On the Global Stability of Magnetized Accretion Disks. II. Vertical and Azimuthal Magnetic Fields
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abstract
We investigate the global stability of a differentially rotating fluid shell
threaded by vertical and azimuthal magnetic fields to linear, axisymmetric
perturbations. This system, which models a thick accretion disk in the vicinity
of its midplane, is susceptible to the Velikhov-Chandrasekhar (VC) instability
in the absence of the azimuthal field. In most cases, the azimuthal field tends
to stabilize the VC instability, although strong fields (Alfv\'en speed of
order the characteristic rotational speed in our incompressible model) are
required for complete stabilization. Stability diagrams are constructed,
indicating critical values of the two fields for instability. We find an
additional strong field instability that arises when the azimuthal Alfv\'en
speed exceeds the characteristic rotational speed. This instability, in the
case of a freely bounded configuration, has certain similarities to the sausage
instability for interpenetrating fields in plasma physics, and may be important
for very massive disks or filamentary molecular clouds. An application to the
L1641 region in Orion A is briefly discussed. Finally, we find that the effect
of a radially varying vertical field (without an azimuthal field) is mainly
stabilizing.