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Astronomy Principles and Practice Fourth Edition.pdf

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Digital photography 449<br />

Figure 24.32. Laboratory equipment for simulating Michelson’s stellar interferometer.<br />

position relative to the image plane of the objective by measuring the position of the double slit when<br />

it is viewed to be in focus in the microscope.<br />

Using the travelling microscope, obtain a mean value for the separation of the slits. By assuming<br />

the mean wavelength of the light to be 5500 Å <strong>and</strong> knowing the focal length of the objective, calculate<br />

the angular size of the artificial star using the formula<br />

α = 1·22λ<br />

a ′ min<br />

= 1·22λD min<br />

.<br />

aF<br />

As a check, calculate the actual angle subtended by measuring the physical size of the hole<br />

constituting the artificial star <strong>and</strong> the distance of the star from the objective.<br />

24.12 Digital photography<br />

The advent of two-dimensional solid state detectors has revolutionized ‘photography’. The use of<br />

digital cameras for everyday use is now fairly common. Such equipment used for l<strong>and</strong>scapes <strong>and</strong><br />

portraits automatically provides colour pictures. Some of the latest models (SLR) have detachable<br />

lenses <strong>and</strong> could, in principle, be attached at the focus of a telescope without the camera lens being<br />

attached. However, there is no facility to make long exposures <strong>and</strong>, without cooling, the recorded<br />

pictures would be very subject to thermal noise. The formatting of the files is also generally not

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