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Hoek, Fizeau, and Einstein's Special Relativity: Difference between revisions

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==Abstract==
==Abstract==


One of the principal concerns of early experimenters in electromagnetism was the detection of a carrier for light waves (the aether). Theories in the mid 1800's ranged from that of Stokes, where it was assumed the aether was completely carried along by matter, to Fresnel and partial convection, to Maxwell and the universal aether, where light did not participate in the motion of matter in the slightest. The main problem in resolving the issue lay in an inability to obtain accuracy greater than first order in terrestrial experiments, because of the exceedingly small ratio between the velocities attainable for material objects and that of light (v/c).[[Category:Scientific Paper]]
One of the principal concerns of early experimenters in electromagnetism was the detection of a carrier for light waves (the aether). Theories in the mid 1800's ranged from that of Stokes, where it was assumed the aether was completely carried along by matter, to Fresnel and partial convection, to Maxwell and the universal aether, where light did not participate in the motion of matter in the slightest. The main problem in resolving the issue lay in an inability to obtain accuracy greater than first order in terrestrial experiments, because of the exceedingly small ratio between the velocities attainable for material objects and that of light (v/c).
 
[[Category:Scientific Paper|hoek fizeau einstein 's special relativity]]


[[Category:Relativity]]
[[Category:Relativity]]

Revision as of 13:31, 1 January 2017

Scientific Paper
TitleHoek, Fizeau, and Einstein\'s Special Relativity
Author(s)Walter Babin
KeywordsHoek, Fizeau, Special Relativity, Einstein
Published2008
JournalGeneral Science Journal
No. of pages4

Abstract

One of the principal concerns of early experimenters in electromagnetism was the detection of a carrier for light waves (the aether). Theories in the mid 1800's ranged from that of Stokes, where it was assumed the aether was completely carried along by matter, to Fresnel and partial convection, to Maxwell and the universal aether, where light did not participate in the motion of matter in the slightest. The main problem in resolving the issue lay in an inability to obtain accuracy greater than first order in terrestrial experiments, because of the exceedingly small ratio between the velocities attainable for material objects and that of light (v/c).