paper

Heating of Accretion-Disk Coronae and Jets by General Relativistic MHD Turbulence

arXiv:1707.06216 · doi:10.1017/S0022377818000387

Abstract

Turbulence in an accretion disk launches Alfvén waves (AWs) that propagate away from the disk along magnetic field lines. Because the Alfvén speed varies with distance from the disk, the AWs undergo partial non-WKB reflection, and counter-propagating AWs subsequently interact, causing AW energy to cascade to small scales and dissipate. To investigate this process, we introduce an Elsasser-like formulation of general relativistic MHD (GRMHD) and develop the theory of general relativistic reduced MHD in an inhomogeneous medium. We then derive a set of equations for the mean-square AW amplitude and turbulent heating rate under the assumption that, in the plasma rest frame, AWs propagating away from the disk are much more energetic than AWs propagating toward the disk. For the case in which the background flow is axisymmetric and time-independent, we solve these equations analytically to determine and as functions of position. We find that, for an idealized thin disk threaded by a large-scale poloidal magnetic field, the AW energy flux is times the disk's radiative flux, where and are the mass densities at the coronal base and disk midplane, respectively, and is the ratio (evaluated at the disk midplane) of plasma-plus-radiation pressure to the pressure of the average vertical magnetic field. This energy flux could have a significant impact on disk coronae and outflows. To lay the groundwork for future global simulations of turbulent disk coronae and jets, we derive a set of averaged GRMHD equations that account for reflection-driven AW turbulence using a sub-grid model.

21 pages, no figures, accepted for publication in JPP. Version 2 contains more detail and a new section on a sub-grid model for incorporating turbulence into GRMHD simulations

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