1999A&A...351..554H


Query : 1999A&A...351..554H

1999A&A...351..554H - Astronomy and Astrophysics, volume 351554-558 (1999/11-2)

Fractionated stellar wind and the H/He abundance anomalies in Bp stars.

HUNGER K. and GROOTE D.

Abstract (from CDS):

Radiatively driven winds occur in all main sequence stars (Babel, 1995A&A...301..823B, 1996A&A...309..867B). However, due to the weak coupling between the photon absorbing metals and the inert elements H and He, the wind in the low temperature domain is fractionated: He decouples from the wind at Teff<25000K, and below 17000K even H. The decoupled elements fall back to the surface of the star thus creating overabundances and abundance stratifications. These anomalies, however, become manifest only if atmospheric turbulence is suppressed (say by magnetic fields). In order to prove the validity of the described scenario, all Bp stars for which reliable fundamental parameters exist, are discussed on the basis of the (augmented) (g, Teff)-diagram of Babel (1996A&A...309..867B). It is shown that the fractionation process is able to explain the observed temperature sequence of He-rich and He-poor stars, additionally to classical diffusion processes. A necessary condition is that a magnetic field is present. This explains why only a fraction of B stars exhibits H/He anomalies. While classical diffusion operates in the quiet zones (no wind) of a star, fractionation takes place above the wind bases.

Abstract Copyright: ∼

Journal keyword(s): stars: abundances - stars: chemically peculiar - stars: mass-loss

Simbad objects: 31

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Number of rows : 31
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 * 29 Psc V* 00 01 49.4481127032 -03 01 39.011820024 4.47 4.98 5.10     B7III-IV 232 0
2 * alf Scl Ro* 00 58 36.3592644040 -29 21 26.832190995 3.52 4.09 4.27 4.30 4.43 B7IIIp 259 0
3 * eps Eri BY* 03 32 55.8444911587 -09 27 29.739493865 5.19 4.61 3.73 3.00 2.54 K2V 2073 1
4 * 20 Eri a2* 03 36 17.4041095200 -17 28 01.472307996 4.61 5.10 5.23     B8/9III 181 0
5 * 22 Eri a2* 03 40 38.3331139440 -05 12 38.555731188 4.81 5.38 5.53     B9IIIpSi4200 134 0
6 * ups04 Eri SB* 04 17 53.6624004496 -33 47 54.052408258 3.07 3.44 3.56 3.57 3.68 B8V+B9.5V? 168 0
7 HD 28843 Ro* 04 32 37.5537339576 -03 12 34.344832032 5.13 5.67 5.81     B9III 140 0
8 HD 37017 SB* 05 35 21.8667428568 -04 29 39.024375324 5.66 6.43 6.56 6.61 6.74 B2/3V 318 0
9 * sig Ori E Y*O 05 38 47.2050040320 -02 35 40.521424812 5.66 6.38 6.46 6.84 7.08 B2IV-Vp_He 486 0
10 V* V901 Ori Ro* 05 40 56.3704617744 -01 30 25.856677224 5.96 6.82 6.96     B2V 354 2
11 * 12 CMa a2* 06 47 01.4835271104 -21 00 55.451696472 5.27 5.89 6.08     B7II/III 152 0
12 HD 58260 * 07 23 19.5997521648 -36 20 24.538554852 5.87 6.61 6.73     B2/3Vp 108 0
13 * alf CMi SB* 07 39 18.11950 +05 13 29.9552 0.82 0.79 0.37 -0.05 -0.28 F5IV-V+DQZ 1925 0
14 HD 62712 * 07 43 42.9160399680 -38 12 06.767386272 5.76 6.24 6.40     B8IV 87 0
15 HD 64740 * 07 53 03.6344819483 -49 36 46.956285817 3.48 4.40 4.63 4.76 4.97 B2V 223 0
16 HD 74196 * 08 40 17.4649643448 -53 00 55.430609904 4.97 5.47 5.61     B9/A0 144 0
17 * L Car * 10 22 58.1465809448 -66 54 05.385596996 4.35 4.86 4.99     B8V 120 0
18 HD 96446 bC? 11 06 05.8219128840 -59 56 59.564064444 5.81 6.57 6.69     B2IIIp 177 0
19 * gam Mus SB* 12 32 28.0129260853 -72 07 58.763241944 3.12 3.73 3.88 3.91 4.08 B5V+A: 155 0
20 V* CU Vir a2* 14 12 15.8055434051 +02 24 33.945178515 4.46 4.90 5.02 5.10 5.23 ApSi 411 0
21 * a Cen Ro* 14 23 02.2387240143 -39 30 42.544559700 3.50 4.24 4.42 4.53 4.70 B2V 289 0
22 * alf Cen ** 14 39 36.50 -60 50 02.3   0.4 -0.1     G2V+K1V 1031 0
23 HD 133518 ** 15 06 55.9713564672 -52 01 47.204898312 5.57 6.29 6.39     B2IVpHe 102 0
24 V* NN Aps a2* 15 31 27.1154643312 -71 03 43.664769144   6.76 6.87     Ap(SiCrFe) 98 0
25 * 3 Sco Ro* 15 54 39.5296532472 -25 14 37.459966128 5.23 5.81 5.87     B8III/IV 232 0
26 V* V913 Sco Ro* 15 58 34.8665694960 -24 49 53.361727284 4.70 5.34 5.43     B5V 226 0
27 HD 143699 * 16 03 24.1895252119 -38 36 09.141541952 4.18 4.75 4.89 4.96 5.10 B5/7III/IV 154 0
28 HD 144334 ** 16 06 06.3891324384 -23 36 22.849641396 5.29 5.84 5.92     B8V 203 0
29 HD 144941 pA* 16 09 24.5513020968 -27 13 38.184011148 9.45 10.17 10.02     B8 96 1
30 HD 146001 * 16 14 53.4294665736 -25 28 37.100440632 5.73 6.09 6.05     B8V 161 0
31 V* V957 Sco BS* 17 52 13.6613130072 -34 47 57.109291728 5.16 5.80 5.90     B5IVp 146 0

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