Book contents
- Frontmatter
- Contents
- Preface
- Introduction
- 1 Fundamentals of Dynamo Theory
- 2 Solar and Stellar Dynamos
- 3 Convection and Magnetoconvection in a Rapidly Rotating Sphere
- 4 Solar Dynamos; Computational Background
- 5 Energy Sources for Planetary Dynamos
- 6 Fast Dynamos
- 7 Nonlinear Planetary Dynamos
- 8 The Chaotic Solar Cycle
- 9 The Nonlinear Dynamo and Model-Z
- 10 Maps and Dynamos
- 11 Bifurcations in Rotating Systems
- Index
1 - Fundamentals of Dynamo Theory
Published online by Cambridge University Press: 25 January 2010
- Frontmatter
- Contents
- Preface
- Introduction
- 1 Fundamentals of Dynamo Theory
- 2 Solar and Stellar Dynamos
- 3 Convection and Magnetoconvection in a Rapidly Rotating Sphere
- 4 Solar Dynamos; Computational Background
- 5 Energy Sources for Planetary Dynamos
- 6 Fast Dynamos
- 7 Nonlinear Planetary Dynamos
- 8 The Chaotic Solar Cycle
- 9 The Nonlinear Dynamo and Model-Z
- 10 Maps and Dynamos
- 11 Bifurcations in Rotating Systems
- Index
Summary
INTRODUCTION
Cosmic Dynamos
Many stars, planets and galaxies possess magnetic fields whose origins are not easily explained. Even the ‘solid’ planets cannot be sufficiently ferromagnetic to account for their magnetism, for the bulk of their interiors are above the Curie temperature at which permanent magnetism disappears; obviously the stars and galaxies cannot be ferromagnetic at all. Nor are the magnetic fields transient phenomena that just happen to be present today. Palaeomagnetism, the study of magnetic fields ‘fossilized’ in rocks at the time of their formation in the remote geological past, shows that Earth's magnetic field has existed at much its present strength for the past 3 x 109 years, at least. But, unless they contain sources of electric current, conducting bodies of spatial dimension, L, can retain their magnetic fields only for times of the order of the electromagnetic diffusion time τη = L2/η, where η is the magnetic diffusivity of their constituents; η = l/μ0σ, where σ is their electrical conductivity and μ0 is the permeability of free space. (SI units are used throughout.) Being proportional to L2, this time may be very considerable, but is as nothing compared with the ages of the bodies concerned. For example, Earth contains a highly conducting region, its core, of radius about L = 3.48 x 100 m, and its conductivity is about 4 x 105 S/m. This gives η ≍ 2 m2/s and τη ≍ 200,000 years. Similarly, it is thought that the magnetic fields of other planets cannot be fossil relicts of their birth. A mechanism is required to maintain them.
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- Lectures on Solar and Planetary Dynamos , pp. 1 - 58Publisher: Cambridge University PressPrint publication year: 1994
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