An Interior model of Charged Fluid Spheres
Naren Babu O., Hemalatha. R, Narayanankutty Karuppath, Sabu M. C
TL;DR
The paper addresses the interior structure of charged fluid spheres within a spheroidal spacetime by employing the Vaidya–Tikekar metric and solving the Einstein–Maxwell equations. It prescribes an electric-field profile $E^2(r)$ to reduce the system to a hypergeometric differential equation for $e^{\nu/2}$, yielding a general solution in terms of ${}_2F_1$ and a physically viable closed-form for the special case $k=-23$. The main contributions include a new class of exact, physically acceptable charged fluid solutions, a computational scheme to determine mass $m$, radius $a$, and charge $q$ from boundary data, and a demonstration that the models satisfy hydrostatic equilibrium and standard energy conditions while matching smoothly to a Reissner–Nordström exterior. The work provides analytic interior models for ultra-dense charged matter and a framework for exploring mass-radius-charge relations of compact stars under charge, with potential implications for the structure of highly compact astrophysical objects.
Abstract
At constant time $t$, we examine the Vaidya-Tikekar metric characterising a three-dimensional, extremely dense spheroidal star configuration. The static, spherically symmetric solution of Einstein's field equations can be expressed in analytic closed form utilising a hypergeometric series. A relativistic, superdense state of matter at a constant $t$ is represented by the resultant model, which describes the geometry of a three-spheroid. Assuming a stellar density of $ρ_{a}= 2*10^{14} gm*cm^{-3}$, we investigate configurations whose total mass and radius vary over a range of well-defined values of the density variation parameter. Similar to an uncharged neutron star, all models possess the same total mass and boundary radius. The hypergeometric solution leads to a new class of exact, physically acceptable solutions. We show that the model satisfies the conditions of hydrostatic equilibrium and fulfils all standard energy conditions, which are verified throughout the analysis.
