Illustrations of the Huttonian Theory of the EarthPlayfair, John
Science
Illustrations of the Huttonian Theory of the Earth
Playfair, John
Geology; Hutton, James, 1726-1797. Theory of the earth
The effect of the inequalities of the land, that rise above the
horizontal surface, is, by their attraction, to render the parts of
that surface immediately under them, more convex, _cæteris paribus_,
than the rest. Again, where there are parts of extraordinary depth in
the sea, that is, where the solid and denser parts are far removed from
the surface of the ocean, the curvature of the superficies of the sea
is thereby diminished, and that superficies is rendered less convex
than it would be if the sea were shallower. These propositions are both
capable of strict mathematical demonstration. Hence the taking away of
any particle of matter from the top of a mountain tends to diminish the
curvature of the horizontal surface under the mountain, where it is
greatest; and the deposition of the same particle at the bottom of the
sea, tends to increase the curvature of this superficies where it is
least. The general tendency, therefore, being to increase the curvature
where it is least, and to diminish it where it is greatest, must be
to bring about an uniform curvature throughout, that is, a spherical
figure. Thus, by the waste and subsequent stratification of the land,
the direction of gravity is continually altered; it is more and more
concentrated, and the figure brought nearer to that which a fluid would
assume.
439. If now we suppose the body to revolve on its axis, all other
things remaining as before, the surface bounding the sea will become
different from what it was in the former case, and will be more swelled
out toward the middle or equatorial regions. The land above the level
of the sea will still, as before, be worn down and deposited in the
bottom of the sea, so as to form strata nearly parallel to its surface:
the tendency, therefore, is to render the real figure of the planet
nearer to the statical. At the same time the _statical_ figure is
changed, as explained above; so that the two figures mutually approach,
and the limit, or ultimate figure to which they tend, is one over which
the ocean might be diffused every where to the same depth, for then the
causes of change would entirely cease. But this figure is no other than
the spheroid of equilibrium, which, therefore, is the effect which the
waste and reconsolidation of the land would necessarily produce, if the
process were continued indefinitely, without interruption. In this, as
in many other instances, when a body is subject to the action of causes
by which its form is _gradually_ changed, the figure best adapted
to resist those changes, is the figure which the changes themselves
ultimately produce.
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