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
PROJECTILES persevere in their
motions, so far as they are not retarded by the resistance of the air,
or impelled downwards by the force of gravity. A top, whose parts by
their cohesion are perpetually drawn aside from rectilinear motions,
does not cease its rotation, otherwise than as it is retarded by the
air. The greater bodies of the planets and comets, meeting with less
resistance in more free spaces, preserve their motions both progressive
and circular for a much longer time.
LAW II.
The alteration of motion is ever proportional to the motive force
impressed; and is made in the direction of the right line in which that
force is impressed.
If any force generates a motion, a double force will generate double
the motion, a triple force triple the motion, whether that force be
impressed altogether and at once, or gradually and successively. And
this motion (being always directed the same way with the generating
force), if the body moved before, is added to or subducted from the
former motion, according as they directly conspire with or are directly
contrary to each other; or obliquely joined, when they are oblique, so
as to produce a new motion compounded from the determination of both.
LAW III.
To every action there is always opposed an equal reaction: or the
mutual actions of two bodies upon each other are always equal, and
directed to contrary parts.
Whatever draws or presses another is as much drawn or pressed by that
other. If you press a stone with your finger, the finger is also
pressed by the stone. If a horse draws a stone tied to a rope, the
horse (if I may so say) will be equally drawn back towards the stone:
for the distended rope, by the same endeavour to relax or unbend
itself, will draw the horse as much towards the stone, as it does the
stone towards the horse, and will obstruct the progress of the one as
much as it advances that of the other.[Pg 84] If a body impinge upon another,
and by its force change the motion of the other, that body also
(because of the equality of the mutual pressure) will undergo an equal
change, in its own motion, towards the contrary part. The changes made
by these actions are equal, not in the velocities but in the motions
of bodies; that is to say, if the bodies are not hindered by any
other impediments. For, because the motions are equally changed, the
changes of the velocities made towards contrary parts are reciprocally
proportional to the bodies. This law takes place also in attractions,
as will be proved in the next scholium.
COROLLARY I.
A body by two forces conjoined will describe the diagonal of a
parallelogram, in the same time that it would describe the sides, by
those forces apart.
Public-domain text, read in full here on John Shaqi.
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