Table 1
Model parameters for Wd1-5.
log (L∗) | R ∗ | T eff | Ṁ | v ∞ | β | f cl | log g | M ∗ | H/He | N/N⊙ | C/C⊙ | O/O⊙ |
(L⊙) | (R⊙) | (kK) | (10-6M⊙ yr-1) | (kms-1) | (M⊙) | |||||||
|
||||||||||||
5.38![]() |
34.0![]() |
21.9![]() |
2.16![]() |
430![]() |
2.50![]() |
0.25![]() |
2.33![]() |
9.0![]() |
4.0![]() |
9![]() |
1.40![]() |
0.3![]() |
Notes. We adopt a distance of ~ 5 kpc (Negueruela et al. 2010) and with AV ~ 10.66 (Sect. 3) determine that MV = −6.63 (implying a bolometric correction of −2.1 mag). We note that R∗ corresponds to R(τRoss = 2/3). The H/He ratio is given by number and other abundances are relative to solar values from Anders & Grevesse (1989); if we use the values from Asplund et al. (2006) as a reference, the derived ratios need to be scaled by 1.38, 1.537 and 1.86 for C, N and O respectively. Finally, our derived H/He abundance corresponds to a surface helium mass fraction, Ys = 0.49.
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