A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions

We present a global magnetohydrodynamic (MHD) three dimensional simulation of a nonradiative accretion flow originating in a pressure supported torus. The evolution is controlled by the magnetorotational instability which produces turbulence. The flow forms a nearly Keplerian disk. The total pressur...

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Main Authors: Hawley, J, Balbus, S, Stone, J
Format: Journal article
Published: 2001
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author Hawley, J
Balbus, S
Stone, J
author_facet Hawley, J
Balbus, S
Stone, J
author_sort Hawley, J
collection OXFORD
description We present a global magnetohydrodynamic (MHD) three dimensional simulation of a nonradiative accretion flow originating in a pressure supported torus. The evolution is controlled by the magnetorotational instability which produces turbulence. The flow forms a nearly Keplerian disk. The total pressure scale height in this disk is comparable to the vertical size of the initial torus. Gas pressure dominates only near the equator; magnetic pressure is more important in the surrounding atmosphere. A magnetically dominated bound outflow is driven from the disk. The accretion rate through the disk exceeds the final rate into the hole, and a hot torus forms inside 10 r_g. Hot gas, pushed up against the centrifugal barrier and confined by magnetic pressure, is ejected in a narrow, unbound, conical outflow. The dynamics are controlled by magnetic turbulence, not thermal convection, and a hydrodynamic alpha model is inadequate to describe the flow. The limitations of two dimensional MHD simulations are also discussed.
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spelling oxford-uuid:116abbe7-9594-411e-b2fb-2303ce27260d2022-03-26T10:02:13ZA Magnetohydrodynamic Nonradiative Accretion Flow in Three DimensionsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:116abbe7-9594-411e-b2fb-2303ce27260dSymplectic Elements at Oxford2001Hawley, JBalbus, SStone, JWe present a global magnetohydrodynamic (MHD) three dimensional simulation of a nonradiative accretion flow originating in a pressure supported torus. The evolution is controlled by the magnetorotational instability which produces turbulence. The flow forms a nearly Keplerian disk. The total pressure scale height in this disk is comparable to the vertical size of the initial torus. Gas pressure dominates only near the equator; magnetic pressure is more important in the surrounding atmosphere. A magnetically dominated bound outflow is driven from the disk. The accretion rate through the disk exceeds the final rate into the hole, and a hot torus forms inside 10 r_g. Hot gas, pushed up against the centrifugal barrier and confined by magnetic pressure, is ejected in a narrow, unbound, conical outflow. The dynamics are controlled by magnetic turbulence, not thermal convection, and a hydrodynamic alpha model is inadequate to describe the flow. The limitations of two dimensional MHD simulations are also discussed.
spellingShingle Hawley, J
Balbus, S
Stone, J
A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions
title A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions
title_full A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions
title_fullStr A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions
title_full_unstemmed A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions
title_short A Magnetohydrodynamic Nonradiative Accretion Flow in Three Dimensions
title_sort magnetohydrodynamic nonradiative accretion flow in three dimensions
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