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. 1)

460 ON THE ORDER OF CERTAIN SYSTEMS OF ALGEBRAICAL EQUATIONS. [77 
we deduce 
and (ce — d 2 ) (arf + 2bfy + erf) 
+ (cd - be) (brf + 2erf) + drf) 
+ (bd — c 2 ) (erf + 2dtjr] + erf) 
= (ace — ad 2 — b 2 e — c 3 + 2bed) rf, 
ae — 4bd + 3c 2 = 0 , 
ace — ad 2 — b 2 e — c 3 + 2bcd = 0; 
which form the system in question, and may for shortness be represented by 1=0, J= 0. 
The three equations in rf rj may be considered as expressing that 
arf + Sbrfr] + 3crfrf + drf = 0, 
brf + 3crf 2 7) + 3 drf 2 + erf = 0, 
have a pair of equal roots in common; in other words, that it is possible to satisfy 
identically 
(A% + Brj) (arf + 3brfrj + 3c£rf + drf) 4-(A'g + B'rf) (brf + 3erfrj + 3d%rf + erf) = 0. 
Equating to zero the separate terms of this equation, and eliminating A, B, A', B', 
we obtain 
= 0. 
. a , 
3b, 
3c, 
• b , 
3c, 
3d, 
a, 3b, 
3c, 
d , 
b, 3c, 
3d, 
e , 
It is not at first sight obvious what connection these equations have with the 
two, 1=0, J = 0, but by actual expansion they reduce themselves to the following five, 
3 [2 (ce - d 2 ) I — 3eJ] = 0, 
3 [(be — cd) I — 3dJ] — 0, 
[— (ae + 2bd — 3c 2 ) 14- 9c J] = 0, 
3 [(ad — be) I — 3bJ] = 0, 
3 [2 (ac — b 2 ) I — 3aJ] = 0 ; 
which are satisfied by I = 0, J = 0. By the theorem above given, the equations are 
to be considered as forming a system of the tenth order; the system must therefore 
be considered as composed of the system 1 = 0, J =0, and of a system of the fourth 
order. The system of the fourth order may be written in the form 
2 (ac — b 2 ) : ad —be : ae + 2bd — 3c 2 : be — cd : 2 (ce — d 2 ) : 3 J 
3c 
d 
I:
	        
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