On Maxwell-Lorentz Equations: Difference between revisions
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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 12:48, 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.