Newton's Principia : $b The mathematical principles of natural philosophyNewton, Isaac
General
Newton's Principia : $b The mathematical principles of natural philosophy
Newton, Isaac
Celestial mechanics -- Early works to 1800; Mechanics -- Early works to 1800
The causes by which true and relative motions are distinguished, one
from the other, are the forces impressed upon bodies to generate
motion. True motion is neither generated nor altered, but by some force
impressed upon the body moved; but relative motion may be generated or
altered without any force impressed upon the body. For it is sufficient
only to impress some force on other bodies with which the former is
compared, that by their giving way, that relation may be changed, in
which the relative rest or motion of this other body did consist.
Again, true motion suffers always some change from any force impressed
upon the moving body; but relative motion does not necessarily undergo
any change by such forces. For if the same forces are likewise
impressed on those other bodies, with which the comparison is made,
that the relative position may be preserved, then that condition will
be preserved in which the relative motion consists. And therefore any
relative motion may be changed when the true motion remains unaltered,
and the relative may be preserved when the true suffers some change.
Upon which accounts, true motion does by no means consist in such
relations.
The effects which distinguish absolute from relative motion are, the
forces of receding from the axis of circular motion. For there are
no such forces in a circular motion purely relative, but in a true
and absolute circular motion, they are greater or less, according to
the quantity of the[Pg 81] motion. If a vessel, hung by a long cord, is so
often turned about that the cord is strongly twisted, then filled with
water, and held at rest together with the water; after, by the sudden
action of another force, it is whirled about the contrary way, and
while the cord is untwisting itself, the vessel continues for some
time in this motion; the surface of the water will at first be plain,
as before the vessel began to move; but the vessel, by gradually
communicating its motion to the water, will make it begin sensibly to
revolve, and recede by little and little from the middle, and ascend
to the sides of the vessel, forming itself into a concave figure (as
I have experienced), and the swifter the motion becomes, the higher
will the water rise, till at last, performing its revolutions in the
same times with the vessel, it becomes relatively at rest in it. This
ascent of the water shows its endeavour to recede from the axis of its
motion; and the true and absolute circular motion of the water, which
is here directly contrary to the relative, discovers itself, and may be
measured by this endeavour. At first, when the relative motion of the
water in the vessel was greatest, it produced no endeavour to recede
from the axis; the water showed no tendency to the circumference, nor
any ascent towards the sides of the vessel, but remained of a plain
surface, and therefore its true circular motion had not yet begun. But
afterwards, when the relative motion of the water had decreased, the
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