Difference between revisions of "The Paradox of Thomas Rotation"

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==Abstract==
 
==Abstract==
  
In order to extend the 1 + 1 Lorentz transformation to one with 1 + 3 dimensions, the so-called Thomas rotation is inevitably involved.&nbsp;This, in turn, provides the relativistic interpretations of the non-commutative and non-associative composition laws of non-collinear velocities.&nbsp;When dealing with two successive Lorentz transformations involving non-collinear velocities, two peculiarities are revealed. The first is related to the vector-scaler pair ('''J''', <em>p</em>''') and the second to the vector pair (E, B'''); neither implies the Thomas rotation. Ungar's attempt to solve these difficulties by applying the Thomas rotation if invalidated by the conservation law of the electromagnetic field. The result is a paradox revealing an internal contradiction of the Special Theory of Relativity.[[Category:Scientific Paper]]
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In order to extend the 1 + 1 Lorentz transformation to one with 1 + 3 dimensions, the so-called Thomas rotation is inevitably involved.&nbsp;This, in turn, provides the relativistic interpretations of the non-commutative and non-associative composition laws of non-collinear velocities.&nbsp;When dealing with two successive Lorentz transformations involving non-collinear velocities, two peculiarities are revealed. The first is related to the vector-scaler pair ('''J''', <em>p</em>''') and the second to the vector pair (E, B'''); neither implies the Thomas rotation. Ungar's attempt to solve these difficulties by applying the Thomas rotation if invalidated by the conservation law of the electromagnetic field. The result is a paradox revealing an internal contradiction of the Special Theory of Relativity.
  
[[Category:Relativity]]
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[[Category:Scientific Paper|paradox thomas rotation]]
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[[Category:Relativity|paradox thomas rotation]]

Latest revision as of 20:05, 1 January 2017

Scientific Paper
Title The Paradox of Thomas Rotation
Author(s) Constantin I Mocanu
Keywords Thomas rotation, non-collinear velocities, electromagnetic field, (STR)
Published 1991
Journal Galilean Electrodynamics
Volume 2
Number 4
Pages 67-74

Abstract

In order to extend the 1 + 1 Lorentz transformation to one with 1 + 3 dimensions, the so-called Thomas rotation is inevitably involved. This, in turn, provides the relativistic interpretations of the non-commutative and non-associative composition laws of non-collinear velocities. When dealing with two successive Lorentz transformations involving non-collinear velocities, two peculiarities are revealed. The first is related to the vector-scaler pair (J, p) and the second to the vector pair (E, B); neither implies the Thomas rotation. Ungar's attempt to solve these difficulties by applying the Thomas rotation if invalidated by the conservation law of the electromagnetic field. The result is a paradox revealing an internal contradiction of the Special Theory of Relativity.