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.

~ 82. Non-essential singular point. 131 2. The rational fractional function: is one-valued (z - a)m and continuous in the entire plane, except at the non-essential singular point z = a. The point infinity is not singular, since by the above substitution we have for it: — ) = ( --- = The most general rational fractional function is of the form: Ca + a1z + a2z2 +. * a, n bo + bz - + b2 - +. b mZ7 It will be shown in next Chapter, that every rational integer function of the degree n may be broken up into n linear factors. If this result be assumed here, and this fraction therefore written in the form: 6n (Z- a,) (b -- 2) * (Z - n) b (Z-Pi1) (Z-P2). - (Z at) where some of the quantities a as well as some of the f may be equal, but each a will be supposed different from each (3 because otherwise factors could be cancelled, then obviously: the rational fractional function is one-valued and continuous in the entire finite plane except at the non-essential singular points pf, f2... Pm. The point infinity likewise is a non-essential singular point when n > m, but is a regular point when n < m. For, the function behaves for -- co as: an (21)(lo)~ **(,). n)~ an _(m —n(1- ) (l- 2Z) -.. (1 —CanX) ( i 1) (f 2 -2)(- ) bm (1-i') (1-Z') ( 1 —mZ behaves for a' = 0. 3. The simplest explicit irrational algebraic function: w = (' — a)T^, m a rational fractional number p- reduces to the form gm by the substitution ' - a =. All propositions which we shall prove for the function zm, can be easily transferred to the more general form (' - a)m since we have only to observe that whatever holds for the point z = 0 relates to the point ' = a. If z = r (cos (p- i sin g), then for k = 0, 1,..q - 1, w = i = ri (cos P ('p + 2kfc) + i sin q ( + 2a )). This exposition shows that the function can be calculated. For, both cosine and sine are series of powers. Each integer value of k determines at each point the corresponding value of a branch of the function; it is therefore a many-valued function, no longer singlevalued as those in the previous examples. At the point z = 0 and at = o all branches have the same values, namely: 9*

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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 131
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 15, 2025.
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