# Page:EB1911 - Volume 14.djvu/578

OUTLINES]
547
INFINITESIMAL CALCULUS

The differential coefficient

ani

axpayvazf

in which p+q+r=n, is formed b differentia tin times with Y . g P

reseaaect to x, q times with respect to y, r times with respect to z, the d i erentiations being performed in any order. Abbreviated notations are sometimes used in such forms as

f» .)

fffyczf 07 LZ;-

Difcrenlials of higher orders are introduced by the defining equation

6 8 ' "

f1"f- (11165-lr'55,) f

3" " 0"f

= (dx)"£+n(dx) 1dyax, , 1ay+ . . .

in which the expression dx%c+dy(% n is developed by the binomial theorem in the same way as if dxéggc and dy% were numbers, and 0

B-rf is replaced by When there are more than two variables the multinomial theorem must be used instead of the binomial theorem.

The problem of forming the second and higher differential coefficients of implicit functions can be solved at once by means of partial differential coefficients. For example, if f (x, y)=o is the equation defining y as a function of x, we have ei: (aff (er) =<n .Q1;.Qt. av: + at) air E dx' By <9y 6x2 6x ay Bxdy 6x 6312

The differential expression Xdx-l-Ydy, in which both X and Y are functions of the two variables x and y, is a total deferential if there exists a function f of x and y which is such that df/6x =X, df/dy = Y.

When this is the case we have the relation BY/6x = 6X/dy. (ii.)

Conversely, when this equation is satisfied there exists a function f which is such that,

dj=Xdx-I-Ydy.

The expression Xdx-l-Ydy in which X and Y are connected by the relation (ii.) is often described as a “perfect differential.” The theory of the perfect differential can be extended to functions of n variables, and in this case there are %n(n-I) such relations as (ii.). In the case of a function of two variables x, y an abbreviated notation is often adopted for differential coefficients. The function being denoted by z, we write

p rstfor%»Q1&»iyi»&

9' ' ' ax 0y ax= axay ayf

Partial differential coefficients of the second order are important in geometry as expressing the curvature of surfaces. When a surface is given by an equation of the form z=f(x, y), the lines of curvature are determined by the equation

l<1+q')S-Pail (ds/)'+{(1+q')f-(1+i>”)l}dxdy ~i<1+p2>.=-pqf1<dx>==so.

and the principal radu of curvature are the values of R which satisfy the equation

R'(ff-82) -Rlfl +Q”)f-2P9S+(I +l>')llw/ (I +P”-l-Qi) +(I+P“+<1'>'=<>.

44. The problem of change of variables was first considered by Brook Taylor in his Methodus lncremenlofum. In the case concbmn of sidered by Taylor y is expressed as a function of z, and z "Hawes as a function of x, and it is desired to express the differential coefficients of y with respect to xwithout eliminating z. The result can be obtained at once by the rules for differentiating a product and a function of a function. We have &' Q'&

dx dz'dx

4a a»e+<1f i. (ay,

dx2"dz dx' dz* dx

¢l3y dy d3z dz>3

z%° ¢E ¢IF+3d22 dx dx2+dz“ (EEC,

The introduction of partial differential coefficients enables us to deal with more general cases of change of variables than that considered above. If u, 11 are new variables, and x, y are connected with them by equations of the type

xzflcui v)v y=f2(u1 U):

while y is either an explicit or an implicit function of x, we have the problem of expressing the differential coefficients of various orders of y with respect to x in terms of the differential coefficients of v with respect to u. We have

fi % 0 2531 in 3 Q)

