Title: Unkown stellar mass loss at low metallicity
1Unkown stellar mass loss at low metallicity
- Henny Lamers
- Astronomical Institute and
- SRON Laboratory for Space Research
- Utrecht University
2Topics to be discussed
- Predictions of properties of normal winds
(Zsolar) - and comparison with observations
- Predicted properties of low Z winds (Z10-4
solar) - Extremely no Z winds (H and He only)
3 Net force in wind gnet - gN ge glines
gt 0
Gravity gN GM / R2
Rad pressure by electrons ge se L / 4 p R2
c Ge gN
Rad pressure by lines gl ge M(t)
Force multiplier M(t) k t-a (ne/W)d
Solar Z k 1/30 a 0.6
d 0.1
Castor, Abbott Klein 1975, CAK
4Predictions scaling laws
Castor, Abbott, Klein 1975
- v8 (2 to 3) v esc v (M/R)
- Mdot L 1/a M (a-1)/a
5Predictions scaling laws
Castor, Abbott, Klein 1975
- v8 (2 to 3) v esc v (M/R)
- Mdot L 1/a M (a-1)/a
?
Kudritzki et al 1989
? Mdot v8 v R L 1/a M 0.5-(1-a)/a
L 1/a ? Modified wind momentum
6Predicted mass loss rates
Vink et al. 2000
7Modified wind momentum ? ? L
predictions
Log ?
observations
Vink et al. 2000
8New study with improved mass loss rates
Galactic stars
Markova et al. 2004
9Problem
- Some stars with very similar stellar
parameters show a large difference in mass loss
rate and wind properties !! -
-
10Tale of two stars
AV 83 AV 69 Type
O7 Iaf O7.5 III L/Lsun 3.5 105
4.1 105 Teff 32800 33900 R/Rsun
18.5 18.6 He/H 0.2
0.1 C/N 0.15 15
Hillier et al. 2003
11AV 83 and AV 69 very different winds!
Hillier et al. 2003
12 AV 83 AV 69 Mdot 7 10-7 9
10-7 V8 940 1800 ß 2.0
1.0 fclump 0.1 1
ROTATION !!!
Hillier et al. 2003
13- Effects of rotation
- Flattening
-
- 2. Gravity f( ?)
- 3. Teff f(? )
- 4. Mdot f(?)
- 5. Vwind f(?)
- 6. Spect type f(sin i)
Meynet Maeder 2002
14The wind of a fast rotating hot supergiant
J. Bjorkman 2005
15Mass loss and metallicity
16Predictions for line driven winds
10-2 lt Z/Zsun lt101
Mdot Z 0.85
Vink et al. 2001
17Observations ? Predictions
LMC SMC
Vink et al. 2001
18The problem of the winds of low luminosity SMC
stars
Black Gal Red LMC Blue SMC
??L relation breaks down at log L lt 5.3 !!
Martins et al. 2004
19Mass loss at very low metallicityZ/Zsun lt 10-3
20Predictions at low Zparameters k, a, d vary
with distance
Z/Zsun 1.0 0.2 10-2 10-3 10-4
?
Kudritzki 2002
21Very low Z stars only have winds when they are
close to Eddington limit !
- grad ge glines gt gN at some depth
- glines M(t) ge
- Mmax 2000 Z/Zsun M(H,He) from atomic
physics - So maximum radiation pressure is
- gradmax (1Mmax) ge (1Mmax) Ge gN gt gN
- Ge gt (1Mmax)-1
22Dependence of mass loss on Ge
? Mdot 10-8
Msun/yr
Kudritzki 2002
23Zero metallicity stars
1. Radiation pressure only due to H and He
lines 2. H lines alone are never strong enough 3.
HeII lines can produce grad-gN gt0 if level
populations are just right but only in very
small region of atmosphere.
Krticka Kubat, 2005
24 geff gt 0 only in very
small zone
Zero metallicity stars have NO line driven winds
!!
Krticka Kubat 2005
25Conclusions
- A 10-3 lt Z/Zsun lt 10 Mdot Z0.85
- but
Mdot depends on (fast) rotation - B 10-4 lt Z/Zsun lt 10-3 Mdot only for
large Ge - Ge gt
(1Mmax)-1 - Mmax
2000 Z/Zsun - C Z/Zsun0 no line driven
wind, - Mdot lt
10 -10 Msun/yr -
26Thats all !
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