Question about large lunar and solar mosaics

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Leo Shatz avatar

I’m interested to hear from users who are doing larger lunar or solar mosaics, especially at longer focal lengths.

One issue I have been looking at recently is residual drift during longer lunar and solar imaging sessions. Many mounts provide standard Lunar and Solar tracking rates, but these rates are still approximations. The actual apparent motion of the Moon and Sun changes continuously with time and depends on the observer’s location.


For short captures, this may not matter much. However, even with perfect polar alignment, during larger mosaic projects, even a small mismatch in tracking rates can gradually show up as drift, framing inconsistency, or extra tweaks needed to keep each panel well positioned.

This is especially noticeable with the Moon, where the apparent motion is much faster and changes more significantly than the Sun’s. The standard lunar rate can reduce drift compared with sidereal tracking, but it does not fully follow the Moon’s true instantaneous topocentric motion.

I’m curious how do you handle this in practice when doing larger lunar or solar mosaics:
• Do you rely only on the mount’s Lunar or Solar tracking rate?
• Do you see drift during panel capture or between panels?
• Is tracking drift a noticeable issue for high-resolution mosaics at longer focal lengths?

One possible way to reduce this kind of drift is to use dynamically updated ephemeris-based tracking rates rather than relying only on a fixed Lunar or Solar tracking rate. I recently implemented this approach in HelioMaker as an optional feature called Dynamic Target Tracking, intended to work alongside SharpCap Pro. It continuously updates the mount’s custom RA and Dec tracking offsets based on the selected object’s real-time apparent topocentric motion. To be clear, HelioMaker is not currently fully integrated with SharpCap’s mosaic workflow to automate panel-by-panel mosaic capture. That is something I may consider adding in the future.

However, even in the current released version, Dynamic Target Tracking can improve the baseline tracking accuracy during lunar or solar mosaic imaging sessions. In practice, this can help reduce residual drift and keep the target more stable in the field during longer captures or manual/semi-automated mosaic workflows.

I would be interested to hear what others have experienced with large lunar and solar mosaics in SharpCap and other imaging software, and whether residual drift during mosaic work has been a noticeable limitation.

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Tony Gondola avatar

In practice it’s not an issue. Here’s a mosaic I did using SharpCap":

https://app.astrobin.com/i/o7uc18

It’s made up of 27 panels with the original captures being 2000 frames long. I did use lunar rate but it only takes about a min. to do each capture so in that time, drift just isn’t a factor if you have a good PA. SharpCap can also automatically keep an object centered through guiding if you need it.

Each Panel is framed manually and that’s about it. It took about 45 min. do do all 27 panels for this mosaic.

I don’t do solar so I can’t address that but with modification of the basic techniques I would imagine that it’s not that different.

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Leo Shatz avatar

That is a very useful feedback, thanks for sharing it. Your workflow makes sense, especially if each panel capture is only about a minute and the polar alignment is good. In that situation, I agree that drift may simply not have enough time to become a practical problem.

My experience was somewhat different when I tried a lunar mosaic without good polar alignment and using just the mount’s lunar tracking rate. The Moon drifted noticeably between panels, and I ended up with missing parts in the mosaic that had to be added manually later. Even though I used a fast planetary camera, the full process took more than just a minute per panel once I included the number of frames captured, slews between panels and mount settling time. The whole mosaic sequence was closer to about 15 minutes.

I can certainly attribute a large part of that drift to imperfect PA. However, later tests made me think that the standard lunar rate itself can also be part of the issue, depending on the setup and duration.

One interesting test was PHD2 calibration directly on the Moon. With standard lunar tracking, I saw an orthogonality error of about 14 degrees, even on a mount with excellent polar alignment. With Dynamic Target Tracking enabled, the calibration result was practically clean, with almost zero orthogonality error.

The same is visible just by watching the Moon in the camera view. With the standard lunar tracking rate, after a few minutes there is still a visible residual drift. With DTT enabled, the Moon stays much more stable.

So I agree that for short panel captures, good PA and a manual workflow, this may not be a major issue. But for longer panel captures, higher focal lengths, less than ideal PA, more automated workflows, or situations where settling and framing overhead add up, improving the baseline lunar tracking rate can still make the process more stable and forgiving.

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