of rotation. If the mount is already polar aligned then the centre of rotation is close to the pole and adjusting the OTA in declination can bring that point to the centre of the FOV at which point you are at dec +/-90 within a few arcminutes. Any residual offset that is orthogonal to the declination movement is due to cone error. If that is substantial you would need to shim the OTA to bring the centre of rotation to the centre of the FOV.

  10. I use the Static Polar Align (SPA) tool in PHD2. If your polar alignment is already good you use SPA to find the centre of rotation of your mount. Then adjust in declination to bring that point to the centre of your field of view. Any offset that is at right angles to declination is due to cone error so you may want to adjust that too.

    Once centred set your mounts home position there.

     

  11. There is a floor on practical sub length. Once they cease being shot noise dominant and become read noise dominant you need more integration time to reach a given SNR. And at some point the individual subs may not have enough SNR to stack. And you also get to a point where download time can be significant leading to more wasted imaging time.

    So let's say that lower limit is 30s and your mount has a worm period of 600s and PE of 30" p-p. So every 300s it moves 30" and in 30s it moves around 3" which would be noticeable. 

  12. 8 hours ago, vlaiv said:

    When we average above sub pixels we will end up with noise being 5*noise / 9, or SNR improvement will be 9/5 = x1.8

    That is very interesting fact - we assumed that it will be x1.5 but calculation shows that it is x1.8

    Now, either I made mistake in calculation above or this is in fact true.

    Any thoughts?

    On the principle that "you don't get something for nothing" I would think the discrepancy arises from using upsampled pixels. The signal per upsampled pixel is not the same as if they were real pixels so when you bin red with orange, green and blue, intuitively you are introducing noise. Otherwise you could upsample 4x before binning 6x6 get an even better result of 2.0

  13. The main issue from poor polar alignment when guiding is field rotation causing elongation of stars

    If you plug in the details of your specific imaging situation into the field rotation calculator at http://celestialwonders.com/tools/rotationMaxErrorCalc.html you can se if field rotation is an issue. It gets worse the closer you are to the celestial pole but for the vast majority of likely situations, 5 arcmin is indeed good enough.

     

  14. 6 hours ago, masjstovel said:

    1. Is this a good camera to go for?

    Yes. Many people have made very good images with it

    2. It's sold with options of filters 1.25", 31mm or 36mm - Why these options, and what determines what i would choose?
    Depending on sensor size, F-ratio and distance from sensor to filter, vignetting may occur. The ASI1600MM enables the filters to be placed close to the sensor so even with 1.25" filters, vignetting with F-ratio down to F/5 is minimal and can be easily calibrated out. Larger filters cost more. You may want to use higher quality filters especially for narrowband. The lower cost of 1.25" filters may make this more affordable for you. I use Astronomik filters.

    If you intend to go with a larger sensor down the track you may want to get larger filters to suit. Filters are a significant part of the cost in mono imaging.

    3. Would you go for another camera in this price range, and why? - Or to rephrase it a bit; If you were in my shoes, which camera would you og for?
    I went for the ASI1600 and have not regretted it.

     

    • Like 2
  15. On 29/09/2019 at 21:54, Gina said:

    My exposures are unlikely to be over 2m maybe 5m for dimmer DSOs.  The lower read noise permits shorter exposures at higher gain

    I shall need to experiment to find the best balance between full well capability and gain/sensitivity.  For my very wide angle images I have been using 60dB gain (the maximum) but may find longer exposures and lower gain give more image depth.  At least the high sensitivity of the ASI makes focussing and plate solving easier/quicker.

    Yes, lots of experimenting and practice needed to get the best out of the camera and the new software, though I did use PixInsight before, it was some time ago and I need to get back into it.  Still learning KStars/Ekos/INDI.  I like the control the Open Source INDI drivers give me - I can change them to control practically everything. 

    I think the problem I'm having with distrusting my decisions is probably all due to this terrible weather and not being able to actually capture images!

    Thank you for your encouraging comments :thumbsup:

    60dB gain (gain 600) is way too high. You have less than 4 stops of dynamic range there. I keep the gain at 200 (20dB) or lower where the dynamic range is a bit less than 10 stops.

    Typically I use gain 75 for luminance,  139 (unity) for RGB and 200 for narrowband unless I an get a reasonable exposure at 139.

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