Unipoplar Induction and Weber's Electrodynamics: Difference between revisions
Imported from text file |
Imported from text file |
||
| Line 10: | Line 10: | ||
==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>.[[Category:Scientific Paper]] | 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:Scientific Paper|unipoplar induction weber 's electrodynamics]] | |||
[[Category:New Energy]] | [[Category:New Energy]] | ||
Revision as of 13:35, 1 January 2017
| Scientific Paper | |
|---|---|
| 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.