Issue |
A&A
Volume 436, Number 2, June III 2005
|
|
---|---|---|
Page(s) | 503 - 526 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361:20042520 | |
Published online | 30 May 2005 |
Relativistic MHD simulations of extragalactic jets
1
Max-Planck-Institut für Astrophysik, Postfach 1312, 85741 Garching, Germany e-mail: maa@mpa-garching.mpg.de
2
Departamento de Astronomía y Astrofísica, Universidad de Valencia, 46100 Burjassot, Spain
3
Departamento de Física Aplicada, Universidad de Alicante, Ap. Correus 99, 03080 Alacant, Spain
Received:
10
December
2004
Accepted:
5
March
2005
We have performed a comprehensive parameter study of the morphology
and dynamics of axisymmetric, magnetized, relativistic jets by means
of numerical simulations. The simulations have been performed with
an upgraded version of the GENESIS code which is based on a
second-order accurate finite volume method involving an approximate
Riemann solver suitable for relativistic ideal magnetohydrodynamic
flows, and a method of lines. Starting from pure hydrodynamic
models we consider the effect of a magnetic field of increasing
strength (up to times the
equipartition value) and different topology (purely toroidal or
poloidal). We computed several series of models investigating the
dependence of the dynamics on the magnetic field in jets of
different beam Lorentz factor and adiabatic index.
We find that the inclusion of the magnetic field leads to diverse
effects which contrary to Newtonian magnetohydrodynamics models do
not always scale linearly with the (relative) strength of the
magnetic field. The relativistic models show, however, some clear
trends. Axisymmetric jets with toroidal magnetic fields produce a
cavity which consists of two parts: an inner one surrounding the
beam which is compressed by magnetic forces, and an adjacent outer
part which is inflated due to the action of the magnetic field. The
outer border of the outer part of the cavity is given by the
bow-shock where its interaction with the external medium takes
place. Toroidal magnetic fields well below equipartition (
) combined with a value of the adiabatic index of 4/3 yield
extremely smooth jet cavities and stable beams.
Prominent nose cones form when jets are confined by toroidal fields
and carry a high Poynting flux (
and
). In contrast, none of our models possessing a
poloidal field develops such a nose cone. The size of the nose cone
is correlated with the propagation speed of the Mach disc (the
smaller the speed the larger is the size). If two models differ
only by the adiabatic index, jets having smaller adiabatic indices
tend to develop smaller nose cones.
Key words: magnetohydrodynamics (MHD) / methods: numerical / relativity / galaxies: active / galaxies: jets
© ESO, 2005
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