Stellar Winds and Hydrodynamic Atmospheres of Stars · 2010. 3. 11. · Stellar winds observable...
Transcript of Stellar Winds and Hydrodynamic Atmospheres of Stars · 2010. 3. 11. · Stellar winds observable...
Stellar Windsand
Hydrodynamic Atmospheresof
Stars
Rolf KudritzkiSpring Semester 2010
I. IntroductionFirst suspicion of existence of continuous stellar winds:
1929 C. BealsMNRAS 90, 202
91, 966 (1931)1934 S. Chandrasekhar
MNRAS 94, 522 Optical spectrum of P CygniB2 hypergiant
and LBV :
broad H, HeI, metal lines withblue-shifted absorptionred-shifted emission
Optical spectrum of Wolf-Rayet
stars
:
broad He, C, N emission linesno hydrogen lines
widths of lines Doppler-shifts of out-flowing atmospheresVexpansion
≈
200 km/s to 3000 km/s
H and HeI
lines of P Cygni
Note different y-scale of plots
Emission in Hα
is hugeHδ
is much weaker
Najarro, Kudritzki
et al. 1997
Same Fig. as before,but now
replaced by
estimate ofoutflow
velocities
P Cygni - B2 hypergiant and LBV: Model atmosphere fit - optical lines
Najarro, Kudritzki et al. 1997
I. IntroductionFirst suspicion of existence of continuous stellar winds:
1929 C. BealsMNRAS 90, 202
91, 966 (1931)1934 S. Chandrasekhar
MNRAS 94, 522 Optical spectrum of P CygniB2 hypergiant
and LBV :
broad H, HeI, metal lines withblue-shifted absorptionred-shifted emission
Optical spectrum of Wolf-Rayet
stars
:
broad He, C, N emission linesno hydrogen lines
widths of lines Doppler-shifts of out-flowing atmospheresVexpansion
≈
200 km/s to 3000 km/s
Conc
epci
on 2
007 Wolf-Rayet
star in NGC 300 at 2 Mpc
distance
WN11 star
Bresolin, Kudritzki, Najarro
et al. 2002, ApJ
Letters 577, L107
emission line diagnostics:first detailed abundance pattern outside Local Group
1934 Adams and McCormack
ApJ
81, 119 optical spectra of M supergiantsα
Ori
M2 Ib
α1
Sco
M1 Ibα1
Her M5 IIblue-shifted absorption cores of groundstatelines of MnI, CaI, CrI
etc. (“0.00 eV
lines”)
modern spectra (high res. & S/N) narrow P Cygni
profile superimposed
to photospheric
line core(Bernat
& Lambert, 1976, ApJ
204, 830)
vexp
≈
10 to 20 km/s but vesc
= [2GM/R]1/2
escape velocity isof same order!
Is the flow able to escape the gravitational potential ????
α
Ori
tiny P Cygni
profile superimposed to photosperic
line core
Bernat
& Lambert, 1976 ApJ
204, 830
MnIλ
4030.8 Å
λ
4033.1 Å
1956 Armin J. Deutsch
ApJ
123, 210Mt. Palomar 5m Coude
spectra with very high resolution
of M supergiants
with earlier spectral-type companions
α1
Sco
M1 Ibα2
Sco
B2 V CaII, TII etc. lines very unsual
for B2
α1
Her M5 IIα1
Her G0 III MNI, CrI
etc. very unusual for G0
circumstellar
linesproduced wind of M supergiant
Model by Kudritzki
& Reimers, 1978, A&A 70, 227
wind envelope extension ≈
1000 Rstarvexp
≈
20 km/s >> Vexp
>> Vesc
(r) M supergiants
have winds !!!
