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| subject: | Re: ATM Ultimate Optical Capability, A possible Mathematical Model Expe |
From: "mommoteandcoyote" To: "Sidor . Kurt" Cc: Reply-To: "mommoteandcoyote" Kurt, How large can I print..."*WOW!!!!"* Now this is getting real interesting. Fine work... And now ...the scrutiny Coyot‚ ----- Original Message ----- From: "Sidor . Kurt" To: Sent: Monday, January 13, 2003 12:28 PM Subject: Re: ATM Ultimate Optical Capability, A possible Mathematical Model Experiment > > Dear List, > > At my current job I have been designing optical encoders utilizing > diffractive optics principals. I have numerous Mathcad files utilizing > Fresnel and Fraunhoffers models for simulating diffractive effects. With > slight dimensional scaling I have run a few simulations of Raleighs and > Dawes criterions for an ATM size 6" diameter aperture case. > > Lambda = 550 nM (0.00022") wavelength of light > D = 6 inches, mirror diameter > > Raleigh Criterion: "Stars are said to be "just resolved" when the center of > one Airy disc falls upon the first minimum of the second Airy disc" > (according to Hect, OPTICS, third edition) > > For a 6" diameter 1.22*Labmda/D = 0.92 arcseconds > > Dawes says stars can be resolved at 4.5/D seconds of arc, or in our case > 0.77 arcseconds. (Smith, MODERN OPTICAL ENGINEERING) > > I plotted some Mathcad graphs of Fraunhoffer diffraction patterns separated > at these spacings of 0.92 and 0.77 arcseconds respectively. > > The results can be seen here: > > http://images.andale.com/f2/115/106/3663062/1042483409819_RALEIGHDAWES1.JPG > > The separate Airy disc intensities are plotted on the left with the > mathematical summations plotted to the right. > The Raleigh separation shows a "contrast" of 28% change in the intensity > from the brightest peak of one Airy disc to the dimmer "shade of gray" that > resolves it from the next one. Due to the slope of the Airy discs central > bright core when you reduce the spacing from 0.92 arcseconds to 0.77 > arcseconds this intensity "contrast" reduces to only a 4% difference from > the brightes peak to the "shade of gray". This result implies that a > "contrast" change as small as 4% could be detected by Dawes defining his > "limit". > > I then created a new model of summing the intensities of 100 Airy discs > defining an object 5 arcseconds wide for the same Fraunhoffer pattern > created by a 6" aperture. This was identical to the previous model using > only two to define two stars but now I am creating an "extended" object by > mathematically putting them all next to eachother. Then I removed one of > the sections in the middle of my source simulating a dark line 0.05 > arcseconds wide. The resulting change in the surface intesity of my 5 > arcsecond object was a 6% "contrast" change. This contrast change is > greater then what the Dawes criterion of 4% contrast needs as a minimum. > > The plot of this dark line (0.05 seconds wide) against a 5 arcsecond object > can be seen here: > > http://images.andale.com/f2/115/106/3663062/1042483417451_RALEIGHDAWES2.JPG > > This does not imply that a 6" telescope can "resolve" (as one would > classically use the word) 0.05 arcseconds but it does imply that one could > detect the prescence of a dark feature that small against a brighter > background although its "gray" width would be quite subtle. I would guess > that Martian "canals" would fall into this category. > > Before I created my model of an "extended" object 5 arcseconds wide, I tried > using smaller objects. I tried 1.8 arseconds, twice the Raleigh criteria. > My results were poor and I could not "resolve" dark features against it. I > believe the cause of this is the slope of the central bright spot in the > Airy disc. This slope itself is too wide and my "extended" object of only > 1.8 arcseconds would not create a "plateu" of uniform "flat" light intensity > across its middle width, it just looked like a wide Airy disc. In other > words the diffractive edge effects washed out the small features because > they were too close to the edge of the object to be "resolvable". You need > to be some finite distance in from the edge before any change in contrast > can be detected. I then increased my width to 5 seconds of arc and got a > good looking "flat" plateu. > > Any thoughts? This is all just a mathematical model, I lack the personal > experience of being an experienced observer of things like Saturns ring > divisions or Martian canals. I'm just an engineer who's worked with > diffraction too much in the last few years. > > Regards, > > Kurt Sidor > Mechanical Engineer > Dynamics Research Corp. > Encoder Division > > > > > > --- BBBS/NT v4.00 MP* Origin: Email Gate (1:379/1.100) SEEN-BY: 633/267 270 @PATH: 379/1 633/267 |
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