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
For action and its opposite re-action are equal, by Law III, and
therefore, by Law II, they produce in the motions equal changes towards
opposite parts. Therefore if the motions are directed towards the same
parts, whatever is added to the motion of the preceding body will be
subducted from the motion of that which follows; so that the sum will
be the same as before. If the bodies meet, with contrary motions, there
will be an equal deduction from the motions of both; and therefore the
difference of the motions directed towards opposite parts will remain
the same.
Thus if a spherical body A with two parts of velocity is triple of a
spherical body B which follows in the same right line with ten parts
of velocity, the motion of A will be to that of B as 6 to 10. Suppose,
then, their motions to be of 6 parts and of 10 parts, and the sum will
be 16 parts. Therefore, upon the meeting of the bodies, if A acquire
3, 4, or 5 parts of motion, B will lose as many; and therefore after
reflexion A will proceed with 9, 10, or 11 parts, and B with 7, 6, or
5 parts; the sum remaining always of 16 parts as before. If the body A
acquire 9, 10, 11, or 12 parts of motion, and therefore after meeting
proceed with 15, 16, 17, or 18 parts, the body B, losing so many parts
as A has got, will either proceed with 1 part, having lost 9, or stop
and remain at rest, as having lost its whole progressive motion of
10 parts; or it will go back with 1 part, having not only lost its
whole motion, but (if I may so say) one part more; or it will go back
with 2 parts, because a progressive motion of 12 parts is taken off.
And so the sums of the conspiring motions 15 + 1, or 16 + 0, and the
differences of the contrary motions 17 - 1 and[Pg 87] 18 - 2, will always be
equal to 16 parts, as they were before the meeting and reflexion of
the bodies. But, the motions being known with which the bodies proceed
after reflexion, the velocity of either will be also known, by taking
the velocity after to the velocity before reflexion, as the motion
after is to the motion before. As in the last case, where the motion
of the body A was of 6 parts before reflexion and of 18 parts after,
and the velocity was of 2 parts before reflexion, the velocity thereof
after reflexion will be found to be of 6 parts; by saying, as the 6
parts of motion before to 18 parts after, so are 2 parts of velocity
before reflexion to 6 parts after.
Public-domain text, read in full here on John Shaqi.
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