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Astronomy Principles and Practice Fourth Edition.pdf

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328 Astronomical optical measurements<br />

PM<br />

Antichopper<br />

Photographic<br />

plate<br />

Neutral density<br />

wedge<br />

Lamp<br />

Figure 19.14. The schematics of a microdensitometer shows two light beams, one passing through the<br />

photographic plate, the other passing through a neutral density wedge. The beams are alternately detected by<br />

a photomultiplier. As the plate is scanned, any difference in intensity of the two beams causes movement of<br />

the neutral density wedge to restore the balance. The movement of the wedge is drawn out as a graph with the<br />

horizontal axis matching the movement of the plate.<br />

be converted to intensity values. There are several laboratory instruments which enable analysis of<br />

spectrograms to be made <strong>and</strong> the brief description of one of them, the automatic microdensitometer,<br />

is given here.<br />

The microdensitometer has an adjustable carriage onto which the photographic plate is placed<br />

(see figure 19.14). A projector lamp, followed by an optical system, illuminates a small area of the<br />

plate <strong>and</strong> light passing through the plate is collected by a microscope. The image produced by the<br />

microscope is projected on to a slit <strong>and</strong> light accepted by it is made to fall on to a photomultiplier. The<br />

current produced by the cell, therefore, corresponds to the transparency of the area of the plate which<br />

has been selected by the slit.<br />

The same projector in the instrument also provides a beam of light which is made to pass through<br />

part of a neutral density wedge. This wedge is made of glass having a density which increases<br />

linearly along its length. After passing through the plate, this beam is made to fall on to the same<br />

photomultiplier as above.<br />

By a chopping mechanism, the photomultiplier is allowed to see each beam in turn. If the<br />

density of the part of the wedge through which the second beam is passing does not match that of<br />

the investigated area of the photographic plate, an error signal is generated. This is made to control a<br />

servo-system which drives the position of the wedge until a match is achieved between the two beams.<br />

Thus, the density of the investigated part of a plate can be read off according to the position of the<br />

density wedge.<br />

Automatic spatial surveys, such as scans through the length of the spectrum, can be effected by<br />

driving the carriage supporting the photographic plate <strong>and</strong> linking the motion to a second table which<br />

is made to pass under the density wedge. A pen attachment to the wedge allows the density variations<br />

to be drawn out automatically on a graph carried by the second table.

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