surface abundances of am stars as a constraint on rotational mixing olivier richard 1,2, suzanne...
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Surface abundances of Am Surface abundances of Am stars stars
as a constraint on rotational as a constraint on rotational mixingmixing
Olivier Richard1,2, Suzanne Talon2, Georges Michaud2
1 GRAAL UMR5024, Université Montpellier II, Montpellier, France
2 Département de physique, Université de Montréal, Montréal, Canada
• Am stars
• Montréal Models
• Results
Surface abundances of Am Surface abundances of Am stars stars
as a constraint on rotational as a constraint on rotational mixingmixing
• Statistics suggest all non-magnetic stars with V<80 km/s• Recent observations in open clusters
Mg~ normal Al, Si, S: ~normal or slight overabundance Ca ~ normal or underabundant Ni and Fe overabundant
Am StarsAm Stars
Burger’s equationsBurger’s equations
• 2 equations for each species (28 in the code)• Solved for each mesh points (~1500)• and at each time step (~1000)
5 5
2 2
j i i jii i i i
j i j
ji ij i
ij ij
ijij ij j
j i
j
r di
j i
a
ij
m r m rPm N g N Z eE
r m m
mTN k a r b
w wg
rr m m
K
w
z
zK w
Radiative accelerationsRadiative accelerations
• 1.5 GigaBytes of data ; OPAL (1996)– Integration over
fraction of photons given to i at each frequency
2 0
1 ( )
(to( ) )
l)(
t4 a
ru
adr
ia
Rr
ud
LP u d
ig u
r c Xi
Expression used in evolution calculations
hu
kT
4
24
15( )
4 1
u
u
u eP u
e
( )u i
(total)u
(Fe)u
(Li)u
Mixing modelMixing model
• Simplest version of the turbulent diffusion coefficient obtained from self-consistent treatment of the meridional circulation following Zahn (1992)
• Mixing added to the code as a diffusion process with a parametric mixing diffusion coefficient:
TnD
Mixing modelMixing model
• Simplest version of the turbulent diffusion coefficient obtained from self-consistent treatment of the meridional circulation following Zahn (1992)
• Mixing added to the code as a diffusion process with a parametric mixing diffusion coefficient:
TnD
Computed modelsComputed models
• Models of 1.7 and 1.9 solar masses
• With mixing coefficient corresponding to surface velocity of 50 km/s (V50), 15 km/s (V15), and 5 km/s (V5, V5N)
Richer et al. (2000) 1.9R300-2 and 1.9R1k-2 models
Effective temperature and surface gravity evolution
1.9
1.7
Radiative acceleration in the 1.9 solar masses models
Abundance profiles at 800 Myr
Model 1.9V5
r
1
0
Abundance evolution in the 1.9 solar masses models
The Praesepe star HD73045
The Praesepe star HD73045
Conclusion
• In the mixing model the turbulence seems to be too strong to allow the Am phenomenon to occur at a reasonable velocity
• Need of self-consistent abundance determination for a lot of chemical species in stars of different ages and metallicity