2013A&A...560A...6G


Query : 2013A&A...560A...6G

2013A&A...560A...6G - Astronomy and Astrophysics, volume 560A, 6-6 (2013/12-1)

Stellar mass-loss near the Eddington limit. Tracing the sub-photospheric layers of classical Wolf-Rayet stars.

GRAEFENER G. and VINK J.S.

Abstract (from CDS):

Towards the end of their evolution, hot massive stars develop strong stellar winds and appear as emission line stars, such as Wolf-Rayet (WR) stars or luminous blue variables (LBVs). The quantitative description of the mass loss in these important pre-supernova phases is hampered by unknowns, such as clumping and porosity due to an inhomogeneous wind structure and by an incomplete theoretical understanding of optically thick stellar winds. Even the stellar radii in these phases are badly understood since they are often variable (LBVs) or deviate from theoretical expectations (WR stars). In this work we investigate the conditions in deep atmospheric layers of WR stars to find out whether they comply with the theory of optically thick winds and whether we find indications of clumping in these layers. We used a new semi-empirical method to determine sonic-point optical depths, densities, and temperatures for a large sample of WR stars of the carbon (WC) and oxygen (WO) sequence. Based on an artificial model sequence we investigated the reliability of our method and its sensitivity to uncertainties in stellar parameters. We find that the WR stars in our sample obey an approximate relation with Prad/Pgas≃80 at the sonic point. This ``wind condition'' is ubiquitous for radiatively driven, optically thick winds, and it sets constraints on possible wind/envelope solutions affecting radii, mass-loss rates, and clumping properties. Our results suggest that the presence of an optically thick wind may force many stars near the Eddington limit to develop clumped, radially extended sub-surface zones. The clumping in these zones is most likely sustained by the non-linear strange-mode instability and may be the origin of the observed wind clumping. The properties of typical late-type WC stars comply with this model. Solutions without sub-surface clumping and inflation are also possible but require compact stars with comparatively low mass-loss rates. These objects may resemble the small group of WO stars with their exceptionally hot stellar temperatures and highly ionized winds.

Abstract Copyright:

Journal keyword(s): stars: Wolf-Rayet - stars: early-type - stars: atmospheres - stars: mass-loss - stars: variables: S Doradus - stars: interiors

