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.

380 Expansion of ambiguous analytic functions. Bk. IV. ch. III. When one root of the equation k == 0 becomes infinite, this means that fo,k = 0, and the degree of 0k reduces to k - 1. In order to obtain that element of the function which belongs to the one infinite root, let us first expand S as a function of w, as at the end of ~ 200. The series begins with the term w2, or with some higher power of w when further consecutive values of the derivates of z with respect to w also vanish. When wsk' is the first term, we obtain by inversion 1 a k'-branched element of the function, having the initial term zk'. The geometric statement of this case is: In the multiple point one of the k branches of the curve has a tangent parallel to ordinates having k' consecutive points on it, or having a contact of the order '- 1 with that branch of the curve. The theorem still holds for each simple root of ck = 0 even when there are multiple roots besides. But, for a multiple root it does not hold; for, because vanishes for such a root, the values of the higher derived functions for it are no longer generally finite. Thus the question finally outstanding is: What is the form of the expansion for a multiple value of w, finite or infinite? 202. Although this question can also be solved by successive substitutions*), a process having the preference: that it employs only the Theorem for the possibility of the expansion in a regular point of an algebraic function in order to deduce from it the existence and nature of the expansions in the singular point, still, since the general investigations in this chapter establish the existence of the expansion, it appears suitable that we should go back to the method given by Newton, which has been elaborated by Puiseux.**) Suppose the equation f(z + a, w + b) = 0, which defines the function that is to be investigated in the neighbourhood of its k-elementary point = 0, w = 0, arranged by powers of z and w. Since we must henceforth assume that some partial derivates of the kth order (specially fo,k) also may vanish, let us conceive the terms of the equation arranged as follows. Take first the term independent of w in which g occurs in the lowest power; there must be such a term, for otherwise the factor w could be separated and the equation would *) See Hamburger: Ueber die Entwickelung algebraischer Functionen in Reihen. Zeitschrift f. Math. u. Physik, Vol. XVI. Nother: Ueber die singularen Werthsysteme einer algebraischen Function. Math. Annal., Vol. IX, pp. 166-182. N*) Newton in the letters to Oldenburg, June 13 and October 24, 1676. Newton's method was explained and proved by Stirling, who says of it: "quae est omnium quam quis excogitare potest, generalissima et elegantissima", Lineae tertii ordinis, 1717; Cramer: Analyse des lignes courbes, 1750; Puiseux, see reference in foot-note ~ 91, p. 154. Compare also the exposition given in Briot et Bouquet.

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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.
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Page 370
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London [etc]: Williams and Norgate,
1891.
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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 9, 2025.
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