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Turbulence and instabilities in magnetised plasmas. Volume 2, Gyrokinetic theory and gyrofluid turbulence. / Bruce Scott.
- Format:
- Book
- Author/Creator:
- Scott, Bruce, author.
- Series:
- IOP Series in Plasma Physics Series
- Language:
- English
- Subjects (All):
- Plasma instabilities.
- Physical Description:
- 1 online resource (526 pages)
- Edition:
- First edition.
- Place of Publication:
- Bristol, England : IOP Publishing, [2021]
- Summary:
- This book is the second of a two-volume set, providing a comprehensive fundamental introduction to gyrokinetic theory and gyrofluid turbulence.
- Contents:
- Intro
- Preface
- Outline placeholder
- Preface to both volumes
- Author biography
- Bruce Scott
- Chapter 1 Prelude to volume two
- 1.1 Plasma, magnetised, parameters
- 1.2 Low frequency, flute mode ordering
- 1.3 Drifts, ExB flow, currents
- 1.4 Polarisation and quasineutrality
- 1.5 Turbulence
- 1.5.1 Energy and enstrophy
- 1.5.2 Magnetic field responses
- 1.6 Turbulence in magnetised plasmas
- 1.6.1 Adiabatic response
- 1.6.2 Two-fluid dynamics
- 1.6.3 Energetics
- 1.6.4 Total-f versus delta-f models
- 1.6.5 Mode structure
- 1.7 Kinetic theory, turbulence, and MHD instabilities
- Further Reading
- Chapter 2 Effects of the electron temperature
- 2.1 Introduction-electron temperature
- 2.2 Conservative effects
- 2.2.1 Parallel dynamics and energetics
- 2.2.2 Diamagnetic fluxes and energetics
- 2.2.3 Gradient forcing
- 2.3 Dissipative effects
- 2.3.1 Conventional treatment
- 2.3.2 Time dependent heat flux
- 2.4 Equations for magnetised plasma turbulence
- 2.5 Parameters, normalised equations, geometry
- 2.5.1 Parameters
- 2.5.2 Normalisation
- 2.5.3 Equations
- 2.5.4 Magnetic geometry
- 2.5.5 Numerics
- 2.6 Energetics
- 2.7 Heat flux and kinetic shear Alfvén waves
- 2.8 Drift Alfvén turbulence
- 2.8.1 Computational examples
- 2.9 Mode structure
- 2.9.1 Details of the energetics
- 2.10 Dependence on parameters
- 2.10.1 Electromagnetic induction
- 2.10.2 The heat flux versus its collisional form
- 2.10.3 Thermal effect on electromagnetic responses
- 2.11 Summary
- Chapter 3 Effects of the ion temperature
- 3.1 Introduction-ion temperature as independent
- 3.2 The Larmor radius and gyro averaging
- 3.3 Gyroaveraging versus gyroviscosity
- 3.4 Effects on cold ion dynamics
- 3.5 Ion temperature gradient (ITG) modes
- 3.6 Warm-ion toroidal drift Alfvén model
- 3.6.1 Equations.
