explanation      blue bibcodes open ADS page with paths to full text
Author name code: schaffenberger
ADS astronomy entries on 2022-09-14
author:"Schaffenberger, Werner" 

---------------------------------------------------------
Title: Properties of small-scale magnetism of stellar atmospheres
Authors: Steiner, Oskar; Salhab, René; Freytag, Bernd; Rajaguru,
   Paul; Schaffenberger, Werner; Steffen, Matthias
2014PASJ...66S...5S    Altcode: 2014PASJ..tmp...95S
  The magnetic field outside of sunspots is concentrated in the
  intergranular space, where it forms a delicate filigree of bright
  ribbons and dots as seen on broad band images of the Sun. We expect this
  small-scale magnetic field to exhibit a similar behavior in stellar
  atmospheres. In order to find out more about it, we perform numerical
  simulations of the surface layers of stellar atmospheres. Here, we
  report on preliminary results from simulations in the range between
  4000 K and 6500 K effective temperature with an initial vertical,
  homogeneous magnetic field of 50 G strength. We find that the field
  strength of the strongest magnetic flux concentrations increases with
  decreasing effective temperature at the height level where the average
  Rosseland optical depth is one. On the other hand, at the same level,
  the field is less strong than the thermal equipartition value in the
  coolest model but assumes superequipartition in the models hotter
  than 5000 K. While the Wilson depression of the strongest field
  concentrations is about one pressure scale height in the coolest
  model, it is more than four times the pressure scale height in the
  hottest one. We also find that the relative contribution of the bright
  filigree to the bolometric, vertically directed radiative intensity is
  most significant for the T<SUB>eff</SUB> = 5000 K model (0.6%-0.79%)
  and least significant for the hottest and coolest models (0.1%-0.46%
  and 0.14%-0.32%, respectively). This behavior suggests that the effect
  of the small-scale magnetic field on the photometric variability is more
  significant for K dwarf stars than for F-type and also M-type stars.

---------------------------------------------------------
Title: First steps with CO5BOLD using HLLMHD and PP reconstruction .
Authors: Steiner, O.; Rajaguru, S. P.; Vigeesh, G.; Steffen, M.;
   Schaffenberger, W.; Freytag, B.
2013MSAIS..24..100S    Altcode:
  We report on first experiences with real-life applications using
  the MHD-module of CO5BOLD together with the piecewise parabolic
  reconstruction scheme and present preliminary results of stellar
  magnetic models with T<SUB>eff</SUB> = 4000 K to T<SUB>eff</SUB> =
  5770 K.

---------------------------------------------------------
Title: Progress in modeling very low mass stars, brown dwarfs,
    and planetary mass objects.
Authors: Allard, F.; Homeier, D.; Freytag, B.; Schaffenberger, W.;
   Rajpurohit, A. S.
2013MSAIS..24..128A    Altcode: 2013arXiv1302.6559A
  We review recent advancements in modeling the stellar to substellar
  transition. The revised molecular opacities, solar oxygen abundances
  and cloud models allow to reproduce the photometric and spectroscopic
  properties of this transition to a degree never achieved before,
  but problems remain in the important M-L transition characteristic
  of the effective temperature range of characterizable exoplanets. We
  discuss of the validity of these classical models. We also present
  new preliminary global Radiation HydroDynamical M dwarfs simulations.

