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
Moreover, in a system of two bodies mutually acting upon each other,
since the distances between their centres and the common centre of
gravity of both are reciprocally as the bodies, the relative motions
of those bodies, whether of approaching to or of receding from that
centre, will be equal among themselves. Therefore since the changes
which happen to motions are equal and directed to contrary parts,
the common centre of those bodies, by their mutual action between
themselves, is neither promoted nor retarded, nor suffers any change
as to its state of motion or rest. But in a system of several bodies,
because the common centre of gravity of any two acting mutually upon
each other suffers no change in its state by that action; and much less
the common centre of gravity of the others with which that action does
not intervene; but the distance between those two centres is divided by
the common centre of gravity of all the bodies into parts reciprocally
proportional to the total sums of those bodies whose centres they are;
and therefore while those two centres retain their state of motion
or rest, the common centre of all does also retain its state: it is
manifest that the common centre of all never suffers any change in the
state of its motion or rest from the actions of any two bodies between
themselves. But in such a system all the actions of the bodies among
themselves either happen between two bodies, or are composed of actions
interchanged between some two bodies; and therefore they do never
produce any alteration in the common centre of all as to its state of
motion or rest. Wherefore since that centre, when the bodies do not act
mutually one upon another, either is at rest or moves uniformly forward
in some right line, it will, notwithstanding the mutual actions of the
bodies among themselves, always persevere in its state, either of rest,
or of proceeding uniformly in a right line, unless it is forced out
of this state by the action of some power impressed from without upon
the whole system. And therefore the same law takes place in a system
consisting of many bodies as in one single body, with regard to their
persevering in their state of motion or of rest. For the progressive
motion, whether of one single body, or of a whole system of bodies is
always to be estimated from the motion of the centre of gravity.
COROLLARY V.
[Pg 89]
The motions of bodies included in a given space are the same among
themselves, whether that space is at rest, or moves uniformly forwards
in a right line without any circular motion.
Public-domain text, read in full here on John Shaqi.
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