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| subject: | Interferometry and Re-focus, was Re: ATM Kennedy Optics vs Galaxy Optic |
From: "James Lerch" To: "ATM List" Reply-To: "James Lerch" ----- Original Message ----- From: "Mark Suchting" > > At 09:24 PM 8/10/2003 -0700, John Sherman wrote: > > >A few people asked me if I still have the original interferometer data from > >my Galaxy mirror. Yes, I do. See www.johnspics.com/hi/hudek.jpg > > The shame about this mirror ( in its original form ) is that most of the > error is just pure overcorrection ....1.6 waves in fact, which refocuses > at best fit to 0.4 waves P-V ( with focus subtracted, as a shown on the > interferogram). This equates to 15% overcorrection for a 22" > F4.5. Hi Mark, Tell me more about this "refocus" trick... Having translated a Foucault data reduction program (I won't say I wrote it, as I didn't!) when I read "refocuses at best fit" I think along the lines of finding a best fit Radius of Curvature for the reference parabola. Once the best fit RoC for the reference parabola has been found, and the Strehl reported, "Refocusing" to a different reference parabola has never made the Strehl and RMS values improve (else the code should have used that one to start with..) Once the best fit RoC has been found, if the optic shows 15% overcorrected, the only 'trick' I've found to make the Strehl and RMS improve is to select a different, non parabolic reference surface (ie changing the Conic Constant, Deformation Constant, "little b", what ever we want to call that term that describes on optical surface as spherical = 0, ellipsoid -1, parabolic = -1, hyperbolic = <-1) I ask all this as I was once told the following: "... the mirror is indeed undercorrected. I have as much as 1/3 wave total aperical aberration, which can refocus to about 1/16 wave by my worst axis measurement (not the two combined)." I studied that paragraph for some time to try and decipher it. My testing showed that the optic was undercorrected with a 1/3.8 lambda (550nm) P-V wave front error. Assuming the author didn't change the definitions of "1/3 wave" and "1/16 wave" mid-stream in the same sentence, I presumed the author was referring to P-V wave front error as the original "1/3 wave" is very near my 1/3.8 P-V wave front value. After presuming to solve the "1/3 wave" mystery, I set about trying to solve the "refocus to about 1/16 wave" mystery. I first found that changing the best fit RoC wasn't the answer as this made things worse, not better. After a bit of head scratching I found that if I changed the Conic Constant to "b = -0.92" I got a 1/19 lambda (550nm) P-V wave front error, well that's pretty close to "1/16 wave"..... Based on my limited experience, and your writings Mike, I wonder if in certain circles "Refocusing" really means changing the Conic Constant? In your case the optic could be advertised as having a 0.859 Strehl, but it would be false to claim that Strehl AND say it is a parabolic mirror.... > I note also that the section showing what `terms' have been removed from > the data has been chopped off the printout ie focus , astigmatism. . I'm > well familiar with what Zygo `Zap' software printouts should look like in > completeness. > > I would suspect from the three equispaced bumps on the phase map, that > astigmatism has been subtracted too. This seems to be standard practice > amongst companies offering interferograms, because of the astigmatism > induced by self weight deformation, but I would question how much effort > goes in to analyzing how much real astigmatism these mirrors might have, > before it is `subtracted out'. Another interesting point! I've been trying my best to Star Test Charlie's mirror (the latest Robo test subject) using an artificial star and a CCD camera. Unfortunately Charlie's mirror is odd in the fact that front optical surface is a larger diameter than the back side diameter of his mirror. This gives the mirror a Conical shaped edge, which is near impossible to support with the mirror vertical for the following reasons: #1 The outside edge of the mirror is very glossy and smooth, AND its cone shaped! #2 Slings and posts that try to support the mirror without touching the beveled face, cause the mirror to slide forward against the mirror clips as the mirror nears vertical (needed to aim at an artificial star) #3 Slings and post that support the mirror ON the bevel (only way to keep it from sliding forward, off the cell and onto the mirror clips) introduce "Stupid" amounts of astigmatism that goes away when the Telescope is pointed at a REAL star. Unfortunately the Real Stars move, and the ones that don't move that much (like Polaris) are too dim to image without long exposure. #4 Gluing the mirror to the cell might help solve the "aiming at an artificial star" dilemma, however Charlie's existing cell is not setup to properly support that much weight in tension directly from the 9 support points (the cell works great in compression!) Current efforts to image the star test results for Charlie's mirror are to be done on an Equatorial Dob platform and a real star such as Vega. Currently were just waiting for a clear night. (apologies to Central Florida observers, the monsoon like rains of late may be our fault ) > Probably the only way to produce an honest interferogram of a large thin > mirror is to build a testing tower so that the optical axis can be vertical > and the mirror lying flat on a flotation cell. Standard practice for large > professional mirror labs. Point well taken! James Lerch --- BBBS/NT v4.01 Flag-5* Origin: Email Gate (1:379/100) SEEN-BY: 633/267 270 @PATH: 379/100 1 106/1 2000 633/267 |
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