1995A&A...300..237N


Query : 1995A&A...300..237N

1995A&A...300..237N - Astronomy and Astrophysics, volume 300, 237-258 (1995/8-1)

Chemical composition of Wolf-Rayet stars. II. Hydrogen-to-helium ratio.

NUGIS T. and NIEDZIELSKI A.

Abstract (from CDS):

The formation of HeII, HeI and HI lines in the winds of some representative WN stars of different spectral subtypes has been modeled. Two different types of models were studied: the clumped winds and smooth winds for both of which the standard velocity law v=v0+(v-v0) (1-R*/r)β with β=1 was assumed. The smooth winds model predicts about two times lower IR fluxes than observed if one determines the matter density in the winds through the observed values of radio fluxes. The increased density smooth wind models with 1.5 times higher density as compared to the radio-flux scaling are in reasonable agreement with IR fluxes and HeII and HeI line fluxes in the case of WN 5, WN 6 and WN 8 stars but for other subtypes these models predict discrepant line fluxes. The clumped wind models agree quite well with the most important observational data whereas somewhat lower mass loss rates are now derived as compared to the smooth wind models. Theoretical line fluxes were found by summing of the contributions from different layers of the wind. The statistical equilibria equations for level populations were solved in the Sobolev approximation by taking into account the overlap of HeII and HI lines in the expanding medium. We used 40, 20 and 52 level atomic models for HeII, HI and HeI respectively, whereas the influence of higher levels was taken into account through the correction terms. On the basis of our modelling study we derived a simple formula for the determination of hydrogen-to-helium ratios for WN stars which was used for concrete estimates for 28 stars. In all cases the hydrogen-to-helium ratios are lower than the mean cosmic value. By inspection of the line fluxes of the neighboring HeII lines of (n-4), (n-6) and (n-8) series in the spectra of two WC stars we concluded that no hydrogen seems to be present in their winds. The hydrogen-to-helium ratio is decreasing when going from late to early WN subtypes with strong scatter existing among the stars of WN 6 and later subtypes.

Abstract Copyright:

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

Simbad objects: 30

goto View the references in ADS

Number of rows : 30
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 4004 WR* 00 43 28.3971737448 +64 45 35.384652468 10.28 10.718 10.138     WN4-s 197 0
2 HD 9974 WR* 01 38 55.6274097096 +58 09 22.673806272 9.85 10.71 10.69     WN3h-w 170 0
3 HD 50896 WR* 06 54 13.0439608392 -23 55 42.023319852 5.74 6.63 6.91 7.74   WN4b 773 0
4 HD 62910 WR* 07 44 58.2217347768 -31 54 29.554957188 10.08 10.44 10.10 10.17   WN6/WC4 128 0
5 CD-45 4482 WR* 08 44 47.2901340000 -45 58 55.417387548 10.95 11.29 10.74 10.58   WN8h+? 103 0
6 HD 86161 WR* 09 54 52.9033957968 -57 43 38.274644604 7.94 8.65 8.36 8.93   WN8h 219 0
7 HD 92740 WR* 10 41 17.5158425712 -59 40 36.895992960 5.68 6.50 6.42 7.38   WN7h+O9III-V 412 0
8 HD 96548 WR* 11 06 17.2032351624 -65 30 35.241182028 7.10 7.80 7.70 8.49   WN8h 412 0
9 HD 117688 WR* 13 33 30.1197052368 -62 19 01.214335740 8.69 10.81 10.90 10.44   WN7 130 0
10 HD 143414 WR* 16 03 49.3455286488 -62 41 35.941627680 9.32 10.03 10.10     WN6-w 112 0
11 HD 151932 WR* 16 52 19.2477039480 -41 51 16.270066224 6.06 6.79 6.51 7.64   WN7h 313 0
12 LS 3982 WR* 17 14 27.1191622584 -39 45 47.051105904 10.63 10.95 10.41     WN6h-w 68 0
13 HD 313846 WR* 18 05 25.7344895280 -23 00 20.334949992 10.48 10.69 9.89 9.89   WN9h+OB 135 0
14 HD 165763 WR* 18 08 28.4692108104 -21 15 11.183076540 7.16 7.54 7.82 8.55   WC6 281 0
15 MR 87 WR* 18 25 30.0135261024 -14 38 40.967308176 13.38 13.09 11.86 11.33   WN6-w 81 0
16 MR 89 WR* 18 41 00.8670061488 -04 26 14.484137676 13.1 12.97 11.93 11.67   WN7 72 2
17 HD 177230 WR* 19 03 59.0233422072 -04 19 01.910240688 11.32 11.60 11.12     WN8 171 0
18 Hen 2-427 WR* 19 11 30.8749167768 +16 51 38.200938264   12.19 11.50     WN8h 340 0
19 HD 187282 WR* 19 48 32.1967360032 +18 12 03.695582124 9.60 10.49 10.51     WN4(h)-w 198 0
20 HD 191765 WR* 20 10 14.1928045152 +36 10 35.070683376 7.64 8.08 8.08     WN6-s 441 0
21 HD 192103 WR* 20 11 53.5274337792 +36 11 50.525765304 7.77 8.13 8.11     WC8+OB: 332 0
22 HD 192163 WR* 20 12 06.5418877464 +38 21 17.784181008 7.12 7.49 7.50     WN6(h)-s 544 0
23 HD 193077 WR* 20 17 00.0260987184 +37 25 23.785483116 7.82 8.32 8.01 8.71   WN5-w+B? 290 0
24 HD 193928 WR* 20 21 31.7290073688 +36 55 12.773070696 10.67 10.60 9.78     WN5-w+O5V-III 199 0
25 HD 197406 WR* 20 41 21.5485520640 +52 35 15.142636896 10.42 10.87 10.30     WN8h+B3IV/BH 197 0
26 HD 211564 WR* 22 16 24.0318845736 +55 37 36.767570232   11.72 11.61     WN3(h)-w 122 0
27 HD 211853 WR* 22 18 45.6057566664 +56 07 33.898679364 8.84 9.534 9.236 9.108   WN6o+O6I 275 0
28 HD 214419 WR* 22 36 53.9548302648 +56 54 20.989190232 8.68 9.376 8.996 8.962   WN6o+O9Ib/II 377 1
29 MR 119 WR* 23 00 10.1253892224 +60 55 38.410870260 11.85 11.949 10.844 10.520   WN8h 101 0
30 EM* AS 513 WR* 23 43 30.5960809392 +61 55 48.139591872 12.02 11.98 11.282     WN7h+Be? 73 0

To bookmark this query, right click on this link: simbad:objects in 1995A&A...300..237N and select 'bookmark this link' or equivalent in the popup menu