vesc
= [2GM/r]1/2
≈
1/30 vesc-photosphere
1951 Ludwig Biermann
Zeitschrift
fuer
Astrophysik
29, 274all comet plasma tails point away from sun
solar wind with v ≈
400 km/s
1962 Neugebauer
& Snyder Science,138, 1169Mariner 2 probe to Venus findsfast solar wind present all times
v ≈
500 ±
300 km/s at Earth orbitnwind
= 5 cm-3 highly variable= some 10-13
Msun
/yr
1958 Eugene Parker ApJ
128, 664first hydrodynamic theory of solar wind
Solar wind
II. Spectroscopic evidence for stellar winds
1. Spectral lines in hydrostatic atmospheres
Hydrostatic
barometric formula
thin, plane-parallel atmosphere with temperature gradient
symmetric absorptionline aroundcentralwavelengthλ0
Width of line determined by
a) thermal motion of gas
b) stellar rotation
c) Pressure broadening, stellar gravity
1. Line scattering in expanding atmospheres
in front of stellar disk: blue-shiftedscattering by gas moving towards observer
remaining envelope: red-
& blue-shiftedscattering by gas moving towards and away from observer
P Cygni
profile
width determined by vmax
Note: “line scattering”
is special re-emission process
photon is absorbed and re-emitted by spontaneous emission in same line transition
de factoscattering
number of photons is conserved
Nabs
= Nem
typical process for resonance lines
2. Thermal or recombination emissionin expanding atmospheres
If τspont
> τcoll
absorbed photon not re-emittedand destroyed by collisionallevel excitation or de-excitationre-emission coupled to local T(r)since wind envelope can a huge volume,an emission line might occur
width determined by vmax
pure emission profile
If ionization of the atoms with subsequent recombination dominates, then the population of the upper level is controlled from electron transitions cascading from above
ionization from groundor excited level
cascade of subsequent spontaneous emissions
pure emission line
3. Other signatures of stellar winds
Stellar winds are ubiquitous in all stellar domains !!!
Radio:
hot stars: free-free emission of winds“
radio-
excess”
cool stars: maser emission of windsOH, H2
O, SiO, NH3
IR: ground-based & satellite telescope (IRAS, ISO, Spitzer, Herschel)
hot stars: free-free emission of windsweaker than “
radio-
excess”
rich emission line spectra H, He, metalscool stars: dust emission in winds, PAHs
Najarro & Kudritzki, 1997
P Cygni - B2 hypergiant and LBV: Model atmosphere fit – IR (ISO)
P Cygni
mid IR (ISO)
Najarro, 2005
Optical:
line diagnostics of mass-loss rateswind velocitieschemical composition
A-supergiant in M31 –
stellar wind
McCarthy, Kudritzki,Venn, Lennon,Puls1997, ApJ
482, 757
Keck, Hires
Hα
emission B superrgiant
–
stellar wind
Kudritzki et al. 1999,A&A 350, 970
Model calculation
Hα
emission O-star Model calculation
Variation ofby ± 20% M
Kudritzki & Puls, 2000, AARA 38, 613
Conc
epci
on 2
007 Wolf-Rayet
star in NGC 300 at 2 Mpc
distance
WN11 star
Bresolin, Kudritzki, Najarro
et al. 2002, ApJ
Letters 577, L107
emission line diagnostics:first detailed abundance pattern outside Local Group
Conc
epci
on 2
007 NGC 300 WN11 star
non-LTE line-blanketed
hydrodynamic model atmospheres
with stellar winds
stellar parameters
wind parameters
H, He, CNO, Al, Si, Fe abundances
Bresolin, Kudritzki, Najarro
et al. 2002, ApJ
Letters 577, L107
Conc
epci
on 2
007 NGC 300 WN11 star
Conc
epci
on 2
007
Najarro, Urbaneja, Kudritzki, Bresolin
2005
LBVLBV
Teff
= 10000K, L = 3.1 105
Lsun
mass fraction X/Xsun
H 0.688 0.97He 0.301 1.06Mg 1.5 10-4
0.22Fe 1.5 10-3
1.08
NGC 36217 Mpc
UV:
satellite telescopes: Copernicus, IUE, HST, ORFEUS,EUVE, FUSE
very rich stellar wind spectra of hot and cool stars
OVI, OV, OIV, OIII, NV, NIV, NIII, CIV, CIII, CII, SiIV, SiIII, SVI, SV, MgII, FeII
…..
