476]
ORBIT OF A PLANET FROM THREE OBSERVATIONS.
467
given by 0 = +1 and 6 = — 1 respectively; the dotted curve on the base C'B (= C'B')
is merely the upper curve on the base C'B' transferred to the base C'B; and the
curve composed of the lower curve on the base AC' and of the dotted curve gives
by its ordinates the value of the eccentricity as the orbit-pole moves along AB'B
within the triangle B'BBthe upper curve on the base AB' gives by its ordinates
the value of the eccentricity as the orbit-pole moves along AB' on the other side
thereof, that is, within the convex region.
The base of the diagram is graduated not for the value of H, but for that of
the angular distance (or distance in longitude) of the orbit-pole from the point A
(or A'); viz. this is the angle opposite II in a right-angled spherical triangle, the sides
and hypothenuse of which are 60°, H, c; writing (3 for the angle in question we have
cos c =
and any position of the orbit-pole on the separator may be conveniently laid down by
means of this angle ¡3. The values of /3 corresponding to the before-mentioned values
A = -9592 and A = 8'073 are ¡3 = 47° 54' and /3 = 83° 53' respectively.
Article Nos. 114 and 115. The Spherogram and Isoparametric Lines—General
Considerations.
114. We first construct a blank spherogram, as already explained (and see also
Plates IV. and V.), viz., we draw on the stereographic projection a hemisphere—say
the northern hemisphere : the meridians being radii and the parallels of colatitude
circles with the pole as centre; the parallel of 60° is the regulator circle, and the
separators are great circles touching this at the points A, A, A, in longitudes 30°, 150°,
270° respectively ; the separators intersect in the points B, B, B, in the northern hemi
sphere, and they are produced to meet again in the points B, B, B, of the southern
hemisphere ; but instead of taking the whole northern hemisphere, we omit portions
thereof, and take in the opposite portions of the southern hemisphere ; the spherogram
being thus bounded by portions of the separator circles, and consisting of the inner
spherical triangle B, B, B, and three surrounding triangles B, B, B. The inner triangle
contains the regulator-circle, touching its sides at the points A, A, A respectively, and
dividing it into an inner circular region and three surrounding regions A, B, A ; these
last are the loci in quitus of the orbit-poles which correspond to convex orbits; and
to mark them off from the other regions, it is proper to shade them in the sphero
gram. Excluding them from consideration, we have the inner circular region and the
outer triangular regions separated off from each other by the shaded regions, except
at the points A, where these are thinned away to nothing. The points A are positions
of the orbit-pole for which the orbit is indeterminate ; and consequently any parameter
belonging to the orbit is also indeterminate. Hence the isoparametric line for any
given value of the parameter will always pass through the points A ; that is, all the
isoparametric lines will pass through these points, which are thus points of connexion
59—2