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Astronomy Principles and Practice Fourth Edition.pdf

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The Schmidt telescope 339<br />

Wavefronts<br />

(a)<br />

Focal plane<br />

(b)<br />

Focal plane<br />

Single star<br />

pattern<br />

Star 2<br />

Star 1<br />

Figure 20.6. The production of speckle patterns for (a) a single <strong>and</strong> (b) a close double star.<br />

20.4 The Schmidt telescope<br />

Improvements in wide-field photography over astrographic refractor systems were contemplated by<br />

considering the use of specially designed reflector cameras. The simplest system would consist of a<br />

single spherical mirror with an aperture stop at its centre of curvature. Such a camera has no unique<br />

axis <strong>and</strong> any point in the field would be imaged equally well—the focal surface would be curved, with<br />

a radius given by the focal length of the mirror.<br />

When such simple camera systems are designed to have smaller focal ratios than those of the<br />

fastest astrographic refractors, the images suffered severely from spherical aberration. Many ways<br />

were suggested whereby this aberration might be reduced but it was not until the 1930s that a design<br />

was successfully manufactured by Schmidt in Hamburg. The system made by Schmidt was similar, in<br />

principle, to an optical device for a good quality parallel light source suggested <strong>and</strong> patented by Kellner<br />

some 20 years previously.<br />

The Schmidt telescope is basically a two-element system, whereby the spherical aberration<br />

produced by the spherical collecting mirror is compensated by using a thin aspherical correcting lens<br />

or plate at the centre of curvature of the mirror. There is a range of shapes that the corrector lens can<br />

take. The basic parts are depicted in figure 20.7 in which the departure of correcting lens from being a<br />

parallel plate is greatly exaggerated. It is usual practice to make no effort to correct for the curvature of<br />

the focal surface <strong>and</strong> specially produced photographic plates or film are required to match the curvature<br />

of the surface of best focus of the camera. Since the introduction of the basic design, improvements<br />

have been suggested <strong>and</strong> investigated which use more elements in the optical system but these will not<br />

be discussed here. Schmidt cameras can have focal ratios of f/1·0 or smaller <strong>and</strong> can provide field

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