Book contents
- Frontmatter
- Contents
- Preface
- 1 A selective overview
- I Stellar convection and oscillations
- II Stellar rotation and magnetic fields
- 6 Stellar rotation: a historical survey
- 7 The oscillations of rapidly rotating stars
- 8 Solar tachocline dynamics: eddy viscosity, anti-friction, or something in between?
- 9 Dynamics of the solar tachocline
- 10 Dynamo processes: the interaction of turbulence and magnetic fields
- 11 Dynamos in planets
- III Physics and structure of stellar interiors
- IV Helio- and asteroseismology
- V Large-scale numerical experiments
- VI Dynamics
7 - The oscillations of rapidly rotating stars
Published online by Cambridge University Press: 11 November 2009
- Frontmatter
- Contents
- Preface
- 1 A selective overview
- I Stellar convection and oscillations
- II Stellar rotation and magnetic fields
- 6 Stellar rotation: a historical survey
- 7 The oscillations of rapidly rotating stars
- 8 Solar tachocline dynamics: eddy viscosity, anti-friction, or something in between?
- 9 Dynamics of the solar tachocline
- 10 Dynamo processes: the interaction of turbulence and magnetic fields
- 11 Dynamos in planets
- III Physics and structure of stellar interiors
- IV Helio- and asteroseismology
- V Large-scale numerical experiments
- VI Dynamics
Summary
We review the effects of rotation on the oscillation spectrum of rapidly rotating stars. We particularly stress the novelties introduced by rotation: for instance, the disappearance of modes in the low frequency band due to the ill-posed natured of the underlying mathematical problem. This is mainly an effect of the Coriolis acceleration. The centrifugal effect changes the shape of the star in the first place. The possible consequences of this deformation on the oscillation spectrum are briefly analyzed. We also describe other possibly important effects of the centrifugal acceleration which come about on the time scale of star evolution.
A short introduction to rapidly rotating stars
All stars are affected by rotation but some of them, the rapid rotators, are more affected than the others! Astronomers usually qualify as rapid rotators all the stars with v sin i ≥ 50 kms−1, i.e. those with an equatorial velocity larger than 50kms−1. Such a value should be compared to the Keplerian limiting velocity which is
Vkep ∼ 440kms−1 (M/M⊙)0.1
for stars on the main sequence (we used the mass-radius relation given by Hansen and Kawaler 1994). Thus, for these stars the limiting velocity is weakly mass-dependent and rapid rotators appear as stars whose centrifugal acceleration exceeds 10% of the surface gravity; since this ratio measures the impact of rotation on the star structure, rapid rotators are those stars whose shape is significantly distorted by rotation.
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- Chapter
- Information
- Stellar Astrophysical Fluid Dynamics , pp. 99 - 110Publisher: Cambridge University PressPrint publication year: 2003