Bill McLaughlin · Jun 12, 2026 at 03:54 AM
John Hayes · Jun 11, 2026, 07:21 PM
If the telescope always reports say 3” FWHM in a location where the typical seeing from the monitor is showing 1.5”, there might be something wrong with the scope.
Or maybe something is set up wrong with the monitor. I suspect that could be fudged to look better than it should pretty easily.
I’m not only a HCRO customer (the CDK14 in the SE corner of Kronos is me), but I also wrote the software that now operates the Santa Barbara Scientific SM-3 seeing monitor there. I wrote it over the past two years because the original ST-i-SM app that SBS supplied for these units had reliability issues. It also offered no good way to get its measurements exported in a manner that is consumable by imaging apps that didn’t involve scraping the contents of periodically-updated text files and other ugly software anti-patterns. With SBS closing up following the unfortunate death of its co-founder, Michael Barber, I picked my project back up and have been testing it at HCRO. On the theory side, I wrote it as a part of my studies in speckle interferometry and participation in a group that does double star research. Part of this practice is understanding theories of atmospheric turbulence and its effects as speckle interferometry aims to undo those effects in order to resolve and measure close binary stars.
In some respects, seeing analysis has close parallels with guiding software. Both aim to detect movement, but of different types. Guiding software wants to ignore the atmospheric turbulence and instead find and respond to mechanical aberrations in tracking. Seeing analysis would like to ignore mechanical movement and only measure atmospheric turbulence. Any of the unwanted stuff creeping into the findings of either is bad and counter-productive to the respective goals. We don’t want to “chase the seeing” with guiding and we have fancy masks and solidly-mounted arrangements for different types of seeing monitors to lock out the influences of movement.
To your wondering if “something is set up wrong” when it comes to seeing monitors, I would be interested in knowing what you might think that “something” might be. I’m guessing that you’re trying to imagine the system in your mind’s eye without really knowing how the system works and is internally structured. Maybe I can help explain that.
Seeing analysis follows a very standard formula. Well, it’s a chain of formulas that vary at the end based on the type of seeing monitor (DIMM, SIMM, etc.) in use, but they all follow a very generalized theme outlined in The ESO differential image motion monitor (Sarazin & Roddier 1990).
Collecting a sample stack of images and finding the centroid of a star or centroids of a spot pair in each
Producing the x/y sigma of the movement across that sample size and feeding it into Kolmogorov’s atmospheric turbulence theorem to find the Fried parameter (r0).
The Fried parameter is a physical measurement and can be thought of as the largest aperture that would be diffraction-limited under the measured conditions. It’s calculated for a given wavelength, so it applies to a specific part of the spectrum and does not apply to the whole of it. Customarily, 500nm is used for general visual broadband. However this means that the effects of turbulence on specific wavelengths can be measured, such as the center wavelength of the optical filter being used by the main imaging telescope. Put simply, larger is more desirable. The cellular turbulence tends to be more stable. But not always, as there is the temporal complement to r0, tau0 or the atmospheric coherency duration. More stable atmosphere entails a large r0 and longer tau0.
r0 is used with the constant that describes a diffraction-limited seeing disk in Kolmogorov turbulence to find the FWHM.
The effects of airmass are removed from the result by applying Kolmogorov’s airmass scaling law, producing a final zenith seeing in FWHM arcsec.
The math itself takes only a single variable input of observing wavelength, which has highly minor effects on the outcome. The pixel size, focal length, and aperture size of the imaging optic must also be known and correctly-supplied, and this can be very easily done. Much of the accuracy comes from sufficiently quality-gating the images that go into the stack for analysis.
Calculating tau0 is complex because the atmosphere is many-layered and there are both local and large-scale effects throughout the air column. However the most outsized effector would be the jet stream, so its winds are usually what are used to determine tau0.
So, using the widely-accepted method of analyzing the seeing, there really isn’t any place to “put a finger on the scale” in terms of favorably skewing things. In fact, there are a lot of ways to deleteriously impact the ability to accurately assess the seeing. Seeing monitors at large professional observatories are often located up on a very sturdy tower in order to raise the system above highly local ground effects such as heat and turbulent air coming off of nearby buildings. Dust accumulation can affect centroiding.
Hope this helps understand it more.
-Dale