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. 5)

[330 
330] ON DIFFERENTIAL EQUATIONS AND UMBILICI. 125 
= 0, f— m; we 
Putting for shortness 
A = mx + Vn, 
B = mot? + y 2 + x VD, 
where it will be remembered that 
□ = m 2 x 2 + y 2 , 
then we have 
2mB = A 2 + (2m — 1) y 2 . 
G 
— i V 2 m — 1 ’ 
The integral equation may be written 
h=P+QVU= U = AB™- 1 ; 
and we have 
U A + 1 ' B ~ VD ’ 
if 
[A! , ^B'\ 
® = V □ + ( m -• 
But we have 
A' >/□ = mV□ + m 2 x + yp = mA 4-yj?, 
Ay + VD)} 2w " T i 
i?' Vn = (2m# + 2yp) VD 4- □ 4- x (m 2 x + yp) 
= 2m 2 x 2 + y 2 + xyp 4- (2mx 4 2y/:>) V □ 
= H 2 4- pyx + 2VO, 
and 
1 2m 
B ~ A 2 + (2m - 1) </ 2 ’ 
and the value of © thus is 
mA+yp A‘-+py(x + 2an) 
®- - A +(2m ¿m) A , + {2m -l)f 
_ 1 n l(m4 + «/») [4* +(2m - 1);/ ! ] + (‘¿ill- - -2m)[A- + Ap,j(x + 2v'd)]), 
A [A 2 + (2m-\)y 2 ] 1 
where the expression in { } is 
= (2m 2 — m) A (A 2 4- y 2 ) 
+ yp {A 2 4- (2m - 1) f + (2m 2 - 2m) A(x + 2VO)}. 
Here the coefficient of is = (2m 2 - m) (¿ 2 + y 2 ); in fact we have identically 
A 2 + y 2 - 2A VO =0, 
and thence 
(2m 2 - 3m 4- 1) (A 2 + y 2 )-% (2m -1) (m - 1) A VQ = 0, 
that is 
(2m 2 - m - 1) ^l 2 + (2m 2 - 3m + 1) y 2 - (2m — 2) A {A + (2m — 1) VD] = 0; 
that is
	        
Waiting...

Note to user

Dear user,

In response to current developments in the web technology used by the Goobi viewer, the software no longer supports your browser.

Please use one of the following browsers to display this page correctly.

Thank you.