2017
DOI: 10.1016/j.newast.2016.09.001
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Perturbation of mass accretion rate, associated acoustic geometry and stability analysis

Abstract: We investigate the stability of stationary integral solutions of an ideal irrotational fluid in a general static and spherically symmetric background, by studying the profile of the perturbation of the mass accretion rate. We consider low angular momentum axisymmetric accretion flows for three different accretion disk models and consider time dependent and radial linear perturbation of the mass accretion rate. First we show that the propagation of such perturbation can be determined by an effective 2 × 2 matri… Show more

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Cited by 23 publications
(30 citation statements)
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“…Moreover, we did not address this question from the point of view of an analytical stability analysis. Such analysis was provided by Moncrief (1980) for the spherical accretion onto non-rotating black hole and quite recently by Bollimpalli et al (2017) for low angular momentum flow with standing shocks, who also report the stability of the solution.…”
Section: Discussionmentioning
confidence: 96%
“…Moreover, we did not address this question from the point of view of an analytical stability analysis. Such analysis was provided by Moncrief (1980) for the spherical accretion onto non-rotating black hole and quite recently by Bollimpalli et al (2017) for low angular momentum flow with standing shocks, who also report the stability of the solution.…”
Section: Discussionmentioning
confidence: 96%
“…where H θ is the characteristic angular scale of the flow. Thus the continuity equation for vertically averaged axially symmetric accretion can be written as [15,17,65] ∂ t (ρv t −gH θ ) + ∂ r (ρv r −gH θ ) = 0 (13) whereg is the value of g, the determinant of the background metric g µν , on the equatorial plane. For Kerr metric g = − sin 2 θA 2 and thusg = −r 4 .…”
Section: Disc Structurementioning
confidence: 99%
“…For simplicity, therefore, we will write H θ simply as H 0 . Further details on different flow geometries can be found in [13,15,17]. From now on all the equations will be derived by assuming the flow to be vertically averaged and the variables have values equal to that in the equatorial plane.…”
Section: Disc Structurementioning
confidence: 99%
“…Now the perturbation on the stationary flow is done by following standard linear perturbation analysis [10,11,45,46] where acoustic space-time metric for conical flow was derived. Time-dependent accretion variables, like the components of four velocity and pressure are written as small time-dependent linear perturbations added their stationary values.…”
Section: Derivation Of Acoustic Metric From Linear Perturbation Of Fl...mentioning
confidence: 99%