Difference between revisions of "On Maxwell-Lorentz Equations"

From Natural Philosophy Wiki
Jump to navigation Jump to search
(Imported from text file)
 
(Imported from text file)
Line 15: Line 15:
 
==Abstract==
 
==Abstract==
  
In this paper, the Maxwell-Lorentz equations have been derived for a particle of mass  moving in the presence of other particles.  It is proved that the gravitational field due to a moving particle consist of i) an irrotational part (gradient of a scalar) and ii) a part depending on velocity  and a rotational part (curl of a vector).  Finally the Lorentz Force equation and the relativistic equation for planetary motion are derived.[[Category:Scientific Paper]]
+
In this paper, the Maxwell-Lorentz equations have been derived for a particle of mass  moving in the presence of other particles.  It is proved that the gravitational field due to a moving particle consist of i) an irrotational part (gradient of a scalar) and ii) a part depending on velocity  and a rotational part (curl of a vector).  Finally the Lorentz Force equation and the relativistic equation for planetary motion are derived.
 +
 
 +
[[Category:Scientific Paper|maxwell-lorentz equations]]
  
 
[[Category:Relativity]]
 
[[Category:Relativity]]

Revision as of 10:48, 1 January 2017

Scientific Paper
Title On Maxwell-Lorentz Equations
Read in full Link to paper
Author(s) M R Chandramohanan
Keywords {{{keywords}}}
Published 2010
Journal Proceedings of the NPA
Volume 7
Number 2
No. of pages 5
Pages 660-664

Read the full paper here

Abstract

In this paper, the Maxwell-Lorentz equations have been derived for a particle of mass moving in the presence of other particles. It is proved that the gravitational field due to a moving particle consist of i) an irrotational part (gradient of a scalar) and ii) a part depending on velocity and a rotational part (curl of a vector). Finally the Lorentz Force equation and the relativistic equation for planetary motion are derived.