Full text: The collected mathematical papers of Arthur Cayley, Sc.D., F.R.S., late sadlerian professor of pure mathematics in the University of Cambridge (Vol. 12)

Multiplying the numerator and denominator by a 2 + 3, we have in the numerator a term 
in 8a 3 , which may be got rid of by means of the pa-equation; the numerator for 
- A„ thus becomes 
{p 8 + 17p 6 + 102p 4 + 225p 2 -|-97} —P \ ^ (p 8 +14p 6 + 63p 4 + 70p 2 — 7) + 8 (p 2 + 7) 
P 
12 (—p 4 — 9p 2 — 9) + 16p (p 2 + 7) a 
+ (a 2 — l)p 
and we finally obtain 
1 A _ 12 (-p 4 - 9p 2 - 9) + 16p (p 2 + 7)a + (a 2 - l)p~ 4 (p 8 + lip 6 + 37p 4 + 20p 2 + 2) 
p (a 2 + 3) (p 4 + op 2 + 1) 
82. The expressions obtained above for p 2 , A lt A 2 are of the form 
M+Na 
Pi + Qiix + RiCt 
S (a 2 + 3) 
1 a P% + + -B 2 a~ 
p 2_ £(a 2 + 3) 
where 
M = p 4 + 29p 2 + 49 ; A r = 8p (p 2 + 7) ; S=p 4 + 5p 2 + l, 
Pi = 12 (—p 4 — p 2 + 7)-p (p 8 + I7p 6 + 102p 4 + 225p 2 + 97), Q 1 = - 16p (p 2 + 7), 
jKj = p (p 8 + 17p 6 + 102p 4 + 22op 2 + 97); 
P 2 =12(— p 4 -9p 2 — 9) — p~ 4 {p 8 + lip* + 37p 4 + 2Op 2 + 2), Q 2 = 16p (^> 2 4- 7), 
B, = p -1 (p 8 + lip 6 4- 37p 4 + 2Op 2 4- 2) ; 
substituting these values in the foregoing equation 
12M 2 = 6A j 2 + 8aA 2 -p 4 + 7, 
we obtain 
P<i + Qa® + -ß 2 a 2 ( _ (6 (Pi + Qiß + Pja 2 ) 2 g a -Pi + Qi a + Pi a 2 (if + Pa) 2 ^ . 
12 " j N (7' i :i i' ; 
that is, 
S 2 (a 2 + 3) 2 
S (a 2 + 3) 
S 2 
p 12 (P 2 + Q 2 a + P 2 a 2 ) 2 (3 + a 2 ) £ ^ Pl + ^ + + 8a,S @ + ^ Pl + + ^ a2 ) 
- (M + Pa) 2 (3 + a 2 ) 2 + 7$ 2 (3 + a 2 ) 2 }, 
which, by means of the pa-equation 
/ Q[3 Q/y\ 
p 8 + 14p 6 + 63p 4 + 7Op 2 - f—- j 8p - 7 = 0, 
should be reducible to the form 
p = Aa 2 + Ba + G, or p = 
Aa + B 
Coc + D’ 
but I have not been able to obtain, in either of these forms, a simple expression of 
p as a function of p, a. Supposing it obtained, the pa-equation, ante No. 51, would 
of course be thereby transformable into the foregoing pa-equation. And considering 
p as an auxiliary parameter thus introduced into the formulae in place of p, then 
/3 and the coefficients A 1} A 2 are, by what precedes, expressed in terms of p, a, that 
is, in effect in terms of p, a; and we thus have the formulae of transformation for the 
C. XII. 70 
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