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
11 - Dynamos in planets
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
Significant advances in our understanding of the geodynamo have been made over the last ten years. In this review, we consider the extent to which this knowledge can be used to understand the origin of the magnetic fields in other planets. Since there is much less observational data available, this requires a ‘first principles’ understanding of the physics of convection driven dynamos.
Introduction
The basic structure of the interior of the Earth has been worked out by seismologists. The iron core is divided at ricb = 1220 km, the inner core boundary (ICB), into the solid, mainly iron, inner core below and the fluid outer core above. The exact composition of the outer core is not known, but the most plausible models suggest it is a mixture of liquid iron and various impurities, probably sulphur and oxygen (Alfè et al., 2000). The whole core is electrically conducting. Above the core-mantle boundary (CMB), at rcmb = 3485 km, lies the rocky mantle. The electrical conductivity of the mantle is very small, except possibly very close to the CMB itself, where iron may have leaked into the mantle. The basic structure of the other terrestrial planets, in which we include the larger satellites, is believed to be similar to that of the Earth, but the size of the iron core varies considerably, and the division between the fluid outer core and the solid inner core, if it exists, has to be computed from theoretical models.
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- Information
- Stellar Astrophysical Fluid Dynamics , pp. 159 - 176Publisher: Cambridge University PressPrint publication year: 2003
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