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#41
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It's not clear to me why it's easier to figure a complex curve on the
corrector plate (lens) rather than parabolizing a spherical mirror. Please elaborate. Well two possible reasons..... The first I am just making an educated guess backed with a little optics making experience... The corrector is pretty much flat...which is the same as saying it is a sphere with a very large to nearly infinite radius.... The primary mirror is section of a sphere with a very short radius... As a general rule, when polishing a sphere, the shorter the radius....the more it "wants" to be/stay a TRUE sphere and the HARDER it is to deform the polishing tool/strokes to create the non spherical surface (ie the correction)...so you have two opposing "conditions" that both become more extreme in their opposition the shorter the radius of the mirror becomes....And SCT primaries are pretty darn short To understand this, remember the ONLY surface shape where you can rub surfaces together is a sphere (with a flat plate just being a sphere of infinite radius).....the fact that pitch can give a little (and in just the right way) is what even allows you to polish (barely) non spherical astronomical mirrors... Now consider the corrector plate, its basically flat, so you are only "fighting" one problem, the correction, and not so much the desire to be a good sphere....of course that also means its easier for the corrector to become all kinds of other undesirable shapes....ie a LARGE flat surface is a royal pain for an optican to make...try pricing an 8 inch F6 1/4 wave mirror and an 8 inch 1/4 wave flat and you'll get the idea pretty quick! Now, up to this point I am just hand waving and havent explicity heard this before so I dont really know if this is TRUE or just sounds good.... The second reason is the REAL one I am pretty sure.... They take a flat corrector plate.....put in on a mechanical widget....and pull a vacuum on it.....or perhaps deform it in some other mechanical way.... The flat plate now becomes a shallow bowl shape....but the shape is NOT exactly spherical.... So, they now grind/polish this warped plate until it becomes a good sphere....and remember this is the easiest/cheapest/fastest most reliable surface an optician can make.... When they have a good sphere they remove the plate from the widget....and it springs back into its old mostly flat self.... Now remember it was NOT spherical (the one surface that is) when it was deformed, but it was MADE into one in its deformed state.... This means that in some areas of the plate more material HAD to be removed and in some areas LESS.... So, what you end up with is a plate that is NO LONGER uniformly thick...and VIOLA, if you done the calcs and the procedure correctly you now have a plate with the right amount of correction on it! Now this isnt easy to engineer or get the procedure down pat, but once you do, you can mass produce decent correctors at an affordable price... BTW, if you want an amatuer "makeable" version of something like an SCT that has a FAST (F4 to F6) with EXCELLENT imaging (better than just about anything else) and only requires making spherical surfaces 2 lenses and 1 mirror....investigage a Laurie? Houghton design... Very few have been made but I bet an 8 inch F6 one would give even a 7 inch apo a good run for the money.... take care Blll |
#42
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![]() starman wrote: Being one of the closest galaxies, M-31 would be spectacular if we could see all of it's size with the naked eye instead of just the central core. Reminds me of the time in Tahiti/Morea when I first saw the Magellanic Clouds. Naked eye, I just thought they were true clouds. Binos revealed them for what they were -- spectacular. Alas M31 is a tad farther away (or maybe, considering is size, a good thing)! Phil |
#43
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starman wrote in message ...
BllFs6 wrote: the best part is (three....) it is easier/cheaper to put the optical correction on the plate because of how they do it rather than putting the correction on the mirrors... It's not clear to me why it's easier to figure a complex curve on the corrector plate (lens) rather than parabolizing a spherical mirror. Please elaborate. It's because a little trick is used to manufacture the corrector. First, a flat piece of optical glass is placed on the mouth of a vacuum chamber. When the pressure is reduced, the glass will warp slightly inward in a complex curve (more in the middle than the edges, of course). The outer surface of the glass is then ground and polished into a slightly concave spheroid, which is relatively easy. When the glass is removed from the mouth of the vacuum chamber, it warps back, and now it's a Schmidt corrector. - Robert Cook |
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starman wrote:
Being one of the closest galaxies, M-31 would be spectacular if we could see all of it's size with the naked eye instead of just the central core. We *can* see most of its size with the unaided eye and not just the core when M31 is observed from a dark sky site. From my rural site, I can see between two and three degrees of total length with averted vision, and from the site of the Nebraska Star Party, it looks to be all of 3 degrees and maybe a bit more. In my 10x50 binoculars, I have measured it out at just about 3 degrees as well. Clear skies to you. -- David W. Knisely Prairie Astronomy Club: http://www.prairieastronomyclub.org Hyde Memorial Observatory: http://www.hydeobservatory.info/ ********************************************** * Attend the 11th Annual NEBRASKA STAR PARTY * * July 18-23, 2004, Merritt Reservoir * * http://www.NebraskaStarParty.org * ********************************************** |
#45
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David Knisely wrote:
