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Gravitational and Electromagnetic Field of an Isolated Positively Charged Particle
International Journal of Applied Mathematics and Theoretical Physics
Volume 6, Issue 4, December 2020, Pages: 54-60
Received: Oct. 24, 2020; Accepted: Nov. 20, 2020; Published: Nov. 27, 2020
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Bikash Kumar Borah, Department of Physics, Jorhat Institute of Science and Technology, Jorhat, India
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A particle which is positively charged with spherically symmetry and non-rotating in empty space is taken to find out a metric or line element. The particle is under the influence of both gravitational and electro-magnetic field and the time component of this metric is depend on the combine effect of these two fields. Therefore in this work especial attention is given in Einstein gravitational and Maxwell’s electro-magnetic field equations. Einstein field equations are individually considered for gravitational and electro-magnetic fields in empty space for an isolated charged particle and combined them like two classical waves. To solve this new metric initially Schwarzschild like solution is used. There after a simple elegant and systematic method is used to determine the value of space coefficient and time coefficient of the metric. Finally to solve the metric the e-m field tensor is used from Maxwell’s electro-magnetic field equations. Thus in the metric the values of space and time coefficient is found a new one. The space and time coefficient in the new metric is not same in the metric as devised by Reissner and Nordstrom, The new space and time coefficient gives such an information about the massive body that at particular mass of a body can stop electro-magnetic interaction. Thus the new metric able to gives us some new information and conclusions.
Metric, Gravitational Field, e-m Field, e-m Field Tensor
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Bikash Kumar Borah, Gravitational and Electromagnetic Field of an Isolated Positively Charged Particle, International Journal of Applied Mathematics and Theoretical Physics. Vol. 6, No. 4, 2020, pp. 54-60. doi: 10.11648/j.ijamtp.20200604.11
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