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#11
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Henry Spencer wrote:
In article , apparently there are practical advantages in having a single filled aperture rather than a wide scattering of smaller mirrors. I suspect that apodisation is very much easier with the filled aperture. |
#12
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#13
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As somebody else mentioned, a large baseline optical interferometer is
likely to give more info for a much smaller price. So, what is th elargest baseline optical interferometer we can build? |
#14
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In article . com,
wrote: As somebody else mentioned, a large baseline optical interferometer is likely to give more info for a much smaller price. No, it depends on what sort of information you are after. In particular, optical interferometers are useless for spectroscopy and are usable for imaging only on fairly bright objects (because you need a fair number of photons per second to form detectable interference fringes). For many astronomical purposes, there is just no substitute for lots of mirror area. Current preference seems to be to build 2-4 quite large telescopes within maybe 100m of each other (e.g., the two Kecks and the four-telescope ESO), so they can be used individually for general-purpose astronomy and experimentally together for interferometry. -- "Think outside the box -- the box isn't our friend." | Henry Spencer -- George Herbert | |
#15
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Henry Spencer wrote:
In article . com, wrote: As somebody else mentioned, a large baseline optical interferometer is likely to give more info for a much smaller price. No, it depends on what sort of information you are after. In particular, optical interferometers are useless for spectroscopy and are usable for imaging only on fairly bright objects (because you need a fair number of photons per second to form detectable interference fringes). For many astronomical purposes, there is just no substitute for lots of mirror area. Erm, interferometers are not really "useless" for spectroscopy. Interferometry makes spectroscopy a whole hell of a lot more difficult, but it's still doable. If the only way to observe the target is through deep interferometric nulling, for example, then you accept the difficulties and move on. Specifically, what you want is to be able to sample the configuration space (by rotation the interferometry assembly along an axis which points at the target, for example) to a degree that allows you to create a processed, properly calibrated spectrum that you can trust. For this specific example, the collection of the spectra relies on the interferometry. This takes advantage of the deep nulling ability of interferometry to allow the observation of very dim targets close to very bright targets (e.g. planets near stars). However, in general, spectroscopy does not rely on the features of interferometry, so in most cases spectroscopy and interferometry live in different worlds. For example, while interferometry can create higher spatial resolution views, doing so necessarily lowers the surface brightness "per pixel" of the image, which is not what you want for spectroscopy (which almost always prefers more signal over finer spatial coverage). And, of course, in general the whole idea of interferometry is to use parlay a small multiple in mirror area (e.g. 2x, 5x) into a large multiple in resolution through separation (or a high degree of nulling). So, in general, as has been pointed out, most spectroscopic targets benefit more from greater light collection area than from anything else. Interestingly, there have been a lot of very innovative alternatives to interferometry in regard to deep nulling and such like which have been proposed for various projects, such as terrestrial planet finding, recently. For example, the leading contender for NASA's TPF mission is, I believe, a coronograph rather than a nulling interferometer. Reflecting, I think, the many advances in overall "old school"ish more or less classic-design type designs which have taken place in the last decade or so as well as advances in instrumentation (dynamic range, etc). Compare, for example, the sophistication and capabilities of, say, Chandra, WMAP, and Spitzer versus say Einstein, COBE, and ISO. Where once the TPF specs. were beyond the state of the art for conventional telescope technologies, those technologies are starting to catch up to the point where just a, mostly, plain jane telescope can meet the specs. As above, one of the great advantages of a coronograph style design is that it would greatly simplify spectra aquisition and improve spectra collection throughput. An even more interesting, and certainly more innovative, concept would be the gigantic pinhole camera*, which would have somewhat similar problems to an interferometer but could offer much deeper nulling and finer resolution at significantly less cost. (*) http://www1.nasa.gov/vision/universe/newworlds/new_worlds_imager.html |
#16
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![]() Henry Spencer wrote: There's no reason why you couldn't build an OWL in space, although it would be an expensive project if it used current infrastructure. Speaking of big telescopes and space, would operation in space simplify (if nothing else) the optical design of an OWL-scale segmented telescope? Mike Miller |
#17
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#18
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How about this: putting 3 or 4 Hubble-sized (for redundancy & time-use
issues) craft in Jovian Trojan orbits would give you a 10 1/2 AU-equivalent instrument! That would almost see planets in Andromeda! |
#19
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In article .com,
wrote: How about this: putting 3 or 4 Hubble-sized (for redundancy & time-use issues) craft in Jovian Trojan orbits would give you a 10 1/2 AU-equivalent instrument! That would almost see planets in Andromeda! Only if you could hold the distance between them stable to within a fraction of a wavelength of light, *and* beam the light gathered by one to another across that distance without losing much of it. That... presents problems, to put it mildly. People are still struggling to make imaging interferometry work well at distances of a hundred *meters* with both telescopes resting on solid rock. -- "Think outside the box -- the box isn't our friend." | Henry Spencer -- George Herbert | |
#20
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In article ,
Henry Spencer wrote: In article .com, wrote: How about this: putting 3 or 4 Hubble-sized (for redundancy & time-use issues) craft in Jovian Trojan orbits would give you a 10 1/2 AU-equivalent instrument! That would almost see planets in Andromeda! Only if you could hold the distance between them stable to within a fraction of a wavelength of light, *and* beam the light gathered by one to another across that distance without losing much of it. That... presents problems, to put it mildly. In principle, there's another option, analogous to the way radio astronomers do inteferometry with telescopes thousands of miles apart; it only requires that you be able to record phase information as well as brightness information. But while this means recording data at a few gigahertz for 20cm radio work, this would mean doing so at about 10^14 Hz, which also... presents problems, to put it mildly. But this particular problem may be more solvable in the long run. cheers, Steven -- "M-Theory is the unifying pachyderm of the five string theories." - Brian Greene, _The Elegant Universe_ |
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