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
This force is ever proportional to the body whose force it is; and
differs nothing from the inactivity of the mass, but in our manner of
conceiving[Pg 74] it. A body, from the inactivity of matter, is not without
difficulty put out of its state of rest or motion. Upon which account,
this vis insita, may, by a most significant name, be called
vis inertiæ, or force of inactivity. But a body exerts this
force only, when another force, impressed upon it, endeavours to change
its condition; and the exercise of this force may be considered both
as resistance and impulse; it is resistance, in so far as the body,
for maintaining its present state, withstands the force impressed; it
is impulse, in so far as the body, by not easily giving way to the
impressed force of another, endeavours to change the state of that
other. Resistance is usually ascribed to bodies at rest, and impulse to
those in motion; but motion and rest, as commonly conceived, are only
relatively distinguished; nor are those bodies always truly at rest,
which commonly are taken to be so.
DEFINITION IV.
An impressed force is an action exerted upon a body, in order to
change its state, either of rest, or of moving uniformly forward in a
right line.
This force consists in this action only; and remains no longer in the
body, when the action is over. For a body maintains every new state
it acquires, by its vis inertiæ only. Impressed forces are of
different origins; as from percussion, from pressure, from centripetal
force.
DEFINITION V.
A centripetal force is that by which bodies are drawn or impelled,
or any way tend, towards a point as to a centre.
Public-domain text, read in full here on John Shaqi.
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