padova, october 1980. padova, october 1980 padova, october 1980

33
Padova, October 1980

Upload: randolf-morrison

Post on 06-Jan-2018

246 views

Category:

Documents


1 download

DESCRIPTION

MASS LOSS ROTATION-MIXING BINARY EVOLUTION MAGNETIC EFFECTS Effects of stellar physics on the chemical yields André Maeder Geneva Observatory In collaboration with Georges Meynet

TRANSCRIPT

Page 1: Padova, October 1980. Padova, October 1980 Padova, October 1980

Padova,October 1980

Page 2: Padova, October 1980. Padova, October 1980 Padova, October 1980

Padova,October 1980

Padova, October 1980

Page 3: Padova, October 1980. Padova, October 1980 Padova, October 1980

•MASS LOSS•ROTATION-MIXING

•BINARY EVOLUTION

•MAGNETIC EFFECTS

Effects of stellar physicson the chemical yields André Maeder Geneva Observatory

In collaborationwith Georges Meynet

Page 4: Padova, October 1980. Padova, October 1980 Padova, October 1980

What mass loss in pre- supernova stages of massive stars ?

The proximity to the Eddington limit is the physical reason for the onset of WR type mass lossGräfener et al. 2011

Case of WR stars

Maeder et al. 2011

Page 5: Padova, October 1980. Padova, October 1980 Padova, October 1980

Eddington Limit G = 1

m2 M = const.

const ~ 30

WR mass loss ratesare determined bycomposition changes

Maeder et al., A&A 539, A110 (2012) For homologous sequences

Page 6: Padova, October 1980. Padova, October 1980 Padova, October 1980

THERE IS ANEXTREME MASSLOSS RATES INPRE-SN STAGES

MASS

Page 7: Padova, October 1980. Padova, October 1980 Padova, October 1980

Mixing vs. mass loss :

1.137.05.0

3.0

1~~~

~~

MRMMR

MTRMT

m

m

MASS LOSS :

MIXING: shear ~ thermal diffusivity

Higher M Higher T Lower

2

3

34

PCTacK = Mass loss and mixing

strongly favoured !

3

~ TPP

gas

rad

Page 8: Padova, October 1980. Padova, October 1980 Padova, October 1980

-1. More fast rotators

Confirmed by:Wisniewski & Björkman, 2006Mokiem et al . 2006Martayan et al. 2007Martayan et al. 2010

Maeder, Grebel, Mermilliod 1999

THREE PROPERTIES OFROTATION AT LOW Z

Page 9: Padova, October 1980. Padova, October 1980 Padova, October 1980

Z=0.004

Z=0.02

- 2. Higher N/C at lower Z

MORE MIXING

Page 10: Padova, October 1980. Padova, October 1980 Padova, October 1980

Z=0.02: drastic deacrease for highmasses

Z=0.004: more stars reach break-up velocities.

Maeder & Meynet, 2001

-3. Low Z stars reach critical rotation ROTATIONALMASS LOSS

Page 11: Padova, October 1980. Padova, October 1980 Padova, October 1980

NEW STABILITY CRITERION Maeder et al. A&A, 553, A1 (2013)

RICHARDSON CRITERION

RAYLEIGH-TAYLOR

LEDOUX CRITERION

ZAHN

ZAHN

ULRICH, KIPPENHAHN

Possible dampingor amplificationof mixing effects !

DUDIS

SCHWARZSCHILD

STABLE , IF

Page 12: Padova, October 1980. Padova, October 1980 Padova, October 1980

Hunter et al. 2008

Page 13: Padova, October 1980. Padova, October 1980 Padova, October 1980

Maeder, Przybilla, Nieva et al. 2013

Page 14: Padova, October 1980. Padova, October 1980 Padova, October 1980

From VLT- FLAMES survey (Hunter et al. 2009)

Page 15: Padova, October 1980. Padova, October 1980 Padova, October 1980

NGC 3293-034

Ex. of fit of spectra and ADS models calculatedby Przybilla with Hunter et al. parameters Maeder, Przybilla, Nieva et al. 2013