Simbad objects: 51

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Number of rows : 51
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 HD 16523 WR* 02 41 11.6753354688 +56 43 49.735070148 10.03 10.34 9.99     WC6 136 0
2 HD 17638 WR* 02 52 11.6613087600 +56 56 07.131052500 10.99 10.86 10.41     WC6 119 0
3 HD 32257 WR* 04 56 02.8931275728 -69 27 21.546891216 13.441 13.962 14.23 14.31 14.514 WC 54 0
4 HD 32125 WR* 04 56 11.0961328800 -66 17 33.052465428 13.704 14.295 14.33   14.618 WC 56 0
5 HD 32402 WR* 04 57 24.0820685472 -68 23 57.120838692   12.53 12.69 13.24   WC 78 0
6 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17432 0
7 HD 37026 WR* 05 30 12.1637529576 -67 26 08.329055928 12.853 13.16 13.53 13.56 13.856 WC 76 0
8 HD 37680 WR* 05 34 19.2493989720 -69 45 10.295445528 12.807 12.98 13.25 13.21 13.490 WC 74 1
9 HD 269888 WR* 05 37 44.6348625936 -69 14 25.673976456 14.413 14.772 14.628 14.81 14.761 WR 46 0
10 * gam02 Vel WR* 08 09 31.95013 -47 20 11.7108 0.64 1.58 1.83 1.85 2.00 WC8+O7.5III-V 906 0
11 Ve 6-15 WR* 08 49 52.9566367968 -45 10 24.005049276   13.83 12.93 12.72   WC6 40 0
12 HD 76536 WR* 08 54 59.1670918944 -47 35 32.662167792 9.04 9.13 8.80 9.52   WC 124 0
13 HD 79573 WR* 09 13 11.7689184720 -50 06 25.523968608 12.30 11.80 10.69 10.52   WC6 82 0
14 HD 88500 WR* 10 10 31.9110817968 -60 38 42.419780376   10.84 10.65 10.67   WC5 86 0
15 HD 92809 WR* 10 41 38.3243333544 -58 46 18.723223308 8.95 9.28 9.03 9.60   WC6 156 0
16 LSWR 4 WR* 10 44 38.0518597224 -58 48 28.806098832   14.95 13.70 13.39   WC6+OB 39 0
17 HD 95435 WR* 11 00 00.7205444088 -57 48 59.277614904   11.78 11.61 11.67   WC6 58 0
18 [MS70] 8 WR* 11 05 46.42920 -61 13 48.7524     14.66 14.713   WC4 41 0
19 [W65] c18 WR* 11 38 05.0961216840 -62 16 01.900054200   14.985 13.921 13.599   WC6 40 1
20 Sand 2 * 12 02 49.7231459664 +28 51 23.162730336   17.25 15.80     M3: 10 0
21 HD 115473 WR* 13 18 27.9941240160 -58 08 13.603221168 9.09 9.68 9.00 9.72   WC5 115 0
22 HD 117297 WR* 13 30 53.2514208432 -62 04 51.858208308 10.81 11.10 10.90 10.70   WC8 97 0
23 WR 56 WR* 13 33 45.3814542096 -64 07 31.276015824   12.75 14.00 13.60   WC6 39 0
24 HD 119078 WR* 13 43 16.3587374232 -67 24 04.973391360 9.11 9.737 9.40 10.08   WC7/8 108 0
25 WRAY 16-136 WR* 13 49 32.5623529944 -61 31 42.272175756 12.09 11.99 11.69 12.72   WC9d 49 1
26 HD 121194 WR* 13 55 48.4481808288 -61 09 48.459624804 14.34 13.65 12.20 12.12 10.31 WC8 41 0
27 WR 64 WR* 14 56 55.1950350600 -55 50 58.552425204   15.11 15.08     WC6.5 23 0
28 WRAY 15-1297 WR* 15 13 41.7103828152 -59 11 44.976787404 16.25 15.58 13.65 13.11   WC9d+OB? 61 0
29 WRAY 16-172 WR* 15 18 20.7584521536 -59 38 17.324150928 14.83 14.52 13.28 12.99   WC7 50 2
30 HD 136488 WR* 15 24 11.3113204344 -62 40 37.578432792 9.15 9.514 9.10 9.71   WC9d+OB? 120 0
31 WRAY 15-1581 WR* 16 59 02.1892610760 -45 43 10.014514788   16.34 14.49 14.31 11.95 WC9 38 0
32 MR 66 WR* 17 02 40.3826152512 -45 59 15.453237084   13.62 12.07 11.77   WC9 64 0
33 CPD-33 4347 WR* 17 18 49.7249262168 -33 57 41.388161760   13.93 12.56 12.21   WN8/WC9 66 0
34 HD 156385 WR* 17 19 29.9012420376 -45 38 23.874269568 6.55 6.97 6.92 8.11   WC7 164 0
35 HD 157451 WR* 17 25 23.2779945960 -43 29 31.469964540 10 10.59 10.20 10.46   WC9 92 0
36 MR 74 WR* 17 36 19.8953017656 -33 26 12.271864344 16.01 14.87 13.18 12.99   WC9 90 1
37 V* V3893 Sgr WR* 17 45 47.5405102320 -26 10 26.779355616   15.13 14.20 14.23   WR 120 1
38 NAME Arches Cluster Cl* 17 45 50.5 -28 49 28           ~ 737 0
39 HD 164270 WR* 18 01 43.1453595672 -32 42 55.161329040 8.52 8.97 8.74 9.51   WC9d+? 225 0
40 HD 313643 WR* 18 04 43.6647313968 -21 09 30.555411624 13.58 13.27 12.02 11.67   WC9d 93 0
41 HD 165763 WR* 18 08 28.4692108104 -21 15 11.183076540 7.16 7.54 7.82 8.55   WC6 281 0
42 HD 169010 WR* 18 23 16.3427231112 -13 43 26.102574732 13.53 12.99 12.02 11.95   WC 80 0
43 MR 88 WR* 18 31 02.5170578472 -06 35 49.627098096   15.34 14.19     WC9 40 0
44 THA 20-1 WR* 18 39 17.9035317744 -10 05 30.898013928   13.07 12.43     WC9d 58 0
45 EM* AS 320 WR* 18 44 13.1526105048 -03 47 57.775268904 13.7 13.340 13.983     WC9d 119 0
46 HD 190002 WR* 20 01 39.7320392256 +32 34 17.996341908 13.83 13.42 12.67     WC7 67 0
47 HD 192103 WR* 20 11 53.5274337792 +36 11 50.525765304 7.77 8.13 8.11     WC8+OB: 332 0
48 WR 142 WR* 20 21 44.3438785440 +37 22 30.544989960   14.39 12.99 12.73 11.04 WO2 129 0
49 MR 110 WR* 20 32 03.0201049320 +41 15 20.499732216   15.99 13.97     WC5 82 0
50 WR 150 WR* 21 50 05.5725399960 +50 42 24.715501200   14.00 13.47     WC5 32 0
51 HD 213049 WR* 22 27 17.8187635824 +56 15 11.770681752   11.270 10.928 10.922   WC6 91 0

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