CHAPTER XVII
CONCLUSION
385. Now that the detailed discussion of particular problems is ended, we
may perhaps attempt to summarise our results and tentative conclusions,
sacrificing logical and chronological order in favour of the arrangement which
offers the broadest and simplest view of the whole subject.
The easiest part of the problem of cosmogony is the interpretation of the
observed shapes of astronomical bodies and formations. Here the effects of
rotation have proved to be of primary importance. The earth and many of the
planets have the shape of flattened oranges. The degree of flattening is such
as would be produced by quite slow rotation about an axis, and there is no
room for doubt that this is the actual cause of the observed flattening. It is
possible to trace out theoretically the shapes assumed by astronomical bodies
having all possible amounts of rotation. Mathematical investigation shews
that the flattened-orange shape is assumed by all bodies in slow rotation, no
matter what their internal constitution and arrangement may be, but that
with more rapid rotation the shape depends on the internal arrangement of the
body, being especially affected by the extent to which its mass is concentrated
at or near its centre.
Two special and quite extreme types of arrangement have been considered
in detail. In the first the body is supposed to consist of matter which cannot
be compressed and is of uniform density throughout; to fix our ideas, we
may think of a mass of water. As the rotation of such a mass increases, the
orange becomes flatter and flatter but retains the shape of an oblate spheroid
throughout, until a stage is reached beyond which the flattening cannot go.
At this stage the body abandons its circular cross-section; it elongates and
concentrates its mass around one of the diameters in its equatorial plane,
thus forming an ellipsoid with three unequal axes. This process continues until
the mass forms a cigar-shaped figure with a length equal to nearly three times
its shorter diameter. At this point the mass begins to concentrate about two
distinct points on its longest diameter, a furrow or waist forming near the
centre which continually deepens until it cuts the body into two distinct
detached masses. These rotate in orbital motion about one another like the
earth and moon, except that the two masses are more nearly equal and are
closer together.
It is possible for a single rotating mass to assume all these configura
tions in turn. The concept, first introduced by Laplace, of a mass shrinking
and at the same time increasing its speed of rotation, because its rotational
momentum must remain constant, remains of the utmost importance to
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