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Physics for Geologists, Second edition

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39 40 41 42 43<br />

Angle from centre of rainbow<br />

Optics 55<br />

Figure 4.8 Angles of light scattered back from a raindrop. The proportion of<br />

the radius at entry is the sine of the angle of incidence, so the cusp<br />

of the curve, where the scattered light is most concentrated, comes<br />

from the rays with an angle of incidence between about 58" and 60".<br />

colours of different frequencies and wavelengths are refracted at slightly<br />

different angles, as from a prism. The red is returned at an angle of about<br />

43", while the violet is returned at an angle of about 40.5" - putting red on<br />

the outside of the rainbow, and violet on the inside.<br />

This is what Descartes found. The only difference is that he would have<br />

taken very much longer to draw his lines.<br />

Rainbows can only be seen by an observer on flat ground when the sun is<br />

low in the sky, beginning with an elevation of less than 40". Standing on top<br />

of the Matterhorn, rainbows can be seen when the sun is higher, and they<br />

can be more complete with your shadow at the centre. A complete circle can<br />

be seen from an aeroplane, when the shadow of the aeroplane is at the centre<br />

of the circle.<br />

The light reflected at the exit point of the primary rainbow and refracted at<br />

the next internal surface sometimes gives rise to another but weaker rainbow<br />

at about 52". In this one, the colours are reversed because of the second<br />

internal reflection.<br />

Stereoscopy<br />

We see things in three dimensions because our brain has the capacity to<br />

fuse the image each eye receives into one, each eye seeing a slightly different<br />

image from its slightly different position. Use is made of this in binoculars,<br />

binocular microscopes and in the making of maps from aerial photographs.<br />

Photographs are taken sequentially from an aircraft flying at a constant<br />

height with the camera pointing vertically downwards, with about 60 per<br />

cent overlap between photographs. Adjacent pairs can be viewed stereo-<br />

scopically through a stereoscope (see Figure 4.9), and a 3-D image of the<br />

common ground in the two photographs is seen. It is as if one eye was in the<br />

position from which the first photograph was taken, the other in the next.<br />

Copyright 2002 by Richard E. Chapman

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