University of Vienna
Department of Astronomy
Tuerkenschanzstrasse 17
A-1180 Vienna
Austria
Tel: +43 1 4277 53815
peter.woitke&univie.ac.at
1. Observations
More than about 90% of all
stars, including our sun, will evolve into
so-called Asymptotic Giant Branch
(AGB) stars at the end of their life time, just before they run
out of fuel for nuclear burning. The "Asymptotic Giant Branch" is a
certain region in the
Hertzsprung-Russel diagram (c
John Lattanzio 2004), occupied by these stars, which become about
10000 times more luminous and about a factor of 2 cooler at the
surface than our present sun. AGB
stars may become as big as the orbit of Earth.
At such large radii, matter can easily be lifted
off from the stellar surface and expelled into space. In fact,
massive stellar winds appear in this stage which enforce a rather
sudden end of the stellar evolution due to mass loss. The mass loss rate of these winds ranges
about from 10-8 to 10-4 solar masses per year
(for comparison, the sun loses only about 10-14 solar
masses per year).
IRC+10216 at 2.2 micro-meter, evolution 1995-2001
(Weigelt et al. 2002, Astronomy and Astrophysics 392, p.131-141)
As a result of these massive stellar winds, the AGB stars are usually surrounded by
large quantities of gas and dust which partly absorb the stellar
radiation and thereby modify the spectral appearance of the stars.
Modern observations with high angular resolution reveal that this
surrounding matter often has an irregular clumpy structure, as e.g. in
the case of the infrared carbon star IRC+10216,
which is the brightest object on the sky at mid infrared wavelengths
(except for the sun). This object shows direct evidence for a clumpy
distribution of dust around the star which changes on timescales of
only a few years.
The final destiny of AGB
stars is to expel their complete outer shell into space as
so-called superwind, except for a tiny but hot white dwarf in the
center, the former core of the star, which remains. As soon as this
stellar remnant becomes visible and ionizes the surrounding matter
ejected before, the so-called Planetary Nebula (PN) phase is reached. PNs are often
asymmetrical, and in particular, show spectacular internal
structures. Here are a few examples:
The Eskimo Nebula, Hubble Space
Telescope, WFPC2
The Bug nebula, Hubble Space
Telescope, WFPC2
A zoomed-in picture from the
Helix nebula, WFPC2
The richness of spatial structures of gas and dust in the fossil
envelope of PNs is surprising and not very well understood so far. One
possible explanation is that the fromer AGB star wind was
not ejected in a spherically symmetric way, but already had a clumpy
internal structure at that time. As the central star gets bright in the
optical wavelength region, we can now see and study the details in the
fossil AGB star wind, which were dark and unobservable before.
Beside this relevance for related
objects like PNs, the winds of AGB
stars are important
for the formation of the first solid particles in space, in
particular the
seed particles which can only be formed in dense and warm environments,
and
to analyze and interpret AGB and post-AGB star observations.
2. Multi-dimensional
models for AGB star winds
The details of the mass loss
mechanismof AGB stars
are still
puzzling. Small solid particles ("dust grains") are expected to form
close
to the star, where the gas is dense and cool enough. These dust
particles absorb
the stellar photons and their momentum, which accelerates them outward,
and drag the gas along due to frictional forces.
Previous models have assumed that all these complicated chemical,
radiative and
dynamical processes occur in a stable, spherically symmetry way.
However, observations seem to tell a different story, and evidence for
chaotic, event-like dust formation epochs in only limited volumes are
numerous.
How
can we understand the chaotic winds of AGB stars?
We have performed axi-symmetric (2D) model calculations for AGB star
winds which combine hydrodynamics
with radiation pressure on dust grains, thermodynamics, chemistry,
time-dependent dust formation, and radiative transfer. These model
calculations show rather unexpected flow patterns, far away from
spherical symmetry:
log density
radial
velocity
degree of
condensation
This model shows the innermost dust
formation and wind acceleration region of a carbon-rich AGB star out to
a distance of 7 stellar radii after about 31 years of evolution. An
.mpeg-animation of the model (degree of condensation) can be downloaded
here (18MB).
3. Conclusions
We propose the following chaotic scenario for dust-driven AGB star
winds:
Excited by hydrodynamical, radiative or thermal instabilities, dust clouds are
formed from time to time in the dust
formation zone close to the star,
which are then accelerated outward due to radiation pressure on dust
grains. At the same
time, dust-free matter falls back towards this zone at different
places. A highly dynamical and
turbulent dust formation zone is created in this way, which - in
return - again bears a strongly inhomogeneous
dust distribution. Further away from the star, where flow
instabilities have time to amplify small disturbances (as e.g. the
Rayleigh-Taylor instability), the dust
arcs, lanes and clouds
produced in the dust formation zone are further shaped and modified.
In the presented model, the central star is assumed to be in
hydrostatic equilibrium. However, observations show that almost all AGB
stars are pulsating variables,
which produces waves which steepen up into shock waves in the large density
gradient of the stellar atmosphere. These pulsational shocks are well-known toinfluence the dust formation zone.
Moreover, the convective envelope of the AGB star is a source of sound waves with a wide spectrum of
wavelengths, which can also affect the dust and wind formation.
Therefore, besides improving the methods for radiative transfer in the
current model, we intend to study the impact of convection and
pulsation in future investigations.
The aim of this research project is
to understand the mass-loss mechanism
of AGB stars, to identify various instabilities and structure formation
processes occurring in these outflows, and to make qualified interpretations of high resolution
observational data.