Exec- (6u+5£ du>/ (614 +55 du

547

by the rule of the total differential. In the same way, by means of differentials of higher orders, we may express d2y/dxz, and so on. Equations such as (i.) ma be interpreted as effecting a transformation by which a point (u, vlyis made to correspond to a point (x, y). The whole theory of transformations, and of functions, or differential expressions, which remain invariant under groups of transformations, has been studied exhaustively by So hus Lie (see, in particular, his Theorie der Transformalionsgruppen, lbeipzig, 1888-1893). (See also DIFFERENTIAL EQUATIONS and GROUPS). A more general problem of change of variables is presented when it is desired to express the partial differential coefficients of a function V with respect to x, y, . . in terms of those with respect to u,11, ., where u, v, . . . are connected with x, y, . by any functional relations. Wllen there are

functions of x, y, we have

two variables x, y, and u, 'v are given a-@va»+@ya, I

6x -El 6x 311 élx

6y du dy. dv dy

and the differential coefficients of higher orders are to be formed by repeated applications of the rule for differentiating a product and the rules of the type »

2. = as +a 1.

6x '6x du 6x 61:

When x, y are given functions of u, 'u, . we have, instead of the above, such equations as

n ne+na.

6u dx Bu 6y Hu

and 6V/élx, 6V/By can be found by solving these equations, provided the Jacobian 6(x, y)/6(u, v) is not zero. The generalization of this method for the case of more than two variables need not detain us.

In cases like that here considered it is sometimes more convenient not to regard the equations connecting x, with u, v as effecting a point transformation, but to consider the lyoci 'u=const., v=const. as two “families” of curves. Then in any region of the plane of (x, y) in which the Iacobian 6(x, y)/6(u, 11) does not vanish or become infinite, any point (x, y) is uniquely determined by the values of u and 'zz which belong to the curves of the two families that pass through the point. Such variables as u, v are then described as “curvilinear coordinates ” of the point. This method is applicable to any number of variables. When the loci u=const., . intersect each other at right angles, the variables are “ orthogonal ” curvilinear coordinates. Three-dimensional systems of such coordinates have important applications in mathematical physics. Reference may be made to G. Lamé, Legons sur les coordonnées cur-vllignes (Paris, 1859), and to G. Darboux, Legans sur les coordonnées curvllignes el systémes orlhogonaux (Paris, 1898).

When such a coordinate as u is connected with x and y by a functional relation of the form f(x, y, u) =o the curves u=c0nst. are a family of curves, and this family may be such that no two curves of the family have a common point. lVhen this is not the case the points in which a curve j(x, y, u) =o is intersected by a curve f(x, y, u+Au) =o tend to limiting positions as Au is diminished indefinitely. The locus of these limiting positions is the “ envelope " of the family, and in general it touches all the curves of the family. It is easy to see that, if 'u, 'v are the parameters of two families of curves which have envelo s, the Jacobian 6(x, y)/6(u, v) vanishes at all points on these envelifpes. It is easy to see also that at any point wheie the reciprocal Jacobian 6(u, "v)/6(x, y) vanishes, a curve of the family n touches a curve of the family 11. If three variables x, y, z are connected by a functional relation f(x, y, z)=o, one of them, z say, may be regarded as an implicit function of the other two, and the partial differential coefficients of z with respect to x and y can be formed by the rule of the total differential. We have

<E= '2i/Q '?E= Q'/QI.

0x 6x dz' 6y éy dz

and there is no difficulty in proceeding to express the higher differential coefficients. There arises the problem of expressing the artial differential coefficients of x with respect to y and z in terms of) those of z with respect to x and y. The problem is known as that of “ changing the dependent variable.” It is solved by applying the rule of the total differential. Similar considerations are applicable to all cases in which n variables are connected by fewer than n equations. "

45. Taylor's theorem can be extended to functions of several variables. In the case of two variables the general for- Extension mula, with a remainder after n terms, can be written of 7-, ,, ,|o, .», most simply in the form

f<a+h, z>+k> =f<a, b>+df<a, b>+ édwa., b>+ . . theorem.

+(@d"-val, b>+;, %d"f<f»+@h, b+@1=>. in which

dv°<a.1»>= [(h§ +k§)'f<x, y> M H; 