- 3.6.2 Energetics
- 3.7 Electromagnetic ITG turbulence in a hot plasma
- 3.7.1 Mode structure
- 3.7.2 Microtearing and the electron energetics
- 3.7.3 Gradient threshold
- 3.8 Warm ion drift Alfvén turbulence
- 3.8.1 Inductivity
- 3.8.2 Collisionality
- 3.8.3 Gradient synergy
- 3.8.4 The heat flux versus its collisional form
- 3.9 On gyroviscosity
- 3.9.1 Gyroviscous cancellation in the brackets
- 3.9.2 Effect on energetics
- 3.9.3 Effect on the turbulence
- 3.10 Summary
- Chapter 4 Lagrangian field theory and drifts
- 4.1 Low frequency drifts
- 4.1.1 Meaning/significance of ExB drift motion
- 4.1.2 Outline of the rest of this lecture
- 4.2 Lagrangian field theory
- 4.3 Canonical representation
- 4.3.1 Canonical form
- 4.3.2 Canonical representation of electrodynamics
- 4.4 Lagrangian field theory in canonical form
- 4.4.1 Functional derivatives for the fields
- 4.4.2 For electrodynamics
- 4.5 Towards drifts
- 4.6 Quasineutrality
- 4.7 Interlude-Noether's theorem
- 4.7.1 Symmetry and total variations
- 4.7.2 Example of a single particle in a field
- 4.7.3 Self-consistent field
- 4.7.4 Maxwell's equations
- 4.7.5 Spatial dependence in the background
- Chapter 5 Introduction to gyrokinetic theory
- 5.1 Ideas behind the gyrokinetic representation
- 5.2 Lagrangian basis of kinetic theory
- 5.2.1 Euler-Lagrange equations
- 5.3 The strategy of gyrokinetics
- 5.4 The drift-kinetic Lagrangian
- 5.5 The field variables as perturbations
- 5.6 The Lie transform
- 5.6.1 The Lie derivative
- 5.6.2 Initial arrangement
- 5.6.3 First order
- 5.6.4 Second order-polarisation
- 5.6.5 Collected result
- 5.7 The gyroaverage
- 5.7.1 Continuous basis
- 5.7.2 Integration space
- 5.8 The gyrocentre phase space density and flow
- 5.9 The gyrokinetic field Lagrangian.
- 5.9.1 Field equations
- 5.10 Simplified limits
- 5.10.1 Electrostatic polarisation
- 5.10.2 Linearised polarisation
- 5.10.3 No gyroaveraging in induction
- 5.10.4 Long wavelengths
- 5.10.5 Importance of energetic consistency
- Chapter 6 Phase space and energetic consistency
- 6.1 Summary of ideas
- 6.2 Basic structure of the model
- 6.3 The Euler-Lagrange equations for gyrocentres
- 6.4 Symmetry in gyrocentre dynamics
- 6.4.1 Poisson bracket form
- 6.4.2 Phase space incompressibility
- 6.4.3 Phase space conservation
- 6.5 Application of Noether's theorem
- 6.6 Energy conservation
- 6.7 Momentum conservation
- 6.7.1 Plasma versus canonical momentum
- 6.7.2 The polarisation cancellation
- 6.7.3 Wave fluxes
- 6.7.4 Local momentum conservation
- 6.7.5 MHD correspondence
- 6.7.6 Computational consistency
- 6.8 Gyrokinetic drifts
- 6.9 Gyrokinetic energetics
- 6.9.1 Long-wave electrostatic systems
- 6.9.2 Electromagnetic energetics
- 6.10 Simplified geometry and the form of the Jacobian
- Chapter 7 Gyrokinetic theory for local dynamics
- 7.1 Ideas behind delta-f gyrokinetics
- 7.2 Total-f Lagrangian and energetics
- 7.3 Linearised polarisation
- 7.3.1 Conserved energy
- 7.3.2 Field equations
- 7.4 The free energy
- 7.5 Sketch of the delta-f approach
- 7.6 Systematics of the delta-f equations
- 7.6.1 Field equations
- 7.7 Delta-f energetics and correspondence
- 7.7.1 Field equations
- 7.8 On consistency
- 7.8.1 Parallel phase space consistency
- 7.8.2 Difficulty of a global model
- 7.9 The gyroaveraged magnetic field
- 7.10 What happened to momentum
- Chapter 8 Gyrokinetic treatment of waves
- 8.1 Introduction
- 8.2 Kinetic responses
- 8.2.1 Landau damping
- 8.3 Adiabatic drift acoustic wave
- 8.3.1 Drift waves with electron Landau damping.