---------------------------------------------------------
Title: Simulations of stellar convection with CO5BOLD
Authors: Freytag, B.; Steffen, M.; Ludwig, H. -G.; Wedemeyer-Böhm,
   S.; Schaffenberger, W.; Steiner, O.
2012JCoPh.231..919F    Altcode: 2011arXiv1110.6844F
  High-resolution images of the solar surface show a granulation
  pattern of hot rising and cooler downward-sinking material - the
  top of the deep-reaching solar convection zone. Convection plays a
  role for the thermal structure of the solar interior and the dynamo
  acting there, for the stratification of the photosphere, where most
  of the visible light is emitted, as well as for the energy budget of
  the spectacular processes in the chromosphere and corona. Convective
  stellar atmospheres can be modeled by numerically solving the coupled
  equations of (magneto)hydrodynamics and non-local radiation transport
  in the presence of a gravity field. The CO5BOLD code described in this
  article is designed for so-called "realistic" simulations that take
  into account the detailed microphysics under the conditions in solar
  or stellar surface layers (equation-of-state and optical properties of
  the matter). These simulations indeed deserve the label "realistic"
  because they reproduce the various observables very well - with only
  minor differences between different implementations. The agreement
  with observations has improved over time and the simulations are now
  well-established and have been performed for a number of stars. Still,
  severe challenges are encountered when it comes to extending these
  simulations to include ideally the entire star or substellar object:
  the strong stratification leads to completely different conditions in
  the interior, the photosphere, and the corona. Simulations have to cover
  spatial scales from the sub-granular level to the stellar diameter and
  time scales from photospheric wave travel times to stellar rotation
  or dynamo cycle periods. Various non-equilibrium processes have to be
  taken into account. Last but not least, realistic simulations are based
  on detailed microphysics and depend on the quality of the input data,
  which can be the actual accuracy limiter. This article provides an
  overview of the physical problem and the numerical solution and the
  capabilities of CO5BOLD, illustrated with a number of applications.

---------------------------------------------------------
Title: Modification of wave propagation and wave travel-time by the
    presence of magnetic fields in the solar network atmosphere
Authors: Nutto, C.; Steiner, O.; Schaffenberger, W.; Roth, M.
2012A&A...538A..79N    Altcode:
  Context. Observations of waves at frequencies above the acoustic cut-off
  frequency have revealed vanishing wave travel-times in the vicinity of
  strong magnetic fields. This detection of apparently evanescent waves,
  instead of the expected propagating waves, has remained a riddle. <BR />
  Aims: We investigate the influence of a strong magnetic field on the
  propagation of magneto-acoustic waves in the atmosphere of the solar
  network. We test whether mode conversion effects can account for the
  shortening in wave travel-times between different heights in the solar
  atmosphere. <BR /> Methods: We carry out numerical simulations of the
  complex magneto-atmosphere representing the solar magnetic network. In
  the simulation domain, we artificially excite high frequency waves
  whose wave travel-times between different height levels we then
  analyze. <BR /> Results: The simulations demonstrate that the wave
  travel-time in the solar magneto-atmosphere is strongly influenced by
  mode conversion. In a layer enclosing the surface sheet defined by the
  set of points where the Alfvén speed and the sound speed are equal,
  called the equipartition level, energy is partially transferred from the
  fast acoustic mode to the fast magnetic mode. Above the equipartition
  level, the fast magnetic mode is refracted due to the large gradient
  of the Alfvén speed. The refractive wave path and the increasing phase
  speed of the fast mode inside the magnetic canopy significantly reduce
  the wave travel-time, provided that both observing levels are above
  the equipartition level. <BR /> Conclusions: Mode conversion and the
  resulting excitation and propagation of fast magneto-acoustic waves is
  responsible for the observation of vanishing wave travel-times in the
  vicinity of strong magnetic fields. In particular, the wave propagation
  behavior of the fast mode above the equipartition level may mimic
  evanescent behavior. The present wave propagation experiments provide an
  explanation of vanishing wave travel-times as observed with multi-line
  high-cadence instruments. <P />Movies are available in electronic form
  at <A href="http://www.aanda.org">http://www.aanda.org</A>

