Padova, October 1980. Padova, October 1980 Padova, October 1980.

33
Padova, October 1980

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 of Padova, October 1980. Padova, October 1980 Padova, October 1980.

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