Article 27
Functions of Complex Numbers.

As vector quantities are of frequent occurrence in Mathematical Physics; and as the numerical measure of a vector in terms of a standard vector is a complex number of the form x + iy, in which x,y are real, and i stands for 1; it becomes necessary in treating of any class of functional operations to consider the meaning of these operations when performed on such generalized numbers.6 The geometrical definitions of coshu, sinhu, given in Art. 7, being then no longer applicable, it is necessary to assign to each of the symbols cosh(x + iy), sinh(x + iy), a suitable algebraic meaning, which should be consistent with the known algebraic values of coshx, sinhx, and include these values as a particular case when y = 0. The meanings assigned should also, if possible, be such as to permit the addition-formulas of Art. 11 to be made general, with all the consequences that flow from them.

Such definitions are furnished by the algebraic developments in Art. 16, which are convergent for all values of u, real or complex. Thus the definitions of cosh(x + iy), sinh(x + iy) are to be

cosh(x + iy) = 1 + 1 2!(x + iy)2 + 1 4!(x + iy)4 + , sinh(x + iy) = (x + iy) + 1 3!(x + iy)3 + (52)

From these series the numerical values of cosh(x + iy), sinh(x + iy) could be computed to any degree of approximation, when x and y are given. In general the results will come out in the complex form7

cosh(x + iy) = a + ib, sinh(x + iy) = c + id.

The other functions are defined as in Art. 7, eq. (9).

Prob. 79.
Prove from these definitions that, whatever u may be, cosh(u) = cosh u, sinh(u) = sinh u, d ducosh u = sinh u, d dusinh u = cosh u, d2 du2 cosh mu = m2 cosh mu, d2 du2 sinh mu = m2 sinh mu.8