Page 16: Padova, October 1980. Padova, October 1980 Padova, October 1980

0 50 100 150 200 250 300

Mg/H is not constant with v sin i ! Maeder, Przybilla, Nieva et al. 2013

Page 17: Padova, October 1980. Padova, October 1980 Padova, October 1980

Be stars

SB2

Maeder et al. (2008)

Data from Hunter et al (2008)

14 < M/MO < 20

Page 18: Padova, October 1980. Padova, October 1980 Padova, October 1980

BINARIES: Tidally shear induced mixing (TISM)Song, Maeder, Meynet, Huang, Ekström, Granada (2013)

Tidal interaction + meridional circulation + shears +horizontal turbulence in binary models (15 MO + 10 MO)

CASE SPIN UP: vini/vcrit=0.2 , Porb= 0.9-1.4 d

. .

Page 19: Padova, October 1980. Padova, October 1980 Padova, October 1980

STRONG MIXING before RLOF !

Page 20: Padova, October 1980. Padova, October 1980 Padova, October 1980

TISM in BINARIES

• Internal mixing and larger cores YIELDS

• Homogeneous before RLOF , for high masses thus, no RLOF !

• Differential rotation at synchronisation

• If spin up, lot of angular momentum conveyed to the

core GRBs ?

Page 21: Padova, October 1980. Padova, October 1980 Padova, October 1980

External magnetic field

ud-Doula & Owocki (2002)

Meynet, Eggenberger, Maeder 2011

Page 22: Padova, October 1980. Padova, October 1980 Padova, October 1980

10 M

Vini=200 km s-1

Z=0.014

Page 23: Padova, October 1980. Padova, October 1980 Padova, October 1980

Magnetic coupling coupling-envelope• Asteroseismology (KEPLER), red giant KIC 8366339: core rotates only 10 x faster than surface Beck et al. (2012), • Additional braking mechanism (Eggenberger et al. 2012)• Pulsar models rotate too fast (Heger et al. 2004)

Truncation radius:

Loss of angular momentum by the core:Maeder & MeynetIn prep.

Page 24: Padova, October 1980. Padova, October 1980 Padova, October 1980

•MASS LOSS•ROTATION-MIXING

•BINARY EVOLUTION

•MAGNETIC BRAKING

Effects of stellar physicson the chemical yields André Maeder Geneva Observatory

Collaborationwith Georges Meynet

Page 25: Padova, October 1980. Padova, October 1980 Padova, October 1980

NGC 3293-034

Ex. of fit of spectra and ADS models calculatedby Przybilla with Hunter et al. parameters Maeder, Przybilla, Nieva et al. 2013

Page 26: Padova, October 1980. Padova, October 1980 Padova, October 1980
Page 27: Padova, October 1980. Padova, October 1980 Padova, October 1980

Ekström, Meynet, Maeder 2005

At low Z: Large fraction of MS spent at break--up

Page 28: Padova, October 1980. Padova, October 1980 Padova, October 1980

Moderate N-enrichment

Initial track ~ homogeneous

Page 29: Padova, October 1980. Padova, October 1980 Padova, October 1980

BINARIES: Tidally shear induced mixing (TISM)Song, Maeder, Meynet, Huang, Ekström, Granada (2013)

Tidal interaction + meridional circulation + shears +horizontal turbulence in binary models (15 M + 10 M)

CASE SPIN DOWN: vini/vcrit=0.6 , Porb= 1.1-1.8 d

Page 30: Padova, October 1980. Padova, October 1980 Padova, October 1980

N/C vs. N/O plot: depends only on nuclear properties, Independent on mass and rotation, ~linear up to 0.6 (Maeder, Przybilla, Nieva ,Meynet et al. 2013)

a

Page 31: Padova, October 1980. Padova, October 1980 Padova, October 1980

N/C vs. N/O plot: depends only on nuclear properties, Independent on mass and rotation, ~linear up to 0.6 (Maeder, Przybilla, Nieva ,Meynet et al. 2013)

CN-cycle

N-cycle

Page 32: Padova, October 1980. Padova, October 1980 Padova, October 1980

From VLT- FLAMES survey (Hunter et al. 2009)

Page 33: Padova, October 1980. Padova, October 1980 Padova, October 1980

Case spin up

CASE SPIN UP: vini/vcrit=0.2 , Porb= 0.9-1.4 d