A View of Sir Isaac Newton's PhilosophyPemberton, Henry
Science
A View of Sir Isaac Newton's Philosophy
Pemberton, Henry
Newton, Isaac, 1642-1727. Principia
19. SINCE we find, that the same power will always produce the same
change in the motion of any body, whether that body were before moving
with a swifter or slower motion; the change wrought in the motion of
a body depends only on the power applied to it, without any regard to
the body’s former motion: and therefore the degree of motion, which the
body already possesses, having no influence on the power applied to
disturb its operation, the effects of the same power will not only be
the same in all degrees of motion of the body; but we have likewise no
reason to doubt, but that a body perfectly at rest would receive from
any power as much motion, as would be equivalent to the effect of the
same power applied to that body already in motion.
20. AGAIN, suppose a body being at rest, any number of equal powers
should be successively applied to it; pushing it forward from time to
time in the same course or direction. Upon the application of the first
power the body would begin to move; when the second power was applied,
it appears from what has been said, that the motion of the body would
become double; the third power would treble the motion of the body; and
so on, till after the operation of the last power the motion of the
body would be as many times the motion, which the first power gave it,
as there are powers in number. and the effect of this number of powers
will be always the same, without any regard to the space of time taken
up in applying them: so that greater or lesser intervals between the
application of each of these powers will produce no difference at all
in their effects. Since therefore the distance of time between the
action of each power is of no consequence; without doubt the effect
will still be the same, though the powers should all be applied at
the very same instant; or although a single power should be applied
equal in strength to the collective force of all these powers. Hence
it plainly follows, that the degree of motion, into which any body
will be put out of a state of rest by any power, will be proportional
to that power. A double power will give twice the velocity, a treble
power three times the velocity, and so on. The foregoing reasoning will
equally take place, though the body were not supposed to be at rest,
when the powers began to be applied to it; provided the direction, in
which the powers were applied, either conspired with the action of
the body, or was directly opposite to it. Therefore if any power be
applied to a moving body, and act upon the body either in the direction
wherewith the body moves, so as to accelerate the body; or if it act
directly opposite to the motion of the body, so as to retard it: in
both these cases the change of motion will be proportional to the
power applied; nay, the augmentation of the motion in one case, and
the diminution thereof in the other, will be equal to that degree of
motion, into which the same power would put the body, had it been at
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