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Astronomy Principles and Practice Fourth Edition.pdf

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Visual resolving power 275<br />

Figure 17.3. The upper frame is by a ground-based telescope of a star field. A section of this has been observed<br />

by the HST telescope. The lower right frame is further magnified <strong>and</strong>, without the effects of atmospheric seeing,<br />

clearly shows the telescope diffraction pattern imposed on the brighter stellar images. The circles indicate the<br />

positions of very faint stars. (By courtesy of STScI.)<br />

empirical criterion gives resolving powers which are typically about 20% better than Rayleigh’s<br />

theoretical criterion. Thus, to a very good approximation, Dawes’ resolving power can be written<br />

as<br />

α = 115<br />

D<br />

where α is in seconds of arc when D is expressed in mm.<br />

In practice, the clarity of separation of two stars depends on many factors including the seeing<br />

conditions, the amount of scattered or background light, the relative brightnesses of the two stars <strong>and</strong><br />

the apparent colours of the stars.<br />

For a reflector telescope, the diffraction pattern corresponding to a point object is influenced <strong>and</strong><br />

made more complicated by the central obscuration <strong>and</strong> the spider which supports the secondary mirror.<br />

The effects are sometimes apparent on long exposed photographs of star fields, where the very bright<br />

stars exhibit a cross-like pattern as depicted in figure 17.3.

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