Buffon's Natural History, Volume 01 (of 10): Containing a Theory of the Earth, a General History of Man, of the Brute Creation, and of Vegetables, Mineral, &c. &cBuffon, Georges Louis Leclerc, comte de
History
Buffon's Natural History, Volume 01 (of 10): Containing a Theory of the Earth, a General History of Man, of the Brute Creation, and of Vegetables, Mineral, &c. &c
Buffon, Georges Louis Leclerc, comte de
Natural history
cause the rapidity of the river to increase, and perhaps move it at
bottom; for it is known, that by putting many boats at one time into the
water, at that instant we increase the rapidity of the under part of the
river, as well as retard that of the upper.
The rapidity of running waters does not exactly, nor even nearly, follow
the proportion of the declivity of their channels. One river whose
inclination is uniform and double that of another, ought, according to
appearance, to flow only as rapid again, but in fact it flows much
faster. Its rapidity, instead of being doubled, is sometimes triple,
quadruple, &c. This rapidity depends much more on the quantity of water
and the weight of the upper waters than on the declivity. When we are
desirous to hollow the bed of a river, we need not equally distribute
the inclination throughout its whole length, in order to give a greater
rapidity, as it is more easily effected by making the descent much
greater at the beginning, than at the mouth, where it may almost be
insensible, as we see it in natural rivers, and yet they preserve a
rapidity so much the greater as the river is fuller of water; in great
rivers, where the ground is level, the water does not cease flowing, and
even rapidly, not only with its original velocity, but also with the
addition of that which it has acquired by the action and weight of the
upper waters. To render this fact more conceivable, let us suppose the
Seine between the Pont-neuf and Pont-royal to be perfectly level, and
ten feet deep throughout: let us then suppose that the bed of the river
below Pont-royal and above Pont-neuf were left entirely dry, the water
would instantly run up and down the channel, and continue to do so until
it had recovered an equilibrium; for the weight of the water would keep
it in motion, nor would it cease flowing until its particles became
equally pressed and have sunk to a perfect level. The weight of water
therefore greatly contributes to its velocity, and this is the reason
that the greatest rapidity of the current is neither of the surface nor
at the bottom of the water, but nearly in the middle of its depth, being
pressed by the action of its weight at its surface, and by the re-action
from the bottom. Still more, if a river has acquired a great rapidity,
it will not only preserve it in passing a level country, but even
surmount an eminence without spreading much on either side, or at least
without causing any great inundation.
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