---------------------------------------------------------
Title: CO5BOLD: COnservative COde for the COmputation of COmpressible
    COnvection in a BOx of L Dimensions with l=2,3
Authors: Freytag, Bernd; Steffen, Matthias; Wedemeyer-Böhm, Sven;
   Ludwig, Hans-Günter; Leenaarts, Jorrit; Schaffenberger, Werner;
   Allard, France; Chiavassa, Andrea; Höfner, Susanne; Kamp, Inga;
   Steiner, Oskar
2010ascl.soft11014F    Altcode:
  CO5BOLD - nickname COBOLD - is the short form of "COnservative
  COde for the COmputation of COmpressible COnvection in a BOx of L
  Dimensions with l=2,3". <P />It is used to model solar and stellar
  surface convection. For solar-type stars only a small fraction of the
  stellar surface layers are included in the computational domain. In
  the case of red supergiants the computational box contains the entire
  star. Recently, the model range has been extended to sub-stellar objects
  (brown dwarfs). <P />CO5BOLD solves the coupled non-linear equations
  of compressible hydrodynamics in an external gravity field together
  with non-local frequency-dependent radiation transport. Operator
  splitting is applied to solve the equations of hydrodynamics (including
  gravity), the radiative energy transfer (with a long-characteristics
  or a short-characteristics ray scheme), and possibly additional 3D
  (turbulent) diffusion in individual sub steps. The 3D hydrodynamics
  step is further simplified with directional splitting (usually). The 1D
  sub steps are performed with a Roe solver, accounting for an external
  gravity field and an arbitrary equation of state from a table. <P
  />The radiation transport is computed with either one of three
  modules: <P />MSrad module: It uses long characteristics. The lateral
  boundaries have to be periodic. Top and bottom can be closed or open
  ("solar module"). <P />LHDrad module: It uses long characteristics
  and is restricted to an equidistant grid and open boundaries at all
  surfaces (old "supergiant module"). <P />SHORTrad module: It uses
  short characteristics and is restricted to an equidistant grid and
  open boundaries at all surfaces (new "supergiant module"). <P />The
  code was supplemented with an (optional) MHD version [Schaffenberger
  et al. (2005)] that can treat magnetic fields. There are also modules
  for the formation and advection of dust available. The current version
  now contains the treatment of chemical reaction networks, mostly used
  for the formation of molecules [Wedemeyer-Böhm et al. (2005)], and
  hydrogen ionization [Leenaarts &amp; Wedemeyer-Böhm (2005)], too. <P
  />CO5BOLD is written in Fortran90. The parallelization is done with
  OpenMP directives.

---------------------------------------------------------
Title: Supergranulation-Scale Convection Simulations
Authors: Stein, R. F.; Nordlund, Å.; Georgoviani, D.; Benson, D.;
   Schaffenberger, W.
2009ASPC..416..421S    Altcode:
  Results of realistic simulations of solar surface convection on the
  scale of supergranules (96 Mm wide by 20 Mm deep) are presented. The
  simulations cover only 10% of the geometric depth of the solar
  convection zone, but half its pressure scale heights. They include the
  hydrogen ionization zone, and the first and most of the second helium
  ionization zones. The horizontal velocity spectrum is a power law,
  and the horizontal size of the dominant convective cells increases
  with increasing depth. Convection is driven by buoyancy work, which
  is largest close to the surface, but significant over the entire
  domain. Close to the surface, buoyancy driving is balanced by the
  divergence of the kinetic energy flux, but deeper down it is balanced
  by dissipation. The damping length of the turbulent kinetic energy
  is 4 pressure scale heights. The mass mixing length is 1.8 scale
  heights. Two thirds of the area is upflowing fluid except very close
  to the surface. The internal (ionization) energy flux is the largest
  contributor to the convective flux for temperatures less than 40,000
  K and the thermal energy flux is the largest contributor at higher
  temperatures. This data set is useful for validating local helioseismic
  inversion methods. Sixteen hours of data are available as four hour
  averages, with two hour cadence, at steinr.msu.edu/~bob/96averages,
  as idl save files. The variables stored are the density, temperature,
  sound speed, and three velocity components. In addition, the three
  velocity components at 200 km above mean continuum optical depth unity
  are available at 30 second cadence.

---------------------------------------------------------
Title: The Horizontal Magnetic Field of the Quiet Sun: Numerical
    Simulations in Comparison to Observations with Hinode
Authors: Steiner, O.; Rezaei, R.; Schlichenmaier, R.; Schaffenberger,
   W.; Wedemeyer-Böhm, S.
2009ASPC..415...67S    Altcode: 2009arXiv0904.2030S
  Three-dimensional magnetohydrodynamic simulations of the surface layers
  of the Sun intrinsically produce a predominantly horizontal magnetic
  field in the photosphere. This is a robust result in the sense that it
  arises from simulations with largely different initial and boundary
  conditions for the magnetic field. While the disk-center synthetic
  circular and linear polarization signals agree with measurements from
  Hinode, their center-to-limb variation sensitively depends on the
  height variation of the horizontal and the vertical field component
  and they seem to be at variance with the observed behavior.

