An introduction to the study of the elements of the differential and integral calculus. From the German of the late Axel Harnack, With the permission of the author.

~ 95. 96. Uniqueness along certain definite paths. 161 back to its initial value. For in this case in the equation f(sm, wn) == 0 we have at the point S = a, q(p(a) =-O, while pl (a) is different from zero. Therefore if we put z = a + A a and consider the equation: wnAO + wun- lA] + * An = 0, writing Ak == (pk ( + A a), we can choose A a so as to make A0 smaller than an arbitrarily small number A, while mod [A,] certainly remains greater than some finite number B. Consequently it is true, in conformity with the proof ~ 93, of the equation: Ao + w'A1 + w'2A, +.. w'An = — 0, that it has for each value of A a one and only one root, for which mod w'= mod - < A, or, mod w > d i. e. when z has gone round the arbitrarily small circle, the final value of w can coincide with no other than the initial value. From the theorem follows further: If we make the argument s begin at a point zo and go round a closed finite curve not including any critical point, the final value of w1 at z0 is the same as that with which it began. 96. These Theorems do not yet enable us to picture to ourselves a branch of the function. For, having calculated the value w1 at a point zo, we can arrive at any other point by very different paths and any two of them may include a critical point; thus it is still possible that we may obtain at each point different values according to the path. The perfectly unique exposition, already exemplified in the explicit irrational function, is obtained here also by Riemann's method of adopting for the representation of z, instead of a single plane, n planes fastened together along their branching sections. But this requires that we should investigate more closely the properties of the critical points. Let the point = 0 be a regular point for all values of the function w; i. e. let n simple finite roots of the equation f(zm, Wtn ) 0 belong to it. Now conceive n different planes lying one on another; to each of them coordinate in the point - 0 one of the values wO,.... ~, indexing each plane by a number 1, 2,... n. Further, mark in each plane all those points 3, which are critical points for any values whatever of w, and from these points to the point infinity draw curves, intersecting neither themselves nor one another; in all the n planes the curves proceeding from a point Pk are conceived to be identical. Let us further coordinate to each point of plane 1 that value of w into which w1~ changes continuously when the argument z is made travel along a path not crossing any of the curves starting from the p points. In this manner a perfectly determinate value of w belongs HARNACC, Calculus. 11

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Title
An introduction to the study of the elements of the differential and integral calculus. From the German of the late Axel Harnack, With the permission of the author.
Author
Harnack, Axel, 1851-1888.
Canvas
Page 161
Publication
London [etc]: Williams and Norgate,
1891.
Subject terms
Calculus
Functions

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"An introduction to the study of the elements of the differential and integral calculus. From the German of the late Axel Harnack, With the permission of the author." In the digital collection University of Michigan Historical Math Collection. https://name.umdl.umich.edu/acm2071.0001.001. University of Michigan Library Digital Collections. Accessed June 22, 2025.
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