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Table 2

Stellar parameters for WN stars with a line effect.

WR WR sub-type T X H log L R M Γe log () v
[kK] [L] [R] [M] [M/ yr] [km s-1]

SMC
HD 5980 WN5 45 0.25 6.35 24 88.4 0.48 –4.5 2200
54.5 0.79

LMC
BAT99-22 WN9h 32 0.4 5.75 25.1 43.4 0.28 –4.85 400
21.5 0.56
BAT99-33 Ofpe/WN9 28 0.2 6.50 74.8 114.3 0.51 –4.43 400
72.2 0.81
BAT99-43 WN4o+OB 67 0.0 5.85 6.3 27.0 0.40 –5.15 1600
24.8 0.44

Milky Way
6 WN4 89.1 0.0 5.6 2.65 17.9 0.342 –4.5 1700
16 WN8 44.7 0.25 6.15 19.9 40.1 0.678 –4.5 650
41.7 0.23 5.68 12.3 20.0 0.453 –4.8
40 WN8 44.7 0.23 6.05 17.7 34.3 0.618 –4.3 650
45.0 0.15 5.61 10.6 18.2 0.397 –4.5
134 WN6 63.1 0.0 5.6 5.29 17.9 0.342 –4.6 1700
1363 WN6 70.8 0.12 5.4 3.34 13.7 0.316 –4.7 1600

Notes. Parameters for the LMC WN stars are from Hainich et al. (2014), whilst the parameters for HD 5980 are from Shenar et al. (2016). The Galactic WN parameters are from Hamann et al. (2006). Masses M and Eddington factors Γe are obtained from the mass-luminosity relations for both homogeneously H-burning and He-burning by Gräfener et al. (2011). The spectroscopically determined mass-loss rates are scaled to a wind clumping factor D = 10. See the discussion in Vink et al. (2011) on the inclusion of WR 136 as a line-effect object.

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