Anisotropic fluid spheres of embedding class one using Karmarkar condition

Abstract We obtain a new anisotropic solution for spherically symmetric spacetimes by analyzing the Karmarkar embedding condition. For this purpose we construct a suitable form of one of the gravitational potentials to obtain a closed form solution. This form of the remaining gravitational potential...

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Main Authors: S. K. Maurya, S. D. Maharaj
Format: Article
Language:English
Published: SpringerOpen 2017-05-01
Series:European Physical Journal C: Particles and Fields
Subjects:
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-4905-7
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spelling doaj-850e0327220346bd873c30587ab303442020-11-24T21:42:10ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-05-0177511310.1140/epjc/s10052-017-4905-7Anisotropic fluid spheres of embedding class one using Karmarkar conditionS. K. Maurya0S. D. Maharaj1Department of Mathematical and Physical Sciences, College of Arts and Science, University of NizwaAstrophysics and Cosmology Research Unit, School of Mathematics, Statistics and Computer Science, University of KwaZulu-NatalAbstract We obtain a new anisotropic solution for spherically symmetric spacetimes by analyzing the Karmarkar embedding condition. For this purpose we construct a suitable form of one of the gravitational potentials to obtain a closed form solution. This form of the remaining gravitational potential allows us to solve the embedding equation and integrate the field equations. The resulting new anisotropic solution is well behaved, which can be utilized to construct realistic static fluid spheres. Also we estimated the masses and radii of fluid spheres for LMC X-4, EXO 1785-248, PSR J1903+327 and 4U 1820-30 by using observational data set values. The masses and radii obtained show that our anisotropic solution can represent fluid spheres to a very good degree of accuracy. The physical validity of the solution depends on the parameter values of a, b and c. The solution is well behaved for the wide range of parameters values $$0.00393\le a \le 0.0055$$ 0.00393 ≤ a ≤ 0.0055 , $$0.0002 \le b \le 0.0025$$ 0.0002 ≤ b ≤ 0.0025 and $$0.0107 \le c \le 0.0155$$ 0.0107 ≤ c ≤ 0.0155 . The range of corresponding physical parameters for the different compact stars are $$0.3266\le v_{r0} \le 0.3708$$ 0.3266 ≤ v r 0 ≤ 0.3708 , $$0.1583\le v_{t0} \le 0.2558$$ 0.1583 ≤ v t 0 ≤ 0.2558 , $$0.3256\le z_{s} \le 0.4450$$ 0.3256 ≤ z s ≤ 0.4450 and $$4.3587\le \Gamma _{0} \le 5.6462$$ 4.3587 ≤ Γ 0 ≤ 5.6462 .http://link.springer.com/article/10.1140/epjc/s10052-017-4905-7Radial PressureCompact StarAdiabatic IndexEinstein Field EquationFluid Sphere
collection DOAJ
language English
format Article
sources DOAJ
author S. K. Maurya
S. D. Maharaj
spellingShingle S. K. Maurya
S. D. Maharaj
Anisotropic fluid spheres of embedding class one using Karmarkar condition
European Physical Journal C: Particles and Fields
Radial Pressure
Compact Star
Adiabatic Index
Einstein Field Equation
Fluid Sphere
author_facet S. K. Maurya
S. D. Maharaj
author_sort S. K. Maurya
title Anisotropic fluid spheres of embedding class one using Karmarkar condition
title_short Anisotropic fluid spheres of embedding class one using Karmarkar condition
title_full Anisotropic fluid spheres of embedding class one using Karmarkar condition
title_fullStr Anisotropic fluid spheres of embedding class one using Karmarkar condition
title_full_unstemmed Anisotropic fluid spheres of embedding class one using Karmarkar condition
title_sort anisotropic fluid spheres of embedding class one using karmarkar condition
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2017-05-01
description Abstract We obtain a new anisotropic solution for spherically symmetric spacetimes by analyzing the Karmarkar embedding condition. For this purpose we construct a suitable form of one of the gravitational potentials to obtain a closed form solution. This form of the remaining gravitational potential allows us to solve the embedding equation and integrate the field equations. The resulting new anisotropic solution is well behaved, which can be utilized to construct realistic static fluid spheres. Also we estimated the masses and radii of fluid spheres for LMC X-4, EXO 1785-248, PSR J1903+327 and 4U 1820-30 by using observational data set values. The masses and radii obtained show that our anisotropic solution can represent fluid spheres to a very good degree of accuracy. The physical validity of the solution depends on the parameter values of a, b and c. The solution is well behaved for the wide range of parameters values $$0.00393\le a \le 0.0055$$ 0.00393 ≤ a ≤ 0.0055 , $$0.0002 \le b \le 0.0025$$ 0.0002 ≤ b ≤ 0.0025 and $$0.0107 \le c \le 0.0155$$ 0.0107 ≤ c ≤ 0.0155 . The range of corresponding physical parameters for the different compact stars are $$0.3266\le v_{r0} \le 0.3708$$ 0.3266 ≤ v r 0 ≤ 0.3708 , $$0.1583\le v_{t0} \le 0.2558$$ 0.1583 ≤ v t 0 ≤ 0.2558 , $$0.3256\le z_{s} \le 0.4450$$ 0.3256 ≤ z s ≤ 0.4450 and $$4.3587\le \Gamma _{0} \le 5.6462$$ 4.3587 ≤ Γ 0 ≤ 5.6462 .
topic Radial Pressure
Compact Star
Adiabatic Index
Einstein Field Equation
Fluid Sphere
url http://link.springer.com/article/10.1140/epjc/s10052-017-4905-7
work_keys_str_mv AT skmaurya anisotropicfluidspheresofembeddingclassoneusingkarmarkarcondition
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