starman wrote: Being one of the closest galaxies, M-31 would be spectacular if we could see all of it's size with the naked eye instead of just the central core. We *can* see most of its size with the unaided eye and not just the core when M31 is observed from a dark sky site. From my rural site, I can see between two and three degrees of total length with averted vision, and from the site of the Nebraska Star Party, it looks to be all of 3 degrees and maybe a bit more. In my 10x50 binoculars, I have measured it out at just about 3 degrees as well. Clear skies to you. -- David W. Knisely I've seen about two degrees with averted vision too but imagine seeing all of it with the naked eye looking directly at it. It would look like a saucer floating in the sky. -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#46
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Robert Cook wrote:
starman wrote in message ... BllFs6 wrote: the best part is (three....) it is easier/cheaper to put the optical correction on the plate because of how they do it rather than putting the correction on the mirrors... It's not clear to me why it's easier to figure a complex curve on the corrector plate (lens) rather than parabolizing a spherical mirror. Please elaborate. It's because a little trick is used to manufacture the corrector. First, a flat piece of optical glass is placed on the mouth of a vacuum chamber. When the pressure is reduced, the glass will warp slightly inward in a complex curve (more in the middle than the edges, of course). The outer surface of the glass is then ground and polished into a slightly concave spheroid, which is relatively easy. When the glass is removed from the mouth of the vacuum chamber, it warps back, and now it's a Schmidt corrector. - Robert Cook I forgot about that 'trick'. I've read that a mirror can be parabolized by heating it to a certain temperature, then polishing it to a sphere. When the mirror returns to normal temperature it has a parabolic surface. Here's more on that subject: http://www.digilife.be/club/johan.va.../thermally.htm -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#47
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starman wrote in message ...
Being one of the closest galaxies, M-31 would be spectacular if we could see all of it's size with the naked eye instead of just the central core. Well, just think, we have something almost as good: the Milky Way! The problem with the Milky Way is that we can't see its spiral structure from our position. But if we could, then we would also see its core, and that would be a significant source of light pollution. You can see what a difference this makes (on a smaller scale) by comparing a near edge-on galaxy such as M104 (where the core is somewhat visible) to a truly edge-on galaxy such as NGC 891 or NGC 3628. I would imagine that living in the Virgo Cluster would be a mixed blessing. I once estimated that about 35 giant galaxies would be visible to the naked eye there. I didn't consider the effects of 15 or so naked cores on the overall visibility, although i did mention something about denizens of M87 having to wait until Virgo A sets before they could see anything. (M87 has no dust lane to hide its massively bright nucleus, and even at 55 million light years away, M87 is *easily* visible through 50mm binoculars from my suburban back yard.) The Magellanic Clouds--particularly the LMC--are a good compromise. Now, all we need to do is pack up and move to Tahiti... Clear skies! -- ------------------- Richard Callwood III -------------------- ~ U.S. Virgin Islands ~ USDA zone 11 ~ 18.3N, 64.9W ~ ~ eastern Massachusetts ~ USDA zone 6 (1992-95) ~ --------------- http://cac.uvi.edu/staff/rc3/ --------------- |
#48
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starman wrote in message ...
Robert Cook wrote: starman wrote in message ... It's not clear to me why it's easier to figure a complex curve on the corrector plate (lens) rather than parabolizing a spherical mirror. Please elaborate. It's because a little trick is used to manufacture the corrector. [snip] I forgot about that 'trick'. I've read that a mirror can be parabolized by heating it to a certain temperature, then polishing it to a sphere. When the mirror returns to normal temperature it has a parabolic surface. The reason for using a corrector lens is not quite as simple as it's been made out to be--note that SCTs (and even Schmidt-Newtonians) are typically more expensive than Newtonians of equivalent aperture. The driving force behind the consumer SCT, more than anything else, is its compact size, along with the location of its focal plane. It's not just a matter of convenience, but of efficiency and cost-effectiveness in performing certain tasks, such as astrophotography. In order to make an exceptionally short reflector, you need an extremely fast primary mirror--as fast as f/2 to really make it worthwhile. However, such a fast parabolic mirror, as you would use in a Classical Cassegrain (along with a hyperboloidal secondary), would have an overwhelming amount of coma. One solution to this problem is the Ritchey-Chrétien design (most large professional telescopes are of this design), which has a hyperboloidal primary and an even more hyperboloidal secondary. The problem now is that no inexpensive way to create this type of figure has yet been found, so the price for a telescope of this design that is available to amateurs currently runs about $1500-$2500 per inch of aperture. Commercial SCTs (and MCTs) are kind of like a poor man's Ritchey-Chrétien. They can't match the optical performance of a good RC telescope, but they can be just as compact, while providing reasonable correction for the various aberrations. Regarding cost, this is a more legitimate comparison than SCTs versus Newtonians, which was sort of implied earlier. - Robert Cook |
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