1999
DOI: 10.1051/aas:1999462
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A nonlinear convective model for radial stellar pulsations

Abstract: Abstract. The physical and numerical ingredients of the Vienna nonlinear model for radially pulsating stars are presented. Stellar pulsations are investigated by solving the full system of radiation hydrodynamics including a time-dependent formulation of turbulent convection. The numerical solution method comprises a state-of-the-art adaptive grid algorithm which provides a powerful tool for resolving and tracking the most important ionization zones. Several already published applications to pulsating stars in… Show more

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Cited by 32 publications
(23 citation statements)
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References 17 publications
(21 reference statements)
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“…Yecko et al 1998 and references therein). Despite the lack of a robust theory, it has now become clear that convective energy transport is essential to describe the observed properties of pulsating stars such as light curves or Fourier coefficients (Yecko et al 1998;Feuchtinger 1999;Feuchtinger et al 2000).…”
Section: Uncertainties On Distance Determinationmentioning
confidence: 99%
“…Yecko et al 1998 and references therein). Despite the lack of a robust theory, it has now become clear that convective energy transport is essential to describe the observed properties of pulsating stars such as light curves or Fourier coefficients (Yecko et al 1998;Feuchtinger 1999;Feuchtinger et al 2000).…”
Section: Uncertainties On Distance Determinationmentioning
confidence: 99%
“…This formalism for the viscosity in the radial direction closely resembles -except of course for the shear part -the customary 1D viscosity description given, e.g., by Dorfi (1998) or Feuchtinger (1999a. In the horizontal direction, discretization yields a viscous force…”
Section: Artificial Viscositymentioning
confidence: 70%
“…The inclusion of the convective stellar mantle in the model requires the use of either a three-dimensional approach (such as presented by Freytag & Höfner 2008) or a description for turbulent energy (see e.g. Kuhfuß 1986;Gehmeyr & Winkler 1992;Canuto & Dubovikov 1998;Wuchterl & Feuchtinger 1998;Feuchtinger 1999), which implies a number of additional free parameters. It should, however, be possible to set many of these new parameters to default values.…”
Section: Modeling Mass-loss Formation Near the Tip Of The Agbmentioning
confidence: 99%