- 8.4 Kinetic shear Alfvén wave
- 8.5 Drift-Alfvén wave
- 8.6 Landau damping as thermal conduction
- 8.6.1 Symmetrisation into even and odd components
- 8.6.2 Evolution of the field variables
- 8.6.3 The wave equation and thermal conduction
- 8.7 Kinetic resonance-Landau damping
- 8.8 Summary
- Chapter 9 Introduction to gyrofluid theory
- 9.1 Introduction
- 9.2 Heuristic gyrofluid 2D turbulence
- 9.3 Heuristic gyrofluid 3D turbulence
- 9.4 Gyrofluid systematics
- 9.4.1 Representation
- 9.4.2 Free energy
- 9.4.3 On not gyroaveraging the magnetic potential
- 9.4.4 Field variable equations
- 9.4.5 Moment variable equations
- 9.4.6 Auxiliary gyrofluid variables
- 9.4.7 ExB advection
- 9.4.8 Curvature terms
- 9.4.9 Parallel dynamics
- 9.4.10 The Landau closure
- 9.4.11 Expression of the moment equations
- 9.4.12 System normalisation
- 9.5 Gyrofluid energetics
- 9.6 Summary
- Chapter 10 Gyrofluid equations for thermal dynamics
- 10.1 Introduction
- 10.2 The gyrofluid model with thermal responses
- 10.2.1 List of moment variables
- 10.2.2 Moment variable equations
- 10.2.3 Field equations
- 10.3 Collisions in general
- 10.4 Thermal gyrofluid energetics
- 10.5 Correspondence to the fluid model
- 10.5.1 Polarisation and vorticity
- 10.5.2 Thermal conduction
- 10.5.3 Thermal anisotropy and parallel viscosity
- 10.6 On usefulness
- Chapter 11 Gyrofluid Drift-Alfvén turbulence
- 11.1 Introduction-gyrofluid turbulence
- 11.2 Electromagnetic gyrofluid equations
- 11.2.1 Six-moment electromagnetic equations
- 11.2.2 Collisional dissipation
- 11.2.3 Field equations
- 11.3 Energetics
- 11.4 ITG turbulence in a hot plasma
- 11.4.1 Dependence on inductivity
- 11.4.2 Temperature gradient threshold
- 11.4.3 Stabilisation by flows.
- 11.4.4 Comparison to the fluid drift model
- 11.5 Drift Alfvén turbulence in a warm plasma
- 11.6 Thermal anisotropy
- 11.6.1 in temperature responses
- 11.6.2 in flows
- 11.7 Summary
- Chapter 12 Electron gyroscale turbulence
- 12.1 Introduction-the gyroscale
- 12.2 Responses below the ion gyroradius
- 12.3 Heuristic 2D electron gyroscale model
- 12.4 ITG and ETG isomorphism
- 12.4.1 Flows and the adiabatic response
- 12.4.2 Polarisation in the ETG and ITG or EZF models
- 12.5 Three-dimensional adiabatic ETG turbulence
- 12.5.1 Normalised gyrofluid moment equations
- 12.5.2 ETG and EZF polarisation and induction
- 12.5.3 Comparison within the standard case
- 12.5.4 Dependence on the temperature gradient
- 12.5.5 Dependence on inductivity
- 12.5.6 Dependence on radial domain size
- 12.5.7 Dependence on field line length
- 12.5.8 The warm plasma case, steeper gradients
- 12.6 The two-scale problem
- 12.6.1 Computational requirements for the two-scale problem
- 12.6.2 The hot plasma case
- 12.6.3 The warm plasma case
- 12.6.4 The two-scale problem is work in progress
- 12.7 Summary
- Chapter 13 Trapped-electron turbulence
- 13.1 Introduction-magnetic trapping
- 13.2 Gyrokinetic Hamiltonian in a system with symmetry
- 13.2.1 Simplest case: 1D mirror field
- 13.2.2 The dipole magnetic field
- 13.2.3 The tokamak magnetic field
- 13.3 The toroidal precession drift
- 13.3.1 Equilibrium and Orthogonal Coordinates
- 13.3.2 Drift combinations
- 13.3.3 The tokamak magnetic field
- 13.3.4 The dipole magnetic field
- 13.3.5 Contrast to the tokamak case
- 13.4 Single-centre drifts versus gyrokinetics
- 13.5 Trapped electrons as separate species in turbulence
- 13.5.1 Bounce averaged objects
- 13.5.2 Simple exposition of the energetics.
- 13.5.3 Integration into the six moment gyrofluid model.
- Notes:
- Description based on publisher supplied metadata and other sources.
- Description based on print version record.
- ISBN:
- 9780750344746
- 0750344741
- OCLC:
- 1429732518
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