[158
158]
A SIXTH MEMOIR UPON QUANTICS.
587
adrantal
distance
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ith the
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and in
ents of
to such
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listance
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or the
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e case
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le, the
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istance
ad we
îe, viz.
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pole
zero,
216. These properties of the circle lead immediately to the analytical expressions
for the distances of points or lines in terms of the coordinates. In fact, take
{a, b, c, /, g, hjx, y, zf = 0
for the point-equation of the Absolute; its line-equation will be
(a §, mm y, &=q.
The point-equation of the circle having the point (x', y', z') for its centre, is
(a, ...$#, y, zf (a, y', z'f cos 2 0 - {(ft, y, z\x, y', z')} 2 = 0,
or
(a, ...$#, y, zf (a, ...$V, y', zf sin 2 6 — (a ...\yz' — y’z, zx - zx, xy' — x'yf — O,
from which (by the same reasoning as for the case of geometry of one dimension) it
follows that the distance of the points (x, y, z), {x, y, z') is
cos -
(a, y, z\x, y, z)
V(ft, ...$#, y, zf \/(a, y', zf ’
or what is the same thing,
sin-1 V(a .yz , ZX - z’x, xy' - x'yf .
' V(a, ...$#, y, zf V (ft, y, /) 2
and it appears from the cosine formula (see ante, No. 208), that if P, P', P" be
points on the same line, then we have, as we ought to have,
Dist. (P, P') + Dist. (P', P") = Dist. (P, P").
217. In like manner, the line-equation of the same circle, the line-coordinates of
the axis being (£', y, £"), is
(a. v, rmv, v, r$r, v. o)*=».
(a, ,, ...m (yco*e-K(a, sr-rf. fu'-W-o,
from which it follows that the distance of the lines (£, ??, £) and (£', 7/, £') is
cos -
(a, y, nr, y, r>
or what is the same thing
■■■$<- V?, ¡Tf- rf, ft'
?>»v<a,v, n*
sin
74—2