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.

~ 171. 172. Infinite domain of integration. 309 When it is to be formed for the inside of one branch of a hyperbola whose equation is: x > 0, xy = -, the double integral can be defined as: a b aZ j f/x y) d T = Lim J dx f(x, y) cdy Lim dy f (x, y) d x. (a =oo, 6 = ) k k (a=oo, b-c) k k X=- Y - By= - x --- b x a y The value of the double integral becomes singular, when it depends on the way in which a and b become infinite. When for arbitrarily increasing value of x and y, the function to be integrated f(x, y) = f(r cos p, r sin p) has ultimately neither maxima nor minima, so that, within its domain of integration for every value of p as r increases infinitely, f converges to zero; then, if its order of vanishing (nullitude) be higher than the seconrd, since from a A certain value rl, f(r cos p,q r sin p) is constantly < a where a > 2, the double integral is finite and completely independent of the method of the transition to the infinite region. For, the part of the integral: f(x, y)cT relative to a domain for which r > rl, is less than: A fl and this expression vanishes for arbitrarily increasing values of r. But the double integral has no finite value whatever, when the function f(x, y), having neither maxima nor minima as the values of x and y increase, becomes infinitely small in an order lower than the second or continues finite. In case the function undergoes incessant oscillations as the values of x and y increase infinitely, the double integral exists, as did the simple integral, without involving any limit as to the order in which the function becomes infinitely small. When the double integral has no existence, there may yet be a singular value for a determinate succession of integrations. One example of this was given in last ~.; another important example is the following: The function f(x, y) = cos (xy) is not integrable in the infinite strip from x = 0 to x = b, y = 0 to y -= o, for we have: h b b b h b C - r / \7 \ / - I sin hx fdyf cos (x y) dcx fdx cos (xy) dy == sif j dx fn - dx, 0 0 0 0 0 0 and if we first make Ih increase arbitrarily in the function to be integrated, this becomes quite indeterminate; but the integral:

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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 290
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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