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.

160 The implicit algebraic function. Bk. II. oh. II. V. precisely into this value v' and into none of the others. For, at each point through which z passes, there is always only o n e value that differs from,w by less than ~D. If then w were to change continuously to a value differing from w1 by more than I-D, this difference should somewhere become equal.to I D; but this cannot be for any point in the circle. Thus too since t' lies in the circle round z', the difference between v' and w' is smaller than -1D. Similarly, to t" belongs one value v", differing from the value w' by less than -D, since t" is on the circumference of the circle drawn round z'. This value is obtained by travelling along the curve (2) from t' to t"; for were w to assume a different final value, it would be one differing from w' by more than ~D. Therefore there should be upon the path t't" a point at which the difference is -I-D; and this again is excluded, because t' and t" are within and upon the circle round S'. Since t" lies in the circle round the centre z" we have: mod [v"- w"] < -ID. In like manner it can be seen that for the values at t" and zv: mod [VV - w"] <- 4D, and from these points we arrive at the values W and V. Here the inequalities are: mod [ WY- tw] < i-D, mod [ - wu, < - D. Hence follows that mod [W - V] < D. Now since by hypothesis the n different values of w at the point Z differ from each other at least by D, W and V cannot signify two different values, so that we must have V== W. Therefore the curve (I) and the curve (2) lead to the same final value. From curve (2) we can pass over to a curve (3) closer to (II) and proceeding thus we must ultimately be able to arrive at curve (II). For, all the radii h are of finite assignable magnitude therefore it is not possible that the number of steps can be infinite. Such a progressus in infinitum can only occur when the interpolated curves are approaching a critical point of w: for, in the immediate neighbourhood of such a point no circle can be determined within which always one only of the corresponding roots differs from wu by less than -I D: the quantity indicated by D), here converges to zero. If in the included domain there be a non-essential singular point that is not also a critical point, the theorem still holds. For, although the algebraic function becomes infinite in this point, yet it retains the character of a rational function and remains unique. In fact if we surround the point by a circle of arbitrarily small radius, then, while z goes round this circle, that root, whose amount increases beyond all limits as the singular point is approached, passes through a continuous series of values, that returns

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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 150
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 9, 2025.
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