---------------------------------------------------------
Title: Supergranulation Scale Convection Simulations
Authors: Stein, R. F.; Lagerfjård, A.; Nordlund, Å.; Georgobiani,
   D.; Benson, D.; Schaffenberger, W.
2009ASPC..415...63S    Altcode:
  Results of realistic simulations of solar surface convection on
  the scale of supergranules (48 and 96 Mm wide by 20 Mm deep) are
  presented. The simulations include the hydrogen, first and most
  of the second helium ionization zones. Horizontal magnetic field is
  advected into the domain by upflows at the bottom. Upflows stretch the
  field lines upward, while downflows push them down, thus producing
  loop like magnetic structures. The mass mixing length is 1.8 scale
  heights. Two thirds of the area is upflowing fluid except very close
  to the surface. The internal (ionization) energy flux is the largest
  contributor to the convective flux for temperatures less than 40,000
  K and the thermal energy flux is the largest contributor at higher
  temperatures. The data is available for evaluating local helioseismic
  procedures.

---------------------------------------------------------
Title: Magnetohydrodynamic Characteristic Boundary Conditions
Authors: Schaffenberger, Werner; Stein, R.
2009SPD....40.0930S    Altcode:
  We implemented MHD characteristic boundary conditions for a non-ideal
  plasma in the "stagger-code" (Gudiksen and Nordlund, 2005, ApJ 618,
  1020). The aim of these boundary conditions is to reduce reflection
  at the boundaries which is important for the simulation of wave
  propagation. We present some test simulations of propagating waves
  demonstrating the capability of these boundary conditions.

---------------------------------------------------------
Title: Solar Magneto-Convection Simulations
Authors: Stein, Robert F.; Lagerfjard, A.; Nordlund, A.; Benson, D.;
   Georgobiani, D.; Schaffenberger, W.
2009SPD....40.0401S    Altcode:
  We present preliminary results of magneto-convection simulations
  of the rise of initially horizontal magnetic flux from 20 Mm deep
  through the solar surface in a domain 48 Mm wide. The magnetic field
  is stretched upward in the diverging upflows and pulled down in the
  downdrafts which produces a hierarchy of loop like structures. The
  strength varies with depth as the square root of the density. The field
  is swept to the boundaries of small supergranular like structures to
  form a magnetic network.

---------------------------------------------------------
Title: Supergranulation Scale Connection Simulations
Authors: Stein, R. F.; Nordlund, A.; Georgobiani, D.; Benson, D.;
   Schaffenberger, W.
2008arXiv0811.0472S    Altcode:
  Results of realistic simulations of solar surface convection on the
  scale of supergranules (96 Mm wide by 20 Mm deep) are presented. The
  simulations cover only 10% of the geometric depth of the solar
  convection zone, but half its pressure scale heights. They include the
  hydrogen, first and most of the second helium ionization zones. The
  horizontal velocity spectrum is a power law and the horizontal
  size of the dominant convective cells increases with increasing
  depth. Convection is driven by buoyancy work which is largest close
  to the surface, but significant over the entire domain. Close to the
  surface buoyancy driving is balanced by the divergence of the kinetic
  energy flux, but deeper down it is balanced by dissipation. The
  damping length of the turbulent kinetic energy is 4 pressure scale
  heights. The mass mixing length is 1.8 scale heights. Two thirds of the
  area is upflowing fluid except very close to the surface. The internal
  (ionization) energy flux is the largest contributor to the convective
  flux for temperatures less than 40,000 K and the thermal energy flux is
  the largest contributor at higher temperatures. This data set is useful
  for validating local helioseismic inversion methods. Sixteen hours
  of data are available as four hour averages, with two hour cadence,
  at steinr.msu.edu/~bob/96averages, as idl save files. The variables
  stored are the density, temperature, sound speed, and three velocity
  components. In addition, the three velocity components at 200 km above
  mean continuum optical depth unity are available at 30 sec. cadence.

