An Elementary Treatise On Quaternions

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Eliminating the first power of r, we evidently must obtain a result such as (|O-e)He^ + r-'' = 0, where (by what precedes) e is the vector of the centre, and e the radius, of a fixed sphere (p - if + e^ = 0, which is cut at right angles by all the varying spheres. By effect- ing the elimination exactly we easily find e and e in terms of given quantities.
247. If two vectors divide one another into parts a and — ea, p and -p, respectively, the lines joining the free ends meet in (1 + e) p - lea.
...
CT= .
1 — e We may write this as e,p = CT + aj, ■f 1 + e 2ea " e, = , a = : 1-e' ^ 1-, 247-] THE SPHERE AND CYCLIC CONE. 187 For another such pair of vectors, passing through the same point, we have, say, /^or = ^ + /3,.
Thus the plane quadrilateral, whose diagonals are made up respectively of the complete a and ^ vectors, will be projected (by lines from the point ■bt) as a square on the plane of p, a; provided Tp=TS.(^ + aJ(tT + ^J=0 (2).


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