by considering the method of Jacobi and Mayer, while a good
summary is obtained by the formulation in terms of a Pfaffian
expression.
Characteristic chains.
Consider a solution of F = 0 expressed by the three independent
equations F = 0, G = 0, H = 0. If it be a solution in which there is
more than one relation connecting x, y, z, let new variables x', y',
z', p', q' be introduced, as before explained under PFAFFIAN
EXPRESSIONS, in which z' is of the form
z' = z - p1x1 - ... - p_s x_s (s = 1 or 2),
so that the solution becomes of a form z' = [psi](x'y'), p' =
d[psi]/dx', q' = d[psi]/dy', which then will identically satisfy the
transformed equations F' = 0, G' = 0, H' = 0. The equation F' = 0, if
x', y', z' be regarded as fixed, states that the plane Z - z' = p'(X -
x') + q'(Y - y') is tangent to a certain cone whose vertex is (x', y',
z'), the consecutive point (x' + dx', y' + dy', z' + dz') of the
generator of contact being such that
/dF' /dF' / / dF' dF'\
dx'/ -- = dy'/ -- = dz'/ ( p'--- + q' --- ).
/ dp' / dq' / \ dp' dq'/
Passing in this direction on the surface z' = [psi](x', y') the
tangent plane of the surface at this consecutive point is (p' + dp',
q' + dq'), where, since F'(x', y', [psi], d[psi]/dx', d[psi]/dy') = 0
is identical, we have dx' (dF'/dx' + p'dF'/dz') + dp'dF'/dp' = 0. Thus
the equations, which we shall call the characteristic equations,
/dF' /dF' // dF' dF'\ // dF' dF'\
dx'/ --- = dy'/ --- = dz'/( p' --- + q'--- ) = dp'/( - --- - p'--- )
/ dp' / dq' / \ dp' dq'/ / \ dx' dz'/
// dF' dF'\
= dq'/( - --- - q'--- )
/ \ dy' dz'/
are satisfied along a connectivity of [oo]^1 elements consisting of a
curve on z' = [psi](x', y') and the tangent planes of the surface
along this curve. The equation F' = 0, when p', q' are fixed,
represents a curve in the plane Z - z' = p'(X - x') + q'(Y - y')
passing through (x', y', z'); if (x' + [delta]x', y' + [delta]y', z' +
[delta]z') be a consecutive point of this curve, we find at once
/dF' dF'\ /dF' dF'\
[delta]x'( --- + p'--- ) + [delta]y'( --- + q'--- ) =
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