1996
DOI: 10.1088/0264-9381/13/8/013
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Equilibrium of a charged test particle in the Kerr - Newman spacetime: force analysis

Abstract: In a previous work, we studied the equilibrium of a charged test particle placed in the combined gravitational and electromagnetic fields of a Kerr - Newman black hole. Recently, general relativistic analogues of inertial forces have been formulated. In this paper we analyse the inertial and the electromagnetic forces acting on the stationary test particle. This leads to an understanding of the behaviour of these forces as well as the mechanism of equilibrium.

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Cited by 16 publications
(21 citation statements)
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References 8 publications
(11 reference statements)
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“…Projecting the right-hand side of the Lorentz equation (A.4), we obtain the equation [19] qh i j F ik u k = E j + M j , (A. 13) where E j = qγF jk n j , (A.14)…”
Section: Discussionmentioning
confidence: 99%
“…Projecting the right-hand side of the Lorentz equation (A.4), we obtain the equation [19] qh i j F ik u k = E j + M j , (A. 13) where E j = qγF jk n j , (A.14)…”
Section: Discussionmentioning
confidence: 99%
“…For the uniform and axially symmetric rotation (32), the centrifugal force formula (56) reduces to formula (27). The embedding diagram ofΣ t equatorial plane is governed by the general embedding formula (51). Here, taking its particular form…”
Section: Conformal Transformation C = E −φmentioning
confidence: 99%
“…Thus, we arrive to covariant definition of inertial forces analogous to the Newtonian physics [2,17] …”
Section: General Casementioning
confidence: 99%