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
COR. 3. If the chords AB, BC, and DE, EF, of arcs described in
equal[Pg 105] times, in spaces void of resistance, are completed into the
parallelograms ABCV, DEFZ; the forces in B and E are one to the other
in the ultimate ratio of the diagonals BV, EZ, when those arcs are
diminished in infinitum. For the motions BC and EF of the body
(by Cor. 1 of the Laws) are compounded of the motions Bc, BV,
and Ef, EZ: but BV and EZ, which are equal to Cc and
Ff, in the demonstration of this Proposition, were generated by
the impulses of the centripetal force in B and E, and are therefore
proportional to those impulses.
COR. 4. The forces by which bodies, in spaces void of resistance,
are drawn back from rectilinear motions, and turned into curvilinear
orbits, are one to another as the versed sines of arcs described in
equal times; which versed sines tend to the centre of force, and bisect
the chords when those arcs are diminished to infinity. For such versed
sines are the halves of the diagonals mentioned in Cor. 3.
COR. 5. And therefore those forces are to the force of gravity as the
said versed sines to the versed sines perpendicular to the horizon of
those parabolic arcs which projectiles describe in the same time.
COR. 6. And the same things do all hold good (by Cor. 5 of the Laws),
when the planes in which the bodies are moved, together with the
centres of force which are placed in those planes, are not at rest, but
move uniformly forward in right lines.
PROPOSITION II. THEOREM II.
Every body that moves in any curve line described in a plane, and
by a radius, drawn to a point either immovable, or moving forward
with an uniform rectilinear motion, describes about that point areas
proportional to the times, is urged by a centripetal force directed to
that point.
CASE. 1. For every body that moves in a curve line, is (by Law I)
turned aside from its rectilinear course by the action of some force
that impels it. And that force by which the body is turned off from
its rectilinear course, and is made to describe, in equal times, the
equal least triangles SAB, SBC, SCD, &c., about the immovable point
S (by Prop. XL. Book I, Elem. and Law II), acts in the place B,
according to the direction of a line parallel[Pg 106] to cC, that is,
in the direction of the line BS, and in the place C, according to the
direction of a line parallel to dD, that is, in the direction of
the line CS, &c.; and therefore acts always in the direction of lines
tending to the immovable point S. Q.E.D.
CASE. 2. And (by Cor. 5 of the Laws) it is indifferent whether the
superfices in which a body describes a curvilinear figure be quiescent,
or moves together with the body, the figure described, and its point S,
uniformly forward in right lines.
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