Classics of modern science : $b (Copernicus to Pasteur)
History
Classics of modern science : $b (Copernicus to Pasteur)
Science; Science -- History
While the work in this case consists in the raising of the heavy
hammer-head, the driving force which sets the latter in motion is
generated by falling water. It is not necessary that the water should
fall vertically, it can also flow in a moderately inclined bed; but
it must always, where it has water-mills to set in motion, move from
a higher to a lower position. Experiment and theory coincided in
teaching, that when a hammer of a hundred weight is to be raised one
foot, to accomplish this at least a hundred weight of water must fall
through the space of one foot; or what is equivalent to this, two
hundred weight must fall full half a foot, or four hundred weight a
quarter of a foot, etc. In short, if we multiply the weight of the
falling water by the height through which it falls, and regard, as
before, the product as the measure of the work, then the work performed
by the machine in raising the hammer can, in the most favourable case,
be only equal to the number of foot-pounds of water which have fallen
in the same time. In practice, indeed, this ratio is by no means
attained; a great portion of the work of the falling water escapes
unused, inasmuch as part of the force is unwillingly sacrificed for the
sake of obtaining greater speed.
I will further remark, that this relation remains unchanged whether
the hammer is driven immediately by the axle of the wheel, or
whether--by the intervention of wheel-work, endless screws, pulleys,
ropes--the motion is transferred to the hammer. We may, indeed, by
such arrangements, succeed in raising a hammer of ten hundred weight,
when by the first simple arrangement, the elevation of a hammer of one
hundred weight might alone be possible; but either this heavier hammer
is raised to only one-tenth of the height, or tenfold the time is
required to raise it to the same height; so that, however we may alter,
by the interposition of machinery, the intensity of the acting force,
still in a certain time, during which the mill-stream furnishes us with
a definite quantity of water, a certain definite quantity of work, and
no more, can be performed.
Public-domain text, read in full here on John Shaqi.
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