Download e-book for kindle: Electric Contacts: Theory and Application by Ragnar Holm

By Ragnar Holm

ISBN-10: 364205708X

ISBN-13: 9783642057083

ISBN-10: 3662066882

ISBN-13: 9783662066881

This booklet is a very revised and rewritten version of "Electric Contacts instruction manual" released in 1958. loads of new in­ vestigations are thought of, and lots of of the elemental theories are revised intimately or even as a rule. The physique of data needed to be restricted because it used to be now not really useful to extend the amount of the publication. particularly, no try out used to be made to hide the entire useful purposes. they seem as examples following centred reasons of easy phenomena. As in different branches of know-how, the options of difficulties ari­ sing within the box of electrical contacts contain perception into numerous disci­ plines of physics. it's feit that experiences of a few of these themes, 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 idea of electrical conduction in solids, convinced professional­ blems in facts, and the idea of the electrical arc. As regards arc difficulties, new rules were brought. so one can make the most textual content much less bulky, such studies are offered as appendices. all through this version, the mksa-unit approach is utilized in accord with the newest advice for standardization of devices in clinical 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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Additional resources for Electric Contacts: Theory and Application

Example text

But in reality the problem i s more 1 Fir8t calculated by MAXWELL and with improved approximation by LoRD see MAxwELL [1] p. 434. R-\YLEIGH ; § 5. Constriction resistances when conditions deviate from those in § 4 21 complicated because the ffim alters the distribution of the current density from that of Eq. 18). Webegin by assuming that the film resistance is very large compared with the constriction resistance in the metal. Then, the interface A between metal and film is no Ionger an equipotential surface on the side of the metal.

At contacts when covered with a chemisorbed oxygen layer, the associa· tion with the corresponding solid curve again being indicated by shading. Every observationwas made with a new contact. The dashed curves . are entirely based on measurements on contacts which were closed after being exposed to air for some minutes (up to one hour) after a thorough cleaning. Under these circumstances, we can expect a chemisorbed oxygen layer to cover the faces.

Itute the inlet and outlet of the current. We assume that bis much smaller than D. We seek the resistance between Ac and A1 . In order to simplify the calculations we first imagine Ac and A 1 to be replaced, in the electrostatic case, by whole spheres Sc and Sl' The capacity between them is known 1 In this deduction, cgs units are used for the following reasons: 1. because with them the expression for 0 is particularly simple, and 2. because they are nsed in the references. ry Contacts 14 to be C !

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Electric Contacts: Theory and Application by Ragnar Holm

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