Study of thermonuclear Alfven instabilities in next step burning plasma proposals

被引:58
作者
Gorelenkov, NN
Berk, HL
Budny, R
Cheng, CZ
Fu, GY
Heidbrink, WW
Kramer, GJ
Meade, D
Nazikian, R
机构
[1] Princeton Plasma Phys Lab, Princeton, NJ 08543 USA
[2] IFS, Austin, TX USA
[3] Univ Calif Irvine, Irvine, CA 92697 USA
关键词
D O I
10.1088/0029-5515/43/7/313
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
The stability of a-particle driven shear Alfven eigenmodes (AE) for nominal burning plasma (BP) parameters in the proposed international tokamak experimental reactor (ITER), fusion ignition research experiment (FIRE) and IGNITOR tokamaks is studied. JET plasma, where fusion as were generated in tritium experiments, is also studied to compare the numerical predictions with the existing experiments. An analytic assessment of toroidal AE (TAE) stability is first presented, where the alpha-particle beta due to the fusion reaction rate and electron drag is simply and accurately estimated in plasmas with central temperature in the range of 7-20 keV. In this assessment the hot particle drive is balanced against ion-Landau damping of the background deuterons, and electron collision effects and stability boundaries are determined. Then two numerical studies of AE instability are presented. In one, the HIgh-n STability (HINST) code is used to predict the instabilities of low and moderately high frequency Alfven modes. HINST computes the non-perturbative solutions of the AE including effects of ion finite Larmor radius, orbit width, trapped electrons etc. The stability calculations are repeated using the global code NOVAK. We show that for these plasmas the spectrum of the least stable AE modes is at medium-/high-n numbers. In HINST, TAEs are locally unstable due to the alpha pressure gradient in all the devices under consideration except IGNITOR. However, NOVAK calculations show that the global mode structure enhances the damping mechanisms and produces stability for the nominal FIRE proposal and near-marginal stability for the nominal ITER proposal. NBI ions produce a strong stabilizing effect for JET. However, in ITER, the beam energies needed to penetrate to the core must be high (similar to1 MeV) so that a diamagnetic drift frequency comparable to that of alpha-particles is produced by the beam ions which induces a destabilizing effect. A serious question remains whether the perturbation theory used in NOVAK overestimates the stability predictions, so that it is premature to conclude that the nominal operation of all three BP proposals without neutral beam injection are stable (or marginally stable) to AEs.
引用
收藏
页码:594 / 605
页数:12
相关论文
共 40 条
[1]   ARBITRARY MODE NUMBER BOUNDARY-LAYER THEORY FOR NONIDEAL TOROIDAL ALFVEN MODES [J].
BERK, HL ;
METT, RR ;
LINDBERG, DM .
PHYSICS OF FLUIDS B-PLASMA PHYSICS, 1993, 5 (11) :3969-3996
[2]  
BERK HL, 1992, PHYS LETT, pA475
[3]   The combined effect of EPMs and TAEs on energetic ion confinement and sawtooth stabilization [J].
Bernabei, S ;
Budny, RV ;
Fredrickson, ED ;
Gorelenkov, NN ;
Hosea, JC ;
Phillips, CK ;
White, RB ;
Wilson, JR ;
Petty, CC ;
Pinsker, RI ;
Harvey, RW ;
Smirnov, AP .
NUCLEAR FUSION, 2001, 41 (05) :513-518
[4]   Beam driven Alfven eigenmodes and fishbones in JET [J].
Borba, D ;
Alper, B ;
Budny, RV ;
Fasoli, A ;
Heeter, RF ;
Kerner, W ;
Sharapov, SE ;
Smeulders, P .
NUCLEAR FUSION, 2000, 40 (04) :775-783
[5]   ENERGETIC PARTICLE DRIVE FOR TOROIDICITY-INDUCED ALFVEN EIGENMODES AND KINETIC TOROIDICITY-INDUCED ALFVEN EIGENMODES IN A LOW-SHEAR TOKAMAK [J].
BREIZMAN, BN ;
SHARAPOV, SE .
PLASMA PHYSICS AND CONTROLLED FUSION, 1995, 37 (10) :1057-1074
[6]  
BRIGUGLIO, 1995, PHYS PLASMAS CONTR A, V279, P37
[7]   Fusion alpha parameters in tokamaks with high DT fusion rates [J].
Budny, RV .
NUCLEAR FUSION, 2002, 42 (12) :1383-1393
[8]   The physics of the International Thermonuclear Experimental Reactor FEAT [J].
Campbell, DJ .
PHYSICS OF PLASMAS, 2001, 8 (05) :2041-2049
[9]   NONIDEAL THEORY OF TOROIDAL ALFVEN EIGENMODES [J].
CANDY, J ;
ROSENBLUTH, MN .
PHYSICS OF PLASMAS, 1994, 1 (02) :356-372
[10]  
CHEN CZ, 1991, PHYS FLUID B, V3