Physics for Geologists, Second edition
Physics for Geologists, Second edition
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