Evolution of Massive Stars from Helium Burning to the Start of Neutronization

1974 ◽  
pp. 150-150
Author(s):  
W. David Arnett
Keyword(s):  
1994 ◽  
Vol 162 ◽  
pp. 67-68
Author(s):  
Frank M. Alberts

In the calculation of stellar models with the Cox–Stewart opacities no convective zones in the outer layers of massive stars appear. The new OPAL opacities (Rogers & Iglesias, 1992) show a significant bump in the opacity near temperatures of log T = 5.2. This opacity effect results in a small convective zone in the envelope of stars with mass ranging from 15 M⊙ to 150 M⊙, apart from possible convective zones caused by ionization. This was also briefly mentioned by Glatzel & Kiriakidis (1993). For stars on the main sequence this zone is small, about 1% of its radius on the zero age main sequence up to 7% at the onset of the core helium burning and contains a negligible amount of mass. For helium burning stars, however, this convective zone moves inward, keeping the same size but containing more and more mass.


1981 ◽  
Vol 59 ◽  
pp. 283-287
Author(s):  
A. Maeder

We have calculated evolutionary models of massive stars in the range 15-120 Mʘ from the zero-age sequence up to the end of the carbon burning stage (Maeder, 1981). Three sets of models with different mass loss rates Ṁ have been computed; the adopted parametrisation of Ṁ is fitted on the observations and thus the expression for Ṁ differs according to the location of the stars in the HRD.In this short note we concentrate on the location of the He-burning stars in the HRD. The helium burning phase, which lasts 8 to 10% of the MS phase, is spent mainly as red supergiants (RSG) and as WR stars (note that for low mass loss, the time spent as A-G supergiants becomes longer).


1973 ◽  
Vol 182 ◽  
pp. 209 ◽  
Author(s):  
Richard Stothers ◽  
Chao Wen Chin

1974 ◽  
Vol 190 ◽  
pp. 95 ◽  
Author(s):  
Richard G. Couch ◽  
Ann B. Schmiedekamp ◽  
W. David Arnett
Keyword(s):  

1982 ◽  
Vol 99 ◽  
pp. 377-381
Author(s):  
A. Tutukov ◽  
L. Yungelson

The larger part of close binary components with initial mass exceeding ∼20 Mo becomes WR stars in the core helium burning stage. Some of the most massive WR stars may be products of evolution of single massive stars with initial masses exceeding ∼50 M0 if the mass loss in the infrared supergiant stage is effective enough. The Ledoux criterion of convective stability seems more promising to explain the observed properties of WR stars.


1981 ◽  
Author(s):  
J. B. Blake ◽  
S. E. Woosley ◽  
T. A. Weaver ◽  
D. N. Schramm

1965 ◽  
Vol 36 (4) ◽  
pp. 1267-1282
Author(s):  
P. Giannone ◽  
M. A. Giannuzzi
Keyword(s):  

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