2003
DOI: 10.1086/379339
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The Fate of Nonradiative Magnetized Accretion Flows: Magnetically Frustrated Convection

Abstract: We present a scenario for non-radiative accretion onto the supermassive black hole at the galactic center. Conducting MHD simulations with 1400 3 grid zones that break the axial and reflection symmetries of earlier investigations and extend inward from the Bondi radius, we find a quasi-hydrostatic radial density profile ρ ∝ r −0.72 with superadiabatic gradient corresponding to an n ∼ 0.72 polytrope. Buoyancy generated by magnetic dissipation is resisted by the same fields so effectively that energy is advected… Show more

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Cited by 74 publications
(69 citation statements)
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“…[See the electronic edition of the Journal for a color version of this figure. ] correspond to generalized wind models (Blandford & Begelman 1999). Numerical hydro and MHD simulations give s 0 anywhere in the range from about 0.7 to 1 (Igumenshchev et al , 2003Pen et al 2003). On the other hand, a model for the accreting supermassive black hole Sgr A Ã at the Galactic center gives s 0 $ 0:3 (Yuan et al 2003).…”
Section: More Quantitative Resultsmentioning
confidence: 97%
“…[See the electronic edition of the Journal for a color version of this figure. ] correspond to generalized wind models (Blandford & Begelman 1999). Numerical hydro and MHD simulations give s 0 anywhere in the range from about 0.7 to 1 (Igumenshchev et al , 2003Pen et al 2003). On the other hand, a model for the accreting supermassive black hole Sgr A Ã at the Galactic center gives s 0 $ 0:3 (Yuan et al 2003).…”
Section: More Quantitative Resultsmentioning
confidence: 97%
“…Future observations of PSRJ1745−2900 will better constrain the magnetic field structure around SgrA * and can potentially be used to test if the accretion flow becomes magnetically dominated (Pen et al 2003).…”
Section: A Physical Model Based On the Depolarizationmentioning
confidence: 99%
“…Numerous two-and three-dimensional global simulations of RIAFs have been performed in hydrodynamics (2D- Stone et al 19993D-Igumenshchev et al 2000) as well as in magnetohydrodynamics (MHD; 2D- Stone & Pringle 2001;3D-Hawley et al 2001, Machida et al 2001, Hawley & Balbus 2002, Igumenshchev et al 2003, Pen et al 2003, Pang et al 2011, McKinney et al 2012, Narayan et al 2012. A key conclusion of most such simulations to date is that the net accretion rate through the inner edge of the torus at r = r in is substantially reduced (by a factor ∼r in /R 0 ) from the feeding rate set by the outer torus at r = R 0 , consistent with both CDAF and ADIOS models (e.g., Yuan et al 2012).…”
Section: Introductionmentioning
confidence: 99%