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This book bridges the gap between general plasma physics lectures and the real world problems in MHD stability. In order to support the understanding of concepts and their implication, it refers to real world problems such as toroidal mode coupling or nonlinear evolution in a conceptual and phenomenological approach. Detailed mathematical treatment will involve classical linear stability analysis and an outline of more recent concepts such as the ballooning formalism. The book is based on lectures that the author has given to Master and PhD students in Fusion Plasma Physics. Due its strong link to experimental results in MHD instabilities, the book is also of use to senior researchers in the field, i.e. experimental physicists and engineers in fusion reactor science.The volume is organized in three parts. It starts with an introduction to the MHD equations, a section on toroidal equilibrium (tokamak and stellarator), and on linear stability analysis. Starting from there, the ideal MHD stability of the tokamak configuration will be treated in the second part which is subdivided into current driven and pressure driven MHD. This includes many examples with reference to experimental results for important MHD instabilities such as kinks and their transformation to RWMs, infernal modes, peeling modes, ballooning modes and their relation to ELMs. Finally the coverage is completed by a chapter on resistive stability explaining reconnection and island formation. Again, examples from recent tokamak MHD such as sawteeth, CTMs, NTMs and their relation to disruptions are extensively discussed.
Auteur
Hartmut Zohm is Director of the Tokamak Scenario Development Division at the Max-Planck-Institute for Plasma Physics located in Garching, Germany. His main fields of interest are the magnetohydrodynamic (MHD) stability of fusion plasmas and their heating by Electron Cyclotron Resonance Heating (ECRH). By combining these two fields, he pioneered the active stabilisation of neoclassical magnetic islands, which set a major performance limit to the tokamak, by ECRH. His present field is the study of tokamak physics on the ASDEX Upgrade tokamak which is operated by his department.
Professor Zohm has published a total of more than 200 papers. He is member of several international committees such as the ITPA coordinating committee, the IEA Implementing Agreement on Collaboration of Tokamak Programmes, the Programme Advisory Committees of MAST, KSTAR, DIII-D and the scientific advisory board of IPP.CR and the EU Fusion STAC. He is also a member of the board of editors of the 'Nuclear Fusion' journal and a member of the advisory boards of the 'Annalen der Physik' journal.
Contenu
Preface IX
1 The MHD Equations 1
1.1 Derivation of the MHD Equations 1
1.1.1 Multispecies MHD Equations 1
1.1.2 One-Fluid Model of Magnetohydrodynamics 4
1.1.3 Validity of the One-Fluid Model of Magnetohydrodynamics 6
1.2 Consequences of the MHD Equations 8
1.2.1 Magnetic Flux Conservation 8
1.2.2 MHD Equilibrium 10
1.2.3 Magnetohydrodynamic Waves 11
1.2.3.1 Compressional Alfvén Waves 12
1.2.3.2 Shear Alfvén Waves 13
2 MHD Equilibria in Fusion Plasmas 15
2.1 Linear Congurations 15
2.1.1 The z-Pinch 15
2.1.2 The Screw Pinch 18
2.2 Toroidal Congurations 22
2.2.1 The Tokamak 23
2.2.1.1 The GradShafranov Equation 23
2.2.1.2 Circular Cross Section 27
2.2.1.3 Arbitrary Cross Section 32
2.2.1.4 The Straight Field Line Angle 34
2.2.2 The Stellarator 37
3 Linear Ideal MHD Stability Analysis 43
3.1 Linear MHD Stability as an Initial Value Problem 44
3.2 The Energy Principle of Ideal MHD 47
3.3 Forms of 𝛿W 48
3.4 The Ideal MHD Energy Principle for the Tokamak 51
4 Current Driven Ideal MHD Modes in a Tokamak 55
4.1 Expression for 𝛿W in Tokamak Ordering 55
4.2 External Kinks in a Tokamak with 𝛽= 0 56
4.2.1 Modes with m = 1 56
4.2.2 Modes with m 2 58
4.3 Internal Kink Modes 61
4.4 n = 0 Modes: The Vertical Displacement Event (VDE) 63
5 Pressure Driven Modes in a Tokamak 69
5.1 Localized Interchange Modes in the Screw Pinch 69
5.2 Localized Pressure Driven Modes in the Tokamak 72
5.2.1 Interchange Modes in a Tokamak 73
5.2.2 Ballooning Modes 76
6 Combined Pressure and Current Driven Modes: Edge Localized Modes 83
6.1 ELM Phenomenology 84
6.2 Linear Stability of the Pedestal 86
6.3 Non-linear Evolution 90
6.3.1 Non-linear Cycles 90
6.3.2 Magnitude of the ELM Crash 92
6.3.3 Timescale of the ELM Crash 94
6.4 ELM Control 94
6.4.1 Small ELM Regimes 95
6.4.2 Active ELM Control 97
7 Combined Pressure and Current Driven Modes: The Ideal 𝜷-Limit 103
7.1 Tokamak Operational Scenarios 103
7.2 External Kink Modes in a Tokamak with Finite 𝛽105
7.3 The Eect of a Conducting Wall on External Kink Modes 107
7.3.1 Ideally Conducting Wall 107
7.3.2 Resistive Wall 110
7.4 The Resistive Wall Mode (RWM) 112
7.5 The Troyon Limit 118
8 Resistive MHD Stability 123
8.1 Stability of Current Sheets 124
8.2 Reconnection in the Presence of a Guide Field 127
8.3 Magnetic Islands in Tokamaks 134
8.4 The Rutherford Equation 137
9 Current Driven ('classical') Tearing Modes in Tokamaks 141
9.1 Eect of Tearing Modes on Kinetic Proles 141
9.2 Nonlinear Saturation 144
9.3 Tearing Mode Rotation and Locking 146
9.3.1 Rotation of Tearing Modes in Tokamaks 146
9.3.2 Locking of Pre-existing Magnetic Islands 148
9.3.3 Ab-initio Locked Modes 152
10 Disruptions 159
10.1 Phenomenology of Disruptions 159
10.1.1 The Density Limit 161
10.2 Consequences of Disruptions 165
10.2.1 Thermal Loads 165
10.2.2 Mechanical Loads 166
10.2.3 Runaway Generation 168
10.3 Disruption Avoidance and Mitigation 171
11 M=1 Modes beyond Ideal MHD: Sawteeth and Fishbones 175
11.1 The Sawtooth Instability 17
11.1.1 Phenomenology 175
11.1.2 Sawtooth Period and Onset Criterion 17
11.1.3 Models for the Sawtooth Crash 181 11.2 The Fishbone Instability 184</p&g...