---------------------------------------------------------
Title: Numerical Experiments with Magnetoacoustic Waves in the
    Solar Atmosphere
Authors: Nutto, C.; Schaffenberger, W.; Steiner, O.
2008ESPM...12.3.23N    Altcode:
  With numerical experiments we explore the feasibility of using high
  frequency waves for probing the magnetic field in the photosphere
  and the chromosphere of the Sun. We track monochromatic wave trains
  that propagates through a magnetically structured, realistic solar
  atmosphere. When entering the magnetically dominated chromosphere,
  the waves undergo partial mode conversion and get refracted and
  reflected. We explore the relationship between wave travel times and
  the topography of the surface of equal Alfven and sound speeds, viz.,
  the magnetic canopy.

---------------------------------------------------------
Title: The Horizontal Internetwork Magnetic Field: Numerical
    Simulations in Comparison to Observations with Hinode
Authors: Steiner, O.; Rezaei, R.; Schaffenberger, W.; Wedemeyer-Böhm,
   S.
2008ESPM...12.3.22S    Altcode:
  Observations with the Hinode space observatory led to the discovery
  of predominantly horizontal magnetic fields in the photosphere of the
  quiet internetwork region. Here we investigate realistic numerical
  simulations of the surface layers of the Sun with respect to horizontal
  magnetic fields and compute the corresponding polarimetric response
  in the Fe I 630 nm line pair. We find a local maximum in the mean
  strength of the horizontal field component at a height of around 500
  km in the photosphere, where, depending on the initial state or the
  boundary condition, it surpasses the vertical component by a factor
  of 2.0 or 5.6. From the synthesized Stokes profiles, we derive a mean
  horizontal field component that is 1.6 or 4.3 times stronger than
  the vertical component, depending on the initial state or the boundary
  condition. This is a consequence of both the intrinsically stronger flux
  density of and the larger area occupied by the horizontal fields. We
  find that convective overshooting expels horizontal fields to the upper
  photosphere, making the Poynting flux positive in the photosphere,
  whereas it is negative in the convectively unstable layer below it.

---------------------------------------------------------
Title: The Horizontal Internetwork Magnetic Field: Numerical
    Simulations in Comparison to Observations with Hinode
Authors: Steiner, O.; Rezaei, R.; Schaffenberger, W.; Wedemeyer-Böhm,
   S.
2008ApJ...680L..85S    Altcode: 2008arXiv0801.4915S
  Observations with the Hinode space observatory led to the discovery
  of predominantly horizontal magnetic fields in the photosphere of the
  quiet internetwork region. Here we investigate realistic numerical
  simulations of the surface layers of the Sun with respect to horizontal
  magnetic fields and compute the corresponding polarimetric response
  in the Fe I 630 nm line pair. We find a local maximum in the mean
  strength of the horizontal field component at a height of around 500
  km in the photosphere, where, depending on the initial state or the
  boundary condition, it surpasses the vertical component by a factor
  of 2.0 or 5.6. From the synthesized Stokes profiles, we derive a mean
  horizontal field component that is 1.6 or 4.3 times stronger than
  the vertical component, depending on the initial state or the boundary
  condition. This is a consequence of both the intrinsically stronger flux
  density of and the larger area occupied by the horizontal fields. We
  find that convective overshooting expels horizontal fields to the upper
  photosphere, making the Poynting flux positive in the photosphere,
  whereas the Poynting flux is negative in the convectively unstable
  layer below it.

---------------------------------------------------------
Title: Surface Convection
Authors: Stein, Robert F.; Benson, David; Georgobiani, Dali; Nordlund,
   Åke; Schaffenberger, Werner
2007AIPC..948..111S    Altcode:
  What are supergranules? Why do they stand out? Preliminary results from
  realistic simulations of solar convection on supergranule scales (96 Mm
  wide by 20 Mm deep) are presented. The solar surface velocity amplitude
  is a decreasing power law from the scale of granules up to giant cells
  with a slight enhancement at supergranule scales. The simulations show
  that the size of the horizontal convective cells increases gradually
  and continuously with increasing depth. Without magnetic fields
  present there is, as yet, no enhancement at supergranule scales at the
  surface. A hypothesis is presented that it is the balance between the
  rate of magnetic flux emergence and the horizontal sweeping of magnetic
  flux by convective motions that determines the size of the magnetic
  network and produces the extra power at supergranulation scales.

