American Journal of Modern Physics

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Gravitational Field of Non-conserving Mass Particle

Received: 24 May 2013    Accepted:     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.

DOI 10.11648/j.ajmp.20130204.17
Published in American Journal of Modern Physics (Volume 2, Issue 4, July 2013)
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), 2024. Published by Science Publishing Group

Keywords

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

References
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    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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    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
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Author Information
  • Dept. of Physics, Shri Chhatrapati Shivaji College, Omerga-413606, Maharashtra, India

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