Abstract

Pseudo-Newtonian potential has always been a useful tool to discuss the motion of a particle in space-time to avoid the tedious and nearly impossible nonlinear computations coming from the field equations of general relativity. Mukhopadhyay, in 2002, has introduced such a pseudo-Newtonian potential for rotating Kerr black hole which is efficient enough to replicate the scenario of the classical mechanics. But there was no such model to explain the dark energy realm. In 2016 Ghosh introduced a Lagrangian for such rotating black hole embedded in quintessence. in this article we obtained a pseudo-Newtonian force for this new black hole solution embedded quintessence. This paper introduces a simple computational scheme to evaluate a pseudo-Newtonian force for any space-time metric. This model possesses at most 4.95% error corresponding to general relativistic results. Since we took a popular agent of dark energy, i.e., quintessence into account, this is a general form of pseudo-Newtonian force to explain late time accelerating universe. In this paper, it also has been discussed about the difference between the pseudo-Newtonian force with and without dark energy effect. This paper also explains the natures of our present universe and its fate(locally around a black hole when repulsive negative pressure of dark energy is taken into account).

Highlights

  • In classical regime, the force acting on an orbiting particle is not just the gravitational force in its own reference frame but there exists a centrifugal force

  • We have shown a brand new and simple calculation scheme to evaluate PNF

  • We have started to obtain the PNF for a rotating Kerr BH

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Summary

Introduction

The force acting on an orbiting particle is not just the gravitational force in its own reference frame but there exists a centrifugal force. Even if we consider charge(as at the time of supernova explosions the electron of the outer layers flashes out with shocks leaving behind the preferably positively charged core which is collapsed to form a compact object) as we see in the Kerr–Newmann black hole, previously done by Ivanov and Prodanov [6] and they have considered the ratio of q and m for further comment but, it is difficult to analyze quantitatively the charge, due to lack of observational evidences, which makes the case with charge complicated It affects the surroundings when it is rotating. In the final section we will discuss our derived results in details

Basic calculations
Graphical interpretations
Findings
Brief discussions and conclusions
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