Асосий контентга ўтиш
AkademIndex

Маҳсулотлар

Ишлаб чиқувчилар учун

AkademBaseЭкотизим учун очиқ API
Мақола

A generalized Finch–Skea class one static solution

Ksh. Newton SinghDepartment of Mathematics, Jadavpur University, Kolkata, West Bengal, 700032, IndiaS. K. MauryaDepartment of Mathematical and Physical Sciences, College of Arts and Science, University of Nizwa, Nizwa, Sultanate of OmanFarook RahamanDepartment of Mathematics, Jadavpur University, Kolkata, West Bengal, 700032, IndiaFrancisco Tello‐OrtizDepartamento de Física, Facultad de ciencias básicas, Universidad de Antofagasta, Casilla 170, Antofagasta, Chile
2019en
ABI

Аннотация

In the present article, we discuss relativistic anisotropic solutions of Einstein field equations for the spherically symmetric line element under the class I condition. To do so we apply the embedding class one technique using Eisland condition. Within this approach, one arrives at a particular differential equation that links the two metric components $$e^{\nu }$$ and $$e^{\lambda }$$ . In order to obtain the full space–time description inside the stellar configuration we ansatz the generalized form of metric component $$g_{rr}$$ corresponding to the Finch–Skea solution. Once the space–time geometry is specified we obtain the complete thermodynamic description i.e. the matter density $$\rho $$ , the radial, and tangential pressures $$p_r$$ and $$p_t$$ , respectively. Graphical analysis shows that the obtained model respects the physical and mathematical requirements that all ultra-high dense collapsed structures must obey. The M–R diagram suggests that the solution yields stiffer EoS as parameter n increases. The M–I graph is in agreement with the concepts of Bejgar et al. (Mon Not R Astron Soc 364:635, 2005) that the mass at $$I_{max}$$ is lesser by few percent (for this solution $$\sim 3\%$$ ) from $$M_{max}$$ . This suggests that the EoSs is without any strong high-density softening due to hyperonization or phase transition to an exotic state.

Ҳали таржима қилинмаган

Идентификаторлар

Иқтибослар ва манбалар

2 та иқтибос0 та фойдаланилган манба