149] OF CERTAIN SYSTEMS OF TWO EQUATIONS. 461
3f =
3g = Z x Z 2 X 3 + Z 2 Z^C X + Z 3 Z x X 2 ,
3h = x x x 2 y 3 + x 2 x 3 y x + x& x y 2 ,
3i = y x z 2 z 3 + y 2 z 3 z x + y & z x z 2 ,
3j = Z x XJX 3 + ZrfC 3 X x + Z 3 X x X2,
3k = x x y 2 y 3 + x 2 y 3 y x +x 3 y x y 2 ,
61 = X x y 2 Z 3 + x 2 y 3 z x + X 3 y x z 2 + X x y 3 Z 2 + X 2 y x z 3 + X 3 y 2 Z x .
But there is in the present case a relation independent of the quantities a, &c., viz.
we have (a, /3, yjx u y x , z x ) = 0, (a, /3, y^x 2 , y 2 , z 2 ) = 0, (a, /3, yjx 3 , y 3 , z 3 ) = 0, and
thence eliminating the coefficients (a, /3, 7), we find
V = x x y 2 z 3 + x 2 y 3 z x + x 3 y x z 2 - x x y 3 z 2 - x 2 y x z 3 - x 3 y,z x = 0.
By forming the powers and products of the second degree a 2 , ab, &c., we obtain 55
equations between the symmetric functions of the second degree in each set of roots.
But we have V 2 = 0 = a symmetric function of the roots, and thus the entire number
of linear relations is 56, and this is in fact the number of the symmetric functions
of the second degree in each set. I use for shortness the sign S to denote the sum
of the distinct terms obtained by permuting the different sets of roots, so that the
equations for the fundamental symmetric functions are—
a = x x x 2 x 3 ,
b= 2AM3,
c = z x z 2 z 3 ,
3f = S y x y 3 z 3 ,
3g = S z x z<>x 3 ,
3h = S x x x 2 y 3 ,
3i = >Sf y x z 2 z 3 ,
3j = Sz x x 2 x3,
3k = S x x y 2 y 3 ,
61 = Sx x y 2 z 3 ;
then the complete system of expressions for the symmetric functions of the second
order is as follows, viz.
a 2 — nr* 2/y» 2no 2
lA/y lAj2 tA/g j
b 2 = y x y 3 y 3 ,
c 2 = Z X 2 Z 2 2 Z 3 2 ,
be = y x z x y 2 z 2 y 3 z 3 ,
ca = z 1 x 1 z 2 x 2 z 3 x 3 ,
ab = x x y x x 2 y 2 x 3 y 3 ,