2021
DOI: 10.1140/epjc/s10052-021-08894-3
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An electromagnetic extension of the Schwarzschild interior solution and the corresponding Buchdahl limit

Abstract: We wish to construct a model for charged star as a generalization of the uniform density Schwarzschild interior solution. We employ the Vaidya and Tikekar ansatz (Astrophys Astron 3:325, 1982) for one of the metric potentials and electric field is chosen in such a way that when it is switched off the metric reduces to the Schwarzschild. This relates charge distribution to the Vaidya–Tikekar parameter, k, indicating deviation from sphericity of three dimensional space when embedded into four dimensional Euclide… Show more

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Cited by 22 publications
(7 citation statements)
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“…[77]. For in depth discussions about the stability of charged spheres have been found in [79][80][81][82]. In Ref.…”
Section: Introductionmentioning
confidence: 99%
“…[77]. For in depth discussions about the stability of charged spheres have been found in [79][80][81][82]. In Ref.…”
Section: Introductionmentioning
confidence: 99%
“…The first interior solution of the Einstein gravitational field equations was obtained by Schwarzschild in 1916 [61] under the assumption of the constant density of the star. It has a remarkable mathematical simplicity, and despite the fact that it is generally considered as not providing a realistic description of neutron stars, its properties have been intensively investigated [62]. In particular, for constant density stars the Buchdahl bound becomes exact, so that 2M/R = 8/9.…”
Section: A Constant Density Starsmentioning
confidence: 99%
“…The probe also prescribes an upper bound on the charge to mass ratio Q 2 /M 2 ≤ 9/8. In a recent article, by developing a model for charged star which was shown to be a generalization of the uniform density Schwarzschild interior solution, Sharma et al [3] regained the charged analogue of the Buchdahl compactness bound…”
Section: Introductionmentioning
confidence: 99%