Energetic ions in ITER plasmas

被引:121
作者
Pinches, S. D. [1 ]
Chapman, I. T. [2 ]
Lauber, Ph. W. [3 ]
Oliver, H. J. C. [2 ,4 ]
Sharapov, S. E. [2 ]
Shinohara, K. [5 ]
Tani, K. [6 ]
机构
[1] ITER Org, F-13067 St Paul Les Durance, France
[2] CCFE, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England
[3] EURATOM, Max Planck Inst Plasmaphys, D-85748 Garching, Germany
[4] Univ Bristol, HH Wills Phys Lab, Bristol BS8 1TL, Avon, England
[5] Japan Atom Energy Agcy, Naka, Ibaraki 3110193, Japan
[6] Nippon Adv Technol Co Ltd, Naka, Ibaraki 3110102, Japan
基金
英国工程与自然科学研究理事会;
关键词
SHEAR-ALFVEN EIGENMODES; WALL MODE STABILIZATION; EUROPEAN TORUS PLASMAS; FUSION ALPHA-PARTICLES; MAGNETIC-FIELD RIPPLE; SAWTOOTH OSCILLATIONS; KINETIC-THEORY; JET; STABILITY; SAWTEETH;
D O I
10.1063/1.4908551
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
This paper discusses the behaviour and consequences of the expected populations of energetic ions in ITER plasmas. It begins with a careful analytic and numerical consideration of the stability of Alfven Eigenmodes in the ITER 15 MA baseline scenario. The stability threshold is determined by balancing the energetic ion drive against the dominant damping mechanisms and it is found that only in the outer half of the plasma (r/a > 0.5) can the fast ions overcome the thermal ion Landau damping. This is in spite of the reduced numbers of alpha-particles and beam ions in this region but means that any Alfven Eigenmode-induced redistribution is not expected to influence the fusion burn process. The influence of energetic ions upon the main global MHD phenomena expected in ITER's primary operating scenarios, including sawteeth, neoclassical tearing modes and Resistive Wall Modes, is also reviewed. Fast ion losses due to the non-axisymmetric fields arising from the finite number of toroidal field coils, the inclusion of ferromagnetic inserts, the presence of test blanket modules containing ferromagnetic material, and the fields created by the Edge Localised Mode (ELM) control coils in ITER are discussed. The greatest losses and associated heat loads onto the plasma facing components arise due to the use of the ELM control coils and come from neutral beam ions that are ionised in the plasma edge.
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页数:26
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