Abstract

Axisymmetric steady-state weakly ionized Hall-MHD Keplerian thin disks are investigated by using asymptotic expansions in the small disk aspect ratio \epsilon. The model incorporates the azimuthal and poloidal components of the magnetic fields in the leading order in \epsilon. The disk structure is described by an appropriate Grad-Shafranov equation for the poloidal flux function \psi that involves two arbitrary functions of \psi for the toroidal and poloidal currents. The flux function is symmetric about the midplane and satisfies certain boundary conditions at the near-horizontal disk edges. The boundary conditions model the combined effect of the primordial as well as the dipole-like magnetic fields. An analytical solution for the Hall equilibrium is achieved by further expanding the relevant equations in an additional small parameter \delta that is inversely proportional to the Hall parameter. It is thus found that the Hall equilibrium disks fall into two types: Keplerian disks with (i) small (Rd ~\delta^0) and (ii) large (Rd > \delta^k, k > 0) radius of the disk. The numerical examples that are presented demonstrate the richness and great variety of magnetic and density configurations that may be achieved under the Hall-MHD equilibrium.

Highlights

  • In the present study the Hall equilibrium of thin Keplerian disks embedded in 3D axially-symmetric magnetic fields is investigated

  • A more realistic model of thin disks is adopted in Regev ( 1983), Kluzniak & Kita (2000), Umurhan et al (2006) for equilibrium nonmagnetized rotating disks (see Ogilvie (1997) for Keplerian disks of ideal MHD plasmas) and is based on an asymptotic approach in the small aspect ratio of the disk

  • In such equilibria the electric potential as well as the toroidal magnetic field are arbitrary functions of the magnetic flux, while the density is an explicit function of the coordinates and the magnetic flux function which satisfies a GS type equation modified for the special case of Hall equilibrium in thin-disk approximation

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Summary

INTRODUCTION

In the present study the Hall equilibrium of thin Keplerian disks embedded in 3D axially-symmetric magnetic fields is investigated. A big variety of geometrical configurations of axially symmetric steady-state equilibria are described through a few arbitrary functions of the poloidal magnetic flux The latter satisfies the Grad-Shafranov (GS) type equations within both one-fluid and multifluid models of the plasmas (e.g. McClements & Thyagaraja (2001); Thyagaraja & McClements (2006), see the earlier study by Lovelace et al (1986), where in particular thin rotating disks have been discussed and references therein). A near Keplerian region of the rotating disk is considered that starts at some radial distance away from a central body The influence of the latter on the Keplerian portion of the disk is modeled by a dipole-like contribution (singular at the disk axis) to the boundary condition for the poloidal magnetic flux at the near-horizontal disk edges.

THE PHYSICAL MODEL FOR THIN KEPLERIAN DISKS
The basic equations
Scaling procedure
General relations
ANALYSIS OF THE EQUILIBRIUM IN TERMS OF THE SCALED INVERSE HALL PARAMETER
First family of solutions: small-radius disks
Second family of solutions: large-radius disks
NUMERICAL EXAMPLES
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