Gravitational Field of Non-conserving Mass Particle

Ghanshyam H Jadhav

doi:doi:10.11648/j.ajmp.20130204.17

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Gravitational Field of Non-conserving Mass Particle

Ghanshyam H Jadhav

Published in American Journal of Modern Physics (Volume 2, Issue 4)

Received: 24 May 2013 Published: 30 June 2013

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Abstract

Gravitational field equations are written in the form of Maxwell’s type field equations. Lorentz gauge on the gravitational scalar and vector potentials is discarded by introducing a gravitational scalar field. It makes the mass particles to be time-dependent. The non-conserving part of the mass causes to produce the gravitational scalar field, which further con-tributes to the gravitational and gravitomagnetic vector fields. This contribution makes possible to produce a repulsive gravitational field by a decaying mass particle beyond a critical distance.

Published in	American Journal of Modern Physics (Volume 2, Issue 4)
DOI	10.11648/j.ajmp.20130204.17
Page(s)	220-222
Creative Commons	This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.
Copyright	Copyright © The Author(s), 2013. Published by Science Publishing Group

Keywords

Maxwell Type Gravitational Field Equations; Lorentz Gauge, Gravitational Potential, Gravitational Fields

References

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APA Style

Ghanshyam H Jadhav. (2013). Gravitational Field of Non-conserving Mass Particle. American Journal of Modern Physics, 2(4), 220-222. https://doi.org/10.11648/j.ajmp.20130204.17

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ACS Style

Ghanshyam H Jadhav. Gravitational Field of Non-conserving Mass Particle. Am. J. Mod. Phys. 2013, 2(4), 220-222. doi: 10.11648/j.ajmp.20130204.17

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AMA Style

Ghanshyam H Jadhav. Gravitational Field of Non-conserving Mass Particle. Am J Mod Phys. 2013;2(4):220-222. doi: 10.11648/j.ajmp.20130204.17

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@article{10.11648/j.ajmp.20130204.17,
  author = {Ghanshyam H Jadhav},
  title = {Gravitational Field of Non-conserving Mass Particle},
  journal = {American Journal of Modern Physics},
  volume = {2},
  number = {4},
  pages = {220-222},
  doi = {10.11648/j.ajmp.20130204.17},
  url = {https://doi.org/10.11648/j.ajmp.20130204.17},
  eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20130204.17},
  abstract = {Gravitational field equations are written in the form of Maxwell’s type field equations. Lorentz gauge on the gravitational scalar and vector potentials is discarded by introducing a gravitational scalar field. It makes the mass particles to be time-dependent. The non-conserving part of the mass causes to produce the gravitational scalar field, which further con-tributes to the gravitational and gravitomagnetic vector fields. This contribution makes possible to produce a repulsive gravitational field by a decaying mass particle beyond a critical distance.},
 year = {2013}
}

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TY  - JOUR
T1  - Gravitational Field of Non-conserving Mass Particle
AU  - Ghanshyam H Jadhav
Y1  - 2013/06/30
PY  - 2013
N1  - https://doi.org/10.11648/j.ajmp.20130204.17
DO  - 10.11648/j.ajmp.20130204.17
T2  - American Journal of Modern Physics
JF  - American Journal of Modern Physics
JO  - American Journal of Modern Physics
SP  - 220
EP  - 222
PB  - Science Publishing Group
SN  - 2326-8891
UR  - https://doi.org/10.11648/j.ajmp.20130204.17
AB  - Gravitational field equations are written in the form of Maxwell’s type field equations. Lorentz gauge on the gravitational scalar and vector potentials is discarded by introducing a gravitational scalar field. It makes the mass particles to be time-dependent. The non-conserving part of the mass causes to produce the gravitational scalar field, which further con-tributes to the gravitational and gravitomagnetic vector fields. This contribution makes possible to produce a repulsive gravitational field by a decaying mass particle beyond a critical distance.
VL  - 2
IS  - 4
ER  -

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Author Information

Ghanshyam H Jadhav

Dept. of Physics, Shri Chhatrapati Shivaji College, Omerga-413606, Maharashtra, India

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APA Style

Ghanshyam H Jadhav. (2013). Gravitational Field of Non-conserving Mass Particle. American Journal of Modern Physics, 2(4), 220-222. https://doi.org/10.11648/j.ajmp.20130204.17

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ACS Style

Ghanshyam H Jadhav. Gravitational Field of Non-conserving Mass Particle. Am. J. Mod. Phys. 2013, 2(4), 220-222. doi: 10.11648/j.ajmp.20130204.17

Copy | Download

AMA Style

Ghanshyam H Jadhav. Gravitational Field of Non-conserving Mass Particle. Am J Mod Phys. 2013;2(4):220-222. doi: 10.11648/j.ajmp.20130204.17

Copy | Download

@article{10.11648/j.ajmp.20130204.17,
  author = {Ghanshyam H Jadhav},
  title = {Gravitational Field of Non-conserving Mass Particle},
  journal = {American Journal of Modern Physics},
  volume = {2},
  number = {4},
  pages = {220-222},
  doi = {10.11648/j.ajmp.20130204.17},
  url = {https://doi.org/10.11648/j.ajmp.20130204.17},
  eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20130204.17},
  abstract = {Gravitational field equations are written in the form of Maxwell’s type field equations. Lorentz gauge on the gravitational scalar and vector potentials is discarded by introducing a gravitational scalar field. It makes the mass particles to be time-dependent. The non-conserving part of the mass causes to produce the gravitational scalar field, which further con-tributes to the gravitational and gravitomagnetic vector fields. This contribution makes possible to produce a repulsive gravitational field by a decaying mass particle beyond a critical distance.},
 year = {2013}
}

Copy | Download

TY  - JOUR
T1  - Gravitational Field of Non-conserving Mass Particle
AU  - Ghanshyam H Jadhav
Y1  - 2013/06/30
PY  - 2013
N1  - https://doi.org/10.11648/j.ajmp.20130204.17
DO  - 10.11648/j.ajmp.20130204.17
T2  - American Journal of Modern Physics
JF  - American Journal of Modern Physics
JO  - American Journal of Modern Physics
SP  - 220
EP  - 222
PB  - Science Publishing Group
SN  - 2326-8891
UR  - https://doi.org/10.11648/j.ajmp.20130204.17
AB  - Gravitational field equations are written in the form of Maxwell’s type field equations. Lorentz gauge on the gravitational scalar and vector potentials is discarded by introducing a gravitational scalar field. It makes the mass particles to be time-dependent. The non-conserving part of the mass causes to produce the gravitational scalar field, which further con-tributes to the gravitational and gravitomagnetic vector fields. This contribution makes possible to produce a repulsive gravitational field by a decaying mass particle beyond a critical distance.
VL  - 2
IS  - 4
ER  -

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