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.

~ 148. 149. Te function to be integrated becomes infinite. 259 cos (e + - exA sin (e ) which for every finite value of x is identical with the derivate: dx X cos (e) becomes completely indeterminate for x - 0, oscillating between arbitrarily great positive and negative values as x approaches zero. Its infinitude is infinite. Nevertheless we have: o ex + jf |cos (e ) + -a- e sin (eA); dx == x cos (e) + C, even for the value x = 0; because: d, x cos (el )lx =x — = cos (e) -- a cos (eA converges to zero along with a and,. Corollary. When the function becomes infinite in infinitely many discrete points of its interval of integration, we can resolve this interval into a finite number of finite intervals that contain none of the infinity points, while these latter are included within intervals whose sum becomes arbitrarily small. The integral has a meaning, provided the partial integrals, formed for the intervals containing no infinity points, converge to fixed values when the limits of these intervals are brought arbitrarily close to the infinity points. When the infinity points form a linear set, such a definition is no longer possible, since there are then finite intervals containing everywhere infinitely many points of the kind. 149. The Theorems given in ~ 146 are somewhat modified by the occurrence of infinity points. We confine our investigation to the assumption of a finite number of such points. Instead of Theorem V., whose proof essentially required that the function to be integrated should be finite, we obtain the theorem: When (p(x) and O(x) are two functions integrable from a to b, each becoming infinite at certain points c, but without any infinity point of (p coinciding with one of Ap, the product (p(x). P (x) can be integrated in the same interval whenever the functions (p2(x) and,P (x) formed of the absolute values of (p and 4 remain integrable. In proving this theorem we need only consider an interval from a to c, within which neither function becomes infinite, while the limit c is an infinity point for one, ex. gr. for (p(x). Evidently then: the amount of 17*

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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 250
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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