Full text: The collected mathematical papers of Arthur Cayley, Sc.D., F.R.S., sadlerian professor of pure mathematics in the University of Cambridge (Vol. 6)

407] 
CURVES WHICH SATISFY GIVEN CONDITIONS. 
269 
106. As regards the case (4Z) (1), taking P an arbitrary point of the given curve 
to, and for the curve W the system of the conics (4J£)(1) which pass through the 
given point P and besides satisfy the four conditions, then the curve © has with 
the given curve (4i/)(l) intersections at P, and the points P' are the remaining 
(2to — 1) (4Z) (1) intersections: in the case of a united point (P, P'), some one of the 
system of conics becomes a conic (4Z) (1); and the number of the united points is 
consequently equal to that of the conics (4^)(1); we have thus the equation 
{(4Z) (1) - 2 (2to - 1) (4Z) (I)} + Supp. (4Z) (T) = (4Z) (I). 2D. 
107. It is in the present case easy to find a priori the expression for the 
Supplement. 1°. The system of conics (4Z) contains 2 (4<Z■) — (4*Z/) point-pairsQ; each 
of these, regarded as a line, meets the given curve in to points, and each of these 
points is (specially) a united point (P, P'); this gives in the Supplement the term 
to (2 (4Z •) — (4Z /)}. 2°. The number of the conics (4Z) which can be drawn through 
a cusp of the given curve is =(4Z-); and the cusp is in respect of each of these 
conics a united point; we have thus the term /¿(4Z ■), and the Supplement is thus 
= to {2 (4iT •) — (4Z/)} + k (4Z•). We have moreover (4Z) (1) = (4Z •), 2D = n— 2to + 2 + k ; 
and substituting these values, we find 
(4£)(1)= (4to — 2) (4<Z •) 
— to {2 (4>Z •) — (4>Z/)} — k (4iZ •) 
+ (n — 2m + 2 + k) (4 Z •) 
= n(4<Z •) + m(4fZ I), 
which is right. 
108. It is clear that if, instead of finding as above the expression of the 
Supplement, the value of (4J?)(1), =n(4>Z •) +m(4eZ ¡), had been taken as known, then 
the equation would have led to 
Supp. (4Z) (I) = to {2 (4Z ■) — (4Z /)} + tc (4Z •) ; 
and this, as in fact already remarked, is the course of treatment employed in the 
remaining cases. It is to be observed also that the equation may for shortness be 
written in the form _ 
(4 Z) {(1)-2(2to-1)(1)} 
+ Supp. (I)=(T)2D; 
viz. the (4Z) is to be understood as accompanying and forming part of each symbol; 
and the like in other cases. 
109. We have the series of equations 
(4Z) {(1) - (I) (2to - 1) - (I) (2to -1)} 
-i- Supp. (1) = (1) ; 
1 The expression a point-pair is regarded as equivalent to and standing for that of a coincident line-pair. 
see First Memoir, No. 30.
	        
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