Difference between revisions of "Are Rotating and Translating Electromagnetic Systems Essentially Different?"
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The experimental detectability of absolute rotation in Mechanics (Foucault'S pendulum), in Optics (Michelson-Gale's 1925 interferometer) and in Electromagnetism (Faraday's unipolar inductor of 1832), contrasts with the undetectability of absolute and linear translation in Mechanics (Newtonian inertia), in Optics (Michelson-Morley 1887 experiment) and in Electromagnetism (Trouten-Noble 1903, Tomaschek 1927). Philosophical, mathematical and physical reasons are searched out for these well established experimental contrasts. Among the physical factors the relationship between the shape of a moving magnet in relationship to the geometry of its motional trajectory is singled out as having a crucial and unexpected importance. Similar considerations are extended to the optical experiments. | The experimental detectability of absolute rotation in Mechanics (Foucault'S pendulum), in Optics (Michelson-Gale's 1925 interferometer) and in Electromagnetism (Faraday's unipolar inductor of 1832), contrasts with the undetectability of absolute and linear translation in Mechanics (Newtonian inertia), in Optics (Michelson-Morley 1887 experiment) and in Electromagnetism (Trouten-Noble 1903, Tomaschek 1927). Philosophical, mathematical and physical reasons are searched out for these well established experimental contrasts. Among the physical factors the relationship between the shape of a moving magnet in relationship to the geometry of its motional trajectory is singled out as having a crucial and unexpected importance. Similar considerations are extended to the optical experiments. | ||
| − | [[Category:Scientific Paper]] | + | [[Category:Scientific Paper|rotating translating electromagnetic systems essentially different]] |
Latest revision as of 10:02, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Are Rotating and Translating Electromagnetic Systems Essentially Different? |
| Author(s) | Francisco J M?ller |
| Keywords | {{{keywords}}} |
| Published | 1997 |
| Journal | None |
Abstract
The experimental detectability of absolute rotation in Mechanics (Foucault'S pendulum), in Optics (Michelson-Gale's 1925 interferometer) and in Electromagnetism (Faraday's unipolar inductor of 1832), contrasts with the undetectability of absolute and linear translation in Mechanics (Newtonian inertia), in Optics (Michelson-Morley 1887 experiment) and in Electromagnetism (Trouten-Noble 1903, Tomaschek 1927). Philosophical, mathematical and physical reasons are searched out for these well established experimental contrasts. Among the physical factors the relationship between the shape of a moving magnet in relationship to the geometry of its motional trajectory is singled out as having a crucial and unexpected importance. Similar considerations are extended to the optical experiments.
