[545
545]
DIFFERENTIAL EQUATIONS OF THE FIRST ORDER.
531
n — 1) fold
i, that is,
f to be
y is, that
function
y, of the
either for
,1 values),
tsively to
regard to
U) to be
for which
:en to be
ly of the
tonal and
to 0, y).
ire of a
equation
we have
equations
ented by
osing the
breaking
) distinct
h system
.fferential
;r system
equation
2 - c = 0,
nsidering
ever, we
r (faulty)
-xy) = 0,
= 0; and
3 are in
iposable ;
in the
5°. It is necessary to consider a form f— 0 involving the m constants connected
by the (m —l)fold relation. For taking such a system of constants, imagine an
equation f{x, y, c 1; c 2 ,..., c m ) = 0 rational and integral in regard to {x, y), and representing
an indecomposable curve; such an integral equation leads to a differential equation
of the form </> {x, y, p) = 0, rational in regard to (x, y); whence, conversely, a differ
ential equation of the form last referred to may have for its integral the equation
f{x, y, Ci, c 2 ,, c m ) = 0. And we cannot in a proper form exhibit this integral in terms
of a single constant. For first consider for a moment c a , c 2 ,..., c m as the coordinates
of a point in m-dimensional space; the curve is not in general unicursal, and unless
it be so, we cannot express the quantities c 1} c 2 ,..., c m rationally in terms of a para
meter; that is, we cannot in general express c 1} c 2 ,..., c m rationally in terms of a
parameter. Secondly, if by means of the {m — 1) fold relation we sought to eliminate
from the equation f = 0 all but one of the m constants, we should indeed arrive at
an equation F (x, y, c) = 0 rational and integral as regards x and y, and also as regards
c; but this equation would not represent an indecomposable curve.
6°. It is important to remark that, even in the case where <£ {x, y, p) is one
valued in regard to {x, y) (2°), there is not in every case a form /=0 one-valued
in regard to (x, y). A simple example shows this; let a, fi be incommensurable
(e.g. a = e, /3 = w), then the equation </> = /3xp + ay = 0 {ay dx + fix dy = 0) has for its
integral c = x a yP, where x a y& is not a one-valued function of x, y, and we cannot in
any way whatever transform the integral so as to express it in terms of one-valued
functions of x and y. But taking x a yP to be a one-valued function—if e.g. for all
real values of x, y we consider x a y& as representing the real value of {±x) a {±yf— r
we shall have, without any loss of generality, the integral of the differential equation;
the whole system of curves c = x a y?, c any value whatever, is the same whether we
attribute to x a y? its infinite series of values, or only one of these values.
7°. The meaning is, that the equation /=0 is not satisfied irrespectively of the
values of c 1} c 2 ,..., c m by any relation between x, y only.
8°. The meaning is, that the function f is not the product of two factors, rational
or irrational in regard to c x , c 2 , ..., c m , but each of them one-valued or taken to be
one-valued in regard to x, y. Thus the function
/= x*y 2 -o, = \xy + f{c)} [xy - V(c)},
is decomposable; but if we do not take any one-valued function, then f=xy — c is
indecomposable; if we take f{xy) to be one-valued, then it is decomposable.
The case /= x a y? — c {a and fi incommensurable) is to be noticed; starting from
the differential equation ay dx + fix dy = 0, there is no reason for writing the integral
— £
f= x a yP — c—0 rather than in either of the forms f=x ma y m P — c=0, f=x m y m — c=0,
{m an integer), {a, fi), {ma, m/3), (—, —\ are, each pair as well as the others, two
777//
— —
incommensurable magnitudes. If we choose to take x a y& but not x m y m as one-valued.
67—2