---------------------------------------------------------
Title: First local helioseismic experiments with CO<SUP>5</SUP>BOLD
Authors: Steiner, O.; Vigeesh, G.; Krieger, L.; Wedemeyer-Böhm, S.;
   Schaffenberger, W.; Freytag, B.
2007AN....328..323S    Altcode: 2007astro.ph..1029S
  With numerical experiments we explore the feasibility of using high
  frequency waves for probing the magnetic fields in the photosphere and
  the chromosphere of the Sun. We track a plane-parallel, monochromatic
  wave that propagates through a non-stationary, realistic atmosphere,
  from the convection-zone through the photosphere into the magnetically
  dominated chromosphere, where it gets refracted and reflected. We
  compare the wave travel time between two fixed geometrical height levels
  in the atmosphere (representing the formation height of two spectral
  lines) with the topography of the surface of equal magnetic and thermal
  energy density (the magnetic canopy or β=1 contour) and find good
  correspondence between the two. We conclude that high frequency waves
  indeed bear information on the topography of the `magnetic canopy'.

---------------------------------------------------------
Title: Holistic MHD-Simulation from the Convection Zone to the
    Chromosphere
Authors: Schaffenberger, W.; Wedemeyer-Böhm, S.; Steiner, O.;
   Freytag, B.
2006ASPC..354..345S    Altcode:
  A three-dimensional magnetohydrodynamic simulation of the integral
  layers from the convection zone to the chromosphere has been
  carried out. The simulation represents magnetoconvection in a quiet
  network-cell interior. The following preliminary new results are
  obtained: The chromospheric magnetic field is very dynamic with a
  continuous rearrangement of magnetic flux on a time scale of less than
  one~minute. Rapidly moving magnetic filaments (rarely exceeding 40~G)
  form in the compression zone downstream and along propagating shock
  fronts that are present throughout the chromosphere. The magnetic
  filaments rapidly move, form, and dissolve with the shock waves. Flux
  concentrations strongly expand through the photosphere into a more
  homogeneous, space filling chromospheric field. “Canopy fields”
  form on a granular scale above largely field-free granule centers
  leading to a mesh-work of current sheets in a height range between
  approximately 400 and 900~km.

---------------------------------------------------------
Title: Simulations of Magnetohydrodynamics and CO Formation from
    the Convection Zone to the Chromosphere
Authors: Wedemeyer-Böhm, S.; Schaffenberger, W.; Steiner, O.; Steffen,
   M.; Freytag, B.; Kamp, I.
2005ESASP.596E..16W    Altcode: 2005ccmf.confE..16W
  No abstract at ADS

---------------------------------------------------------
Title: Magnetohydrodynamic Simulation from the Convection Zone to
    the Chromosphere
Authors: Schaffenberger, W.; Wedemeyer-Böhm, S.; Steiner, O.;
   Freytag, B.
2005ESASP.596E..65S    Altcode: 2005ccmf.confE..65S
  No abstract at ADS

