If perturbations are ignored, a planet can be regarded as moving in an
ellipse with the sun in one focus. The size and shape of the ellipse
can be defined by the length of its axis and by the eccentricity; the
plane in which the ellipse is situated is determined by the position of
the line, called the line of =nodes=, in which it cuts a fixed plane,
usually taken to be the ecliptic, and by the inclination of the two
planes. When these four quantities are fixed, the ellipse may still
turn about its focus in its own plane, but if the direction of the apse
line is also fixed the ellipse is completely determined. If, further,
the position of the planet in its ellipse at any one time is known, the
motion is completely determined and its position at any other time can
be calculated. There are thus six quantities known as =elements= which
completely determine the motion of a planet not subject to perturbation.
When perturbations are taken into account, the path described by
a planet in any one revolution is no longer an ellipse, though it
differs very slightly from one; while in the case of the moon the
deviations are a good deal greater. But if the motions of a planet at
two widely different epochs are compared, though on each occasion the
path described is very nearly an ellipse, the ellipses differ in some
respects. For example, between the time of Ptolemy (A.D. 150) and that
of Euler the direction of the apse line of the earth’s orbit altered by
about 5°, and some of the other elements also varied slightly. Hence
in dealing with the motion of a planet through a long period of time
it is convenient to introduce the idea of an elliptic path which is
gradually changing its position and possibly also its size and shape.
One consequence is that the actual path described in the course of a
considerable number of revolutions is a curve no longer bearing much
resemblance to an ellipse. If, for example, the apse line turns round
uniformly while the other elements remain unchanged, the path described
is like that shewn in the figure.
[Illustration: FIG. 81.—A varying ellipse.]
Public-domain text, read in full here on John Shaqi.
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