Difference between revisions of "Unipoplar Induction and Weber's Electrodynamics"
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==Abstract== | ==Abstract== | ||
− | Unipolar induction is the generation of current on a conductor for the case in which the conductor and the magnet are in relative rotary motion. A typical case of unipolar induction is shown in figure 1. Since Faraday's experiments of 1932 on electromagnetic induction on rotation systems there are intense debates concerning the location of the seat of the electromotive force (<em>emf</em>)<sup>2</sup>. | + | Unipolar induction is the generation of current on a conductor for the case in which the conductor and the magnet are in relative rotary motion. A typical case of unipolar induction is shown in figure 1. Since Faraday's experiments of 1932 on electromagnetic induction on rotation systems there are intense debates concerning the location of the seat of the electromotive force (<em>emf</em>)<sup>2</sup>. |
− | [[Category:New Energy]] | + | [[Category:Scientific Paper|unipoplar induction weber 's electrodynamics]] |
+ | |||
+ | [[Category:New Energy|unipoplar induction weber 's electrodynamics]] |
Latest revision as of 20:11, 1 January 2017
Scientific Paper | |
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Title | Unipoplar Induction and Weber\'s Electrodynamics |
Author(s) | Andre K T Assis, Dario S Thober |
Keywords | unipolar induction, electrodynamics, conductor, magnet, relative rotary motion |
Published | 1994 |
Journal | None |
Pages | 409-414 |
Abstract
Unipolar induction is the generation of current on a conductor for the case in which the conductor and the magnet are in relative rotary motion. A typical case of unipolar induction is shown in figure 1. Since Faraday's experiments of 1932 on electromagnetic induction on rotation systems there are intense debates concerning the location of the seat of the electromotive force (emf)2.