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. 8. But since the progress or regress of the apsides depends upon
the decrease of the centripetal force, that is, upon its being in a
greater or less ratio than the duplicate ratio of the distance TP, in
the passage of the body from the lower apsis to the upper; and upon a
like increase in its return to the lower apsis again; and therefore
becomes greatest where the proportion of the force at the upper apsis
to the force at the lower apsis recedes farthest from the duplicate
ratio of the distances inversely; it is plain, that, when the apsides
are in the syzygies, they will, by reason of the subducting force KL
or NM - LM, go forward more swiftly; and in the quadratures by the
additional force LM go backward more slowly. Because the velocity of
the progress or slowness of the regress is continued for a long time;
this inequality becomes exceedingly great.
COR. 9. If a body is obliged, by a force reciprocally proportional to
the square of its distance from any centre, to revolve in an ellipsis
round that centre; and afterwards in its descent from the upper apsis
to the lower apsis, that force by a perpetual accession of new force is
increased in more than a duplicate ratio of the diminished distance; it
is manifest that the body, being impelled always towards the centre by
the perpetual accession of this new force, will incline more towards
that centre than if it were urged by that force alone which decreases
in a duplicate ratio of the diminished distance, and therefore will
describe an orbit interior to that elliptical orbit, and at the lower
apsis approaching nearer to the centre than before. Therefore the orbit
by the accession of this new force will become more eccentrical. If
now, while the body is returning from the lower to the upper apsis, it
should decrease by the same degrees by which it increases before the
body would return to its first distance: and therefore[Pg 208] if the force
decreases in a yet greater ratio, the body, being now less attracted
than before, will ascend to a still greater distance, and so the
eccentricity of the orbit will be increased still more. Therefore if
the ratio of the increase and decrease of the centripetal force be
augmented each revolution, the eccentricity will be augmented also;
and, on the contrary, if that ratio decrease, it will be diminished.
Public-domain text, read in full here on John Shaqi.
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