---------------------------------------------------------
Title: Analysis of mirror modes convected from the bow shock to
    the magnetopause
Authors: Erkaev, N. V.; Schaffenberger, W.; Biernat, H. K.; Farrugia,
   C. J.; Vogl, D. F.
2001P&SS...49.1359E    Altcode:
  Spacecraft observations confirm the existence of mirror fluctuations
  in the magnetosheath. The mirror instability occurs in an anisotropic
  magnetized plasma when the difference between perpendicular and
  parallel (with respect to the magnetic field) plasma pressure exceeds
  a threshold depending on the perpendicular plasma beta. The anisotropy
  of the plasma pressure increases from the shock to the magnetopause as
  a result of magnetic field line stretching. This gives rise to plasma
  fluctuations which in turn lead to a relaxation between parallel and
  perpendicular temperatures. Mirror perturbations do not propagate
  and are convected with plasma flow along the streamlines. Using an
  anisotropic steady-state MHD flow model, we calculate the growth
  of mirror fluctuations from the bow shock to the magnetopause along
  the subsolar streamline. For the anisotropic MHD model, we use the
  empirical closure equation suitable for the AMPTE/IRM observations. The
  amplitudes of mirror fluctuations, which are obtained as a function of
  distance from the magnetopause, are directly compared with AMPTE/IRM
  observations on October 24, 1985. With regard to both the amplification
  of the magnetic field and the plasma density oscillations, as well
  as the location of maximum amplitudes, model calculations are in good
  agreement with values obtained from the AMPTE/IRM data.

---------------------------------------------------------
Title: A Lattice Gas Model for Twodimensional Boussinesq Convection
Authors: Schaffenberger, W.; Hanslmeier, A.; Messerotti, M.
2001HvaOB..25...49S    Altcode:
  In this paper, we present a 2-D model for simulating the convection of
  an incompressible fluid between two walls of different temperatures. In
  particular, a bidimensional cellular automaton (CA) was developed to
  study the evolution of a discrete particle system, which represents a
  modified Frisch-Hasslacher-Pomeau (FHP) lattice gas. The derivation of
  the model equations and some relevant diagnostics, such as the Rayleigh,
  Prandtl and Nusselt numbers, are briefly outlined. The diagnostics
  computed for test runs indicate the consistency of the model as well
  as the preliminary simulation performed with a CA.

---------------------------------------------------------
Title: MHD effects of the solar wind flow around planets
Authors: Biernat, H. K.; Erkaev, N. V.; Farrugia, C. J.; Vogl, D. F.;
   Schaffenberger, W.
2000NPGeo...7..201B    Altcode:
  The study of the interaction of the solar wind with magnetized and
  unmagnetized planets forms a central topic of space research. Focussing
  on planetary magnetosheaths, we review some major developments in this
  field. Magnetosheath structures depend crucially on the orientation of
  the interplanetary magnetic field, the solar wind Alfvén Mach number,
  the shape of the obstacle (axisymmetric/non-axisymmetric, etc.), the
  boundary conditions at the magnetopause (low/high magnetic shear),
  and the degree of thermal anisotropy of the plasma. We illustrate the
  cases of Earth, Jupiter and Venus. The terrestrial magnetosphere is
  axisymmetric and has been probed in-situ by many spacecraft. Jupiter's
  magnetosphere is highly non-axisymmetric. Furthermore, we study
  magnetohydrodynamic effects in the Venus magnetosheath.

---------------------------------------------------------
Title: Cellular Automata Models for Convection
Authors: Schaffenberger, W.; Hanslmeier, A.; Messerotti, M.
1999ASSL..239..267S    Altcode: 1999msa..proc..267S
  We present here three models for convection. The models make use of
  the concept of cellular automata (CA). CA are discrete systems. The
  advantages of CA are their simple and parallel structure. The
  simplest of the presented models simulates two-dimensional Boussinesq
  convection. The two other models are extensions to compressible fluids
  and three-dimensional convection, respectively. We derive the model
  equations for the simplest model and present some of our results.

---------------------------------------------------------
Title: Simulating convection with cellular automata.
Authors: Schaffenberger, W.; Hanslmeier, A.; Messerotti, M.
1997AGAb...13..175S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: On the Influence of Supernova Shockfronts on the Stability
    of the Solar System
Authors: Schaffenberger, W.; Hanslmeier, A.
1997dbps.conf..393S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: Simulation of solar convection with cellular automata -
    first results.
Authors: Schaffenberger, W.; Hanslmeier, A.; Messerotti, M.
1997joso.proc...82S    Altcode:
  No abstract at ADS

---------------------------------------------------------
Title: A cellulare automaton for modelling the convection.
Authors: Schaffenberger, W.; Hanslmeier, A.; Messerotti, M.
1996AGAb...12..162S    Altcode:
  No abstract at ADS