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.

~ 144. 145. Discretely and linearly discontinuous functions. 247 By "fluctuation" of the function is meant the magnitude of the breaches of continuity, or, the difference of the limits between which the indeterminate values lie, or lastly the difference between the maximum and minimum values. On the other hand we call a function linearly discontinuous, in which such points form a linear set of points. Now it is easy to see from Riemann's Theorem that within its interval: A discretely discontinuous function is integrable. For, a being a prescribed arbitrarily small finite number, we can carry the partition of the length ab so far, that in the partial intervals generally the fluctuations become less than a, while s, the sum of the neighbourhoods of all the points at which the fluctuations exceed a, can be arbitrarily diminished. Let m be the greatest value among these fluctuations, then: y=-n d dD < a(b - a) + sm. t =1 But the sum on the right can be diminished arbitrarily, since a may be assumed arbitrarily small, and likewise s in consequence of the property of a discrete set of points. Linearly discontinuous functions are not integrable. Examples of functions infinitely often discontinuous that are integrable. 1) Let the value of the function f(x) be zero everywhere in the interval from 0 to 1, except in the infinite series of points: i, ()2, ()3j (;)4,... (1)n in which its value is to be -. This function is infinitely often discontinuous within an arbitrarily small interval from zero; but the sum of the intervals in which the fluctuations are - can be made arbitrarily small. The value of the integral is determinate, it vanishes. 2) We can likewise construct a function that is integrable, although it is discontinuous in every interval however small, and though the number of points, at which it has discontinuities greater than some finite number, is not finite. Determining, ex. gr., that the function f(x) is to vanish generally in the interval from zero to unity, but yet that at all points of a discrete set of which the point ~ is the derived set its value is to be ~; at the set of points whose derived set are the points a, 2, its value is to be a; at the set of points with the derived set -,,,,, its value is to be {-; and generally: if p be a prime number and q denote each number smaller than p, at the set of points with the derived set, its value is to be p~ 2o

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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 230
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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