Download Electric Contacts: Theory and Application by Ragnar Holm PDF

By Ragnar Holm

This publication is a very revised and rewritten version of "Electric Contacts instruction manual" released in 1958. a good number of new in­ vestigations are thought of, and lots of of the fundamental theories are revised intimately or even normally. The physique of data needed to be constrained because it used to be now not a good suggestion to extend the amount of the e-book. particularly, no try was once made to hide the entire useful purposes. they seem as examples following targeted motives of uncomplicated phenomena. As in different branches of know-how, the suggestions of difficulties ari­ sing within the box of electrical contacts contain perception into a number of disci­ plines of physics. it truly is feit that stories of a few of these subject matters, especi­ best friend tailored to electrical touch phenomena, are welcome to many readers. for instance, chapters were dedicated to the constitution of carbon, the band conception of electrical conduction in solids, convinced professional­ blems in information, and the idea of the electrical arc. As regards arc difficulties, new principles were brought. on the way to make the most textual content much less bulky, such reports are provided as appendices. all through this variation, the mksa-unit method is utilized in accord with the newest suggestion for standardization of devices in medical and technical writings. The bankruptcy "History of Early Investigations on Contacts" forming half IV within the previous version of 1958 has no longer been repeated during this book.

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Extra info for Electric Contacts: Theory and Application

Example text

The theory of indentation in § I treats the formation of calculable load bearing areas, Ab, for members with smooth surfaces and cases when Ab is a circle or an ellipse, particularly the cases when the members are spheres, including a sphere and a plane, or crossed cylinders. Imagine the indentation to be produced purely elastically at sufficiently smallload. Fora circular Ab, the radius is given by HERTz's formula (I, 1); for ellipses, formulas are given in RoARK [1]. These formulas are deduced for ideally smooth surfaces.

10) where f-l is a parameter and the axes of the ellipse coincide with the directions of x and y. It is obvious from Eq. 10) that the height of a --semi-ellipsoid (normal to the xy-plane) is ltt and that vo: 2 + f-l is its axis in the x direction, cf. Fig. 16). 10) is, in cgs electrostatic units [/vl•' + -~~ß' + •>,]_, Thus with Eq. ) p. 12) Evalutions of Eq. 11) are discussed in problems D and E. Problem D with verification of the constriction resistance. , a circular conducting surface A 0 • 1 Sl\IYTHE [1] Chapter V, pp.

Let R(a, B) be the constriction resistance, for one member, whichforafB->Oisef4a and fora = Bis zero. 85 1 according to RoEss: e2 1 nB R(a, B) = 0 ·296 00 and with R (a, B) = RcE according to Eq. 82 00 Problem I. Another kind of distortion appears when the current enters an infinite slab (thickness h, resistivity e) through a circular contact area A 1 (radius a), with the bottom surface A 2 of the slab in perfect contact with an ideal conductor; cf. Fig. 19). Let R(h, a) be the reZasistance in a slab characterized by h and Ideal a.

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