1994A&A...290..819L


Query : 1994A&A...290..819L

1994A&A...290..819L - Astronomy and Astrophysics, volume 290819-833 (1994/10-3)

Towards an understanding of very massive stars. A new evolutionary scenario relating O stars, LBVs and Wolf-Rayet stars.

LANGER N., HAMANN W.-R., LENNON M., NAJARRO F., PAULDRACH A.W.A. and PULS J.

Abstract (from CDS):

Based on recent progress in the theory of stellar structure and evolution, in the theory of stellar atmospheres and winds, and in the observational data base, we propose a new scenario for the evolution of very massive stars (MZAMS>40M☉) in our Galaxy. A sample evolutionary calculation for a 60M☉ star, incorporating recent theoretical results about violent pulsational instabilities in very massive stars, is critically compared with a multitude of observational facts. The relation between those pulsational instabilities and observed line profile variability in O stars is discussed. New wind models for PCygni are computed, with particular emphasis on the determination of its mass and surface He/H-ratio. A detailed comparison of our sequence with the Galactic WR population is performed, considering newly determined surface abundances. Our results suggest a new interpretation of luminous hydrogen-rich late-type WN stars as core hydrogen burning objects, while hot WN stars with small or zero hydrogen abundance are core helium burning stars. PCygni is identified with the hydrogen shell burning phase of our sequence. The observed upper luminosity limit for Galactic hydrogen-free WN stars appears to be consistent with our picture. Hence we propose the following evolutionary sequence for very massive stars: O -> Of -> H-rich WN -> LBV -> H-poor WN -> H-free WN -> WC -> SN.

Abstract Copyright: ∼

Journal keyword(s): stars: abundances - stars: evolution - stars: mass-loss - stars: Wolf-Rayet - stars: supergiants

Simbad objects: 13

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Number of rows : 13
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * zet Pup BY* 08 03 35.04754 -40 00 11.3321 0.89 1.98 2.25 2.36 2.58 O4I(n)fp 1190 1
2 HD 92740 WR* 10 41 17.5158425712 -59 40 36.895992960 5.68 6.50 6.42 7.38   WN7h+O9III-V 426 0
3 HD 93162 WR* 10 44 10.3890266112 -59 43 11.106500520 7.90 8.55 8.80 8.66   O2.5If*/WN6+OB 374 0
4 WRAY 15-682 WR* 10 53 59.5777329720 -60 26 44.361095316   11.64 10.85 10.56   WN11h 155 3
5 V* AG Car WR* 10 56 11.5781414448 -60 27 12.810673260 7.00 7.57 6.96 7.73   WN11h 649 0
6 HD 134877 WR* 15 14 57.7186057272 -59 50 30.215432688 12.13 12.19 11.34 11.08   WN8(h) 112 0
7 HD 313846 WR* 18 05 25.7344895280 -23 00 20.334949992 10.48 10.69 9.89 9.89   WN9h+OB 143 0
8 HD 193077 WR* 20 17 00.0260987184 +37 25 23.785483116 7.82 8.32 8.01 8.71   WN5o+B? 297 0
9 * P Cyg s*b 20 17 47.2019733389 +38 01 58.549132671 4.66 5.24 4.82 4.28 4.02 B1-2Ia-0ep 1200 1
10 HD 193576 WR* 20 19 32.4229160448 +38 43 53.959035756 8.15 8.53 8.00     WN5+O6II-V 721 0
11 EM* AS 431 WR* 20 36 43.6322747712 +40 21 07.442607924     13.73 12.51   WN8(h)+B0.5V 228 0
12 MR 119 WR* 23 00 10.1253892224 +60 55 38.410870260 11.85 11.949 10.844 10.520   WN8h 106 0
13 EM* AS 513 WR* 23 43 30.5960809392 +61 55 48.139591872 12.02 11.98 11.282     WN7h+Be? 76 0

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