Difference between revisions of "Co-Lorentz Coordinate Transformations; Co-Einstein Special Relativity: Part I"

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The qualitative analysis of coordinate transformations, from the view-point of the reciprocity principle, allows the derivation of not only the Lorentz's transformation (LT), involving inertial motions, but also of a non-reciprocal transformation (N-LT), here called the Co-Lorentz transformation (Co-LT), valid for non-uniform motions. Consequently, relativistic kinematics is a double faced theory: it assumes either the LT, when the motion is inertial, or the Co-LT when the motion is non-inertial. The complementarity of LT and Co-LT implies the complementarity of the corresponding Einstein special relativity (ESR) and a non-reciprocal counter-part (N - ESR), here called Co-Einstein special relativity (Co-ESR). By neglecting gravitational effects, a relativistic electrodynamics, founded on Co-ESR is elaborated. Adding to the classical LT and ESR their corresponding complementary versions Co-LT and Co-ESR, a complete view of the special relativity of physical reality is obtained.  '''Motto:''' Extended Special Relativity is like the Moon which shows us only one of her faces: it is Einstein's SR. The hidden face is Hertz's SR.
 
The qualitative analysis of coordinate transformations, from the view-point of the reciprocity principle, allows the derivation of not only the Lorentz's transformation (LT), involving inertial motions, but also of a non-reciprocal transformation (N-LT), here called the Co-Lorentz transformation (Co-LT), valid for non-uniform motions. Consequently, relativistic kinematics is a double faced theory: it assumes either the LT, when the motion is inertial, or the Co-LT when the motion is non-inertial. The complementarity of LT and Co-LT implies the complementarity of the corresponding Einstein special relativity (ESR) and a non-reciprocal counter-part (N - ESR), here called Co-Einstein special relativity (Co-ESR). By neglecting gravitational effects, a relativistic electrodynamics, founded on Co-ESR is elaborated. Adding to the classical LT and ESR their corresponding complementary versions Co-LT and Co-ESR, a complete view of the special relativity of physical reality is obtained.  '''Motto:''' Extended Special Relativity is like the Moon which shows us only one of her faces: it is Einstein's SR. The hidden face is Hertz's SR.
  
[[Category:Scientific Paper]]
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[[Category:Scientific Paper|co-lorentz coordinate transformations co-einstein special relativity]]
  
 
[[Category:Relativity]]
 
[[Category:Relativity]]

Revision as of 10:09, 1 January 2017

Scientific Paper
Title Co-Lorentz Coordinate Transformations; Co-Einstein Special Relativity: Part I
Author(s) Constantin I Mocanu
Keywords Lorentz and Co-Lorentz coordinate transformations; Einstein and Co-Einstein special relativities
Published 1998
Journal Galilean Electrodynamics
Volume 9
Number 6
Pages 103-109

Abstract

The qualitative analysis of coordinate transformations, from the view-point of the reciprocity principle, allows the derivation of not only the Lorentz's transformation (LT), involving inertial motions, but also of a non-reciprocal transformation (N-LT), here called the Co-Lorentz transformation (Co-LT), valid for non-uniform motions. Consequently, relativistic kinematics is a double faced theory: it assumes either the LT, when the motion is inertial, or the Co-LT when the motion is non-inertial. The complementarity of LT and Co-LT implies the complementarity of the corresponding Einstein special relativity (ESR) and a non-reciprocal counter-part (N - ESR), here called Co-Einstein special relativity (Co-ESR). By neglecting gravitational effects, a relativistic electrodynamics, founded on Co-ESR is elaborated. Adding to the classical LT and ESR their corresponding complementary versions Co-LT and Co-ESR, a complete view of the special relativity of physical reality is obtained. Motto: Extended Special Relativity is like the Moon which shows us only one of her faces: it is Einstein's SR. The hidden face is Hertz's SR.