2005 47th Annual Meeting of the Division of Plasma Physics
Monday–Friday, October 24–28, 2005;
Denver, Colorado
Session RI1b: Space and Astrophysical Plasmas II
3:00 PM–5:00 PM,
Thursday, October 27, 2005
Adam's Mark Hotel
Room: Plaza Ballroom ABC
Chair: Annick Pouquet, National Center for Atmospheric Research
Abstract ID: BAPS.2005.DPP.RI1b.2
Abstract: RI1b.00002 : Turbulence and Plasma Physics in Clusters of Galaxies*
3:30 PM–4:00 PM
Preview Abstract
Abstract
Author:
Alexander Schekochihin
(University of Cambridge)
The intracluster medium appears to be in a turbulent state. It
is also threaded by
randomly tangled magnetic fields. In the past few years there
has been a dramatic
increase in the quantity and quality of observational data on
cluster turbulence and
magnetic fields. The observed magnetic fields are strong enough
to be dynamically
important. The turbulence and magnetic field regulate the
viscous heating and heat
transport that determine the thermal structure of clusters. A
coherent theory of
magnetized cluster turbulence is necessary for understanding
cluster behaviour on
both large and small scales. The strength and certainly the
structure of the cluster
fields are determined by their interaction with the turbulence.
This talk will first
describe the fundamental properties of the turbulent generation
of magnetic fields:
(1) what type of field structure can be produced and maintained;
(2) how a dynamical saturated state is achieved;
(3) what are the observable signatures of the field structure
in clusters.
The field structure in no small measure depends on the nature
of the viscous and
magnetic cutoffs. These are determined by the plasma physics of
the intracluster
medium, which has very low collisionality. It will be shown
that, under very general
conditions, cluster plasmas threaded by weak magnetic fields
are subject to firehose
and mirror instabilities. These are driven by the anisotropies
of the plasma pressure
(viscous stress) that naturally arise in any weakly magnetized
plasma that has low
collisionality and is subject to stirring. The effect is
captured by the extended MHD
model with Braginskii viscosity, but, as the instability growth
rates are proportional
to the wavenumber down to the ion gyroscale, MHD equations with
Braginskii
viscosity are not well posed and a fully kinetic description
is necessary. The
instabilities may lead to the amplification of magnetic fields
in clusters to the
observed strength of $\sim10\mu$G on cosmologically trivial
time
scales ($\sim10^8$~yr). The saturation of the instabilities
controls the effective
transport properties of the cluster plasmas.
*Work supported by the UKAFF Fellowship
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2005.DPP.RI1b.2