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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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