Conc
epci
on 2
007 UV spectrum of O4
supergiant z Puppis Pauldrach, Puls, Kudritzki et al. 1994, SSRev, 66, 105
Conc
epci
on 2
007
HD 93129A O3IaTaresch, Kudritzki et al. 1997, A&A, 321, 531
X-ray: hot stars: emit X-rays through shocks in their winds strong X-ray emitters
cool stars: have coronae, except M supergiants/giants
Conc
epci
on 2
007 time dependent stellar wind radiation-hydro
shocks
(Owocki
et al., 1988; Feldmeier, 1997)
Conc
epci
on 2
007
ζ
Pup, O4 If ι
Ori
O9 III 15 Mon O7 V
Calculated spectra and ROSAT observationsFeldmeier, Kudritzki et al., 1997
theory
convolved withROSAT FWHM
●
ROSAT
III. Stellar winds and Astronomy
1. Stellar winds and galaxies
Massive stars dominate light of star forming galaxies
Strong and broad stellar wind lineseasily detectable in spectraof integrated stellar populationsExample: starburst galaxies at high z
UV shifted to optical/IR
population synthesis, metallicities,Energy and momentum input galactic winds, star formation Nuclear burned material input
chemical evolution of galaxies
P Cygni profiles and metallicity
Galaxy LMC SMC
Kudritzki, 1998
cB58
@ z=2.7
non-LTE atmospheres with windsplus stellar evolution models
Synthetic spectra of galxies
at high z as a function of Z, IMF, SFR
Population synthesis of highPopulation synthesis of high--z galaxiesz galaxies
Galaxy spectra
Stellar spectra
Stellar Population
Initial Mass Function
Star Formation History MetallicityStellar Evolution
NGC 5253
Leitherer
et al. 2001, ApJ, 550, 724
Starburst99 population synthesis models
+
UV stellar libraries at ~solar and ~0.25 solar (LMC,
SMC) abundance
Rom
e 200
5Spectral diagnostics of high-z starbursts
Rix, Pettini, Leitherer, Bresolin, Kudritzki, Steidel, 2004, ApJ 615, 98
Starburst models - fully synthetic spectra based on model atmospheres
Rom
e 200
5Spectral diagnostics of high-z starbursts
Rix, Pettini, Leitherer,Bresolin, Kudritzki, Steidel2004, ApJ 615, 98
cB58 @ z=2.7
fully synthetic spectravs. observation
2. Winds and stellar evolution Winds affect stellar evolution significantly
winds mass-loss
mass M is decisive parameterfor stellar structure/evolution
crucial in certain phases, because it changes stellar mass
stars with significant during red giant
stage
good approximationReimers
–
formulaReimers, 1975; Kudritzki
& Reimers, 1978, A&A 70, 227
Note:
tremendous mass-loss in RGS and AGB –
phasestar with 8 Msun
on main sequence ends up with 1 Msun
7 Msun
re-cycled to ISMejection of Planetary Nebula at tip of AGB
Late stages of low-mass stellar evolution: CSPN
depends on L
small, but ≈
mass of hydrogenburning shell
tevol
strongly modifiedby winds
for review of CSPN winds seeKudritzki, Mendez et al., 1997, Proc. IAU Symp. 180, 64Kudritzki
et al., 2006, Proc. IAU Symp. 234, 119
White Dwarfs: extremely narrow mass distribution
without mass-loss stars with such masses cannot have evolved from the main sequence within Hubble time
from the HRDs
of open clusters we know the all stars with
have formed WDs
The mass spectrum observed can be explained by IMF and stellar evolution with mass-loss applying Reimers
-
formula
stars with Stellar winds observable during whole evolution
Kudritzki
& Puls, 2000, AARA 38, 683Kudritzki
& Urbaneja, 2009
strong forno evolution towardsred supergiants
stars can lose up to 90% of their mass until He-ZAMS
Wolf-Rayet
stars: massive stars on He-ZAMS with no Hvery strongwinds !!!
3. Winds and galaxy evolution stellar winds Energy and momentum input into ISM
affects star formationcauses “galactic winds”recycles nuclear burned matterinto ISMaffects chemical evolution