Models for Weak Wind and Momentum Problems in the Winds of Hot Stars

We pesent models for the velocity structure in the supersonic part of hot star winds in order to estimate the effects of clumping in density and velocity. XSTAR (Kallman,2018) was used to calculate radiation pressure in spectral lines (force multiplier FM) in Sobolev approximation (Castor et al., 19...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Hauptverfasser: Vilhu, Osmi, Kallman, Timothy R
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext bestellen
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:We pesent models for the velocity structure in the supersonic part of hot star winds in order to estimate the effects of clumping in density and velocity. XSTAR (Kallman,2018) was used to calculate radiation pressure in spectral lines (force multiplier FM) in Sobolev approximation (Castor et al., 1975 CAK; Stevens and Kallman, 1990). FM was computed as a function of two parameters: Xi and t. The line force was included in the momentum equation and mass conservation. These were integrated in the supersonic part of the wind for a sample of OB- and WR-stars. Fitting with the velocity-law gives mass loss rate and outflow velocity as outputs. The boundary condition of the subsonic part and the velocity law were approximated by using a beta-law formulation with beta = 0.6 and Vin = 10 km/s. It is found that WR-stars , owing to their large absorption, had already at r/Rstar = 1.01 radiation spectra lacking soft X-rays below 230 Angstroem (HeII ionization). This crucial fact enhances the force multiplier by a factor of 10, making it possible to accelerate their winds in the CAK-framework. Hence, the momentum problem is an opacity problem (Gayley et al. ,1995). Results for OB-stars point to a moderate density clumping (Fvol=0.13). In addition, main sequence OB-stars require velocity clumping (Fvel=0.1, Sundqvist et al 2014). This can explain the weak wind problem.
DOI:10.48550/arxiv.1906.05581