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Physical analysis of Rastall PFRF black hole through accretion process

Hamood Ur RehmanDepartment of Mathematics, The Islamia University of Bahawalpur, Bahawalpur, PakistanG. AbbasDepartment of Mathematics, The Islamia University of Bahawalpur, Bahawalpur, PakistanAbdul JawadDepartment of Mathematics, COMSATS University Islamabad, Lahore-Campus, Lahore, 54000, PakistanRong-Jia YangCollege of Physics Science and Technology, Hebei University, Baoding, 071002, People’s Republic of ChinaG. MustafaDepartment of Physics, Zhejiang Normal University, Jinhua, 321004, People’s Republic of China
ABI

Аннотация

Abstract The adiabatic accretion onto the charged black hole surrounded by perfect fluid radiation field (PFRF) in Rastall gravity is addressed in this manuscript. For this purpose, mass accretion rate $$\dot{M}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>M</mml:mi> <mml:mo>˙</mml:mo> </mml:mover> </mml:math> , critical horizon radius and some other flow parameters are being determined in the presence of polytropic fluid. Overall the process is being done analytically. The location of critical points, polytropic gas compression ratios and temperature profiles are also being investigated for different versions of polytropic equation of state. We also give the comparison of the location of critical points with case of Schwarzschild black hole in which critical points lies out side the horizon. Through above scenario, it is found that charge Q and Rastall parameter $$N_{r}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>N</mml:mi> <mml:mi>r</mml:mi> </mml:msub> </mml:math> have deep effects on the accretion process. It is also mentioned here that under some constraints on parameters, our results reduce to Schwarzschild and charged black holes results.

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