By Raymond N. Wilson

ISBN-10: 3642082238

ISBN-13: 9783642082238

ISBN-10: 3662084880

ISBN-13: 9783662084885

This quantity is worried primarily with the trendy advancements in reflecting telescope optics. within the final 20 years, sleek know-how has revolutionized not just production and attempt strategies but in addition the total quarter of caliber specification with the advent of energetic keep watch over into the functioning telescope. different topics coated listed below are alignment of telescope optics, atmospheric optics, together with adaptive optics, reflecting coatings and ancillary apparatus (adapters and baffles). even though an autonomous paintings, Vol. II is seriously cross-referenced with Vol. I. it truly is richly illustrated and provides, including Vol. I, the main entire record of references on hand; it will probably additionally for that reason be considered as a resource book.

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Extra info for Reflecting Telescope Optics II: Manufacture, Testing, Alignment, Modern Techniques

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4 reproduces results quoted for six segments before and after correction with the warping harness. 52 arcsec. 4. 1992. 58]. The conclusions will be discussed furt her in Chap. 3. At that time, it appeared that stress polishing could be highly successful with circular elements, either axisymmetric or off-axis, but that the problems with non-circular segments were not fully solved. Subsequently, they were effectively solved by the technique of ion beam figuring, discussed in the next section. 5 Ion beam figuring (IBF).

74]) = 2t = m>.. 25) where a is the wedge angle, y is the distance from the intersection line of the planes, t the separation and m an integer. Dark fringes result from the phase change at the air-glass surface. The only difference, physically, in the Fizeau compared with the Newton form, is that the air gap is much larger so that the order of the fringes m is much higher. This makes the practical work simpler by avoiding surface contact, but requires a collimated system with a pinhole source. The Newton arrangement with an appreciable source size falsifies the fringe pattern if m is large because Eq.

Positions are sensed by encoders, and speeds of all three motors are updated about 20 times a second. A cyde of polishing strokes is determined by computer simulation to establish a desired removal function. Aseparate microcomputer controls the shape of the lap. 41] using a Jull-size stressed lap. 2 m WHT. The limitation of such a passive deformation proportional to p4, where p is the zonal radius, to give the required asphericity as third order spherical aberration, is that an excentric position (overhang) of the tool due to the polishing stroke produces amismatch which is, to a first approximation, the differential of the function, Le.

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Reflecting Telescope Optics II: Manufacture, Testing, Alignment, Modern Techniques by Raymond N. Wilson


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