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.

334 The definite integral of a unique analytic function. Bk. IV. ch. 1. The case n =1, that already served as an example in ~ 179, requires a particular treatment; for here round a circle with the point zero or origin as centre we have: 2 7Z fdz ifd. 0 Therefore independently of the radius r the integral is equal to 2 in. Around the point infinity the integral has likewise a finite value; for, integrating along a circle with an arbitrarily great radius II, keeping the origin on the right, the integral is converted by the substitution 1 dz' i=-, dlo —,*e into: j- - to be integrated along a circle of radius -t keeping the origin on the left; thus its value is - 2iA. The value of the integral will accordingly depend on the path of integration; along a finite closed curve its value will be 2i7tk or zero, according as the closed curve goes round the origin k times or not at all. The integral z J z is a unique function of its upper limit a, when the paths that lead from the lower limit z0 to S do not cross a section leading from the origin to the point infinity; it is only in the plane perforated along this section that the values of the integral calculated along such curves are continuous; on opposite banks arbitrarily near the branching section they differ by the constant quantity 2iT. But the many-valued function which is presented by the integral is the logarithm treated in ~ 82, 5; for, 1(z) is that function whose derivate is -. The method there employed of rendering it a unique function by means of arbitrarily many leaves, is valid also for the integral. For each path not crossing the branching section we have: Zf ( - n a t his equation however, and thus in particular j c = (z). In writing this equation, however, we must observe that the quantity on the left is now determinate, while that on the right is still many-valued. What is the value on the right belonging to a determinate path? Before we can characterise a definite kind of path, we must adopt a definite branching section, ex. gr. the positive axis of ordinates. We reject the positive axis of

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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 330
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 May 16, 2025.
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