Theoretical investigation of field-line quality in a driven spheromak

被引:10
作者
Cohen, RH
Berk, HL
Cohen, BI
Fowler, TK
Hooper, EB
LoDestro, LL
Morse, EC
Pearlstein, LD
Rognlien, TD
Ryutov, DD
Sovinec, CR
Woodruff, S
机构
[1] Lawrence Livermore Natl Lab, Livermore, CA 94550 USA
[2] Univ Texas, Inst Fus Studies, Austin, TX 78712 USA
[3] Univ Calif Berkeley, Dept Nucl Engn, Berkeley, CA 94720 USA
[4] Univ Wisconsin, Madison, WI 53706 USA
关键词
D O I
10.1088/0029-5515/43/10/025
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
Theoretical studies aimed at predicting and diagnosing field-line quality in a spheromak are described. These include nonlinear three-dimensional MHD simulations and analyses of confinement in spheromaks dominated by either open (stochastic) field lines or approximate flux surfaces. Three-dimensional nonlinear MHD simulations confirm that field lines are predominantly open when there is a large-amplitude toroidal-mode-number n = 1 mode. However, an appreciable volume of good flux surfaces can be obtained either during the drive-off phase of a scheme with periodic pulsed drive or for an extended period under driven conditions, with oscillating volume, when the odd-n modes are suppressed. If a configuration with radially localized perturbations can be achieved, a scaling analysis for a Rosenbluth-Bussac spheromak equilibrium indicates a favourable (1/Lundquist number) scaling to larger, higher-field devices. A hyper-resistivity analysis, which also assumes small-scale perturbations, reproduces well magnetic probe data in the sustained spheromak physics experiment, while an analysis of the same experiment based on one-dimensional transport along open field lines contradicts experimental observations in several key ways. The scaling analysis is also applied to reversed-field pinches and indicates that a completely determined scaling can be obtained with less approximation to the resistive MHD equations than indicated in the previous literature.
引用
收藏
页码:1220 / 1234
页数:15
相关论文
共 23 条
[1]  
[Anonymous], PLASMA BOUNDARY MAGN
[2]  
BERK HL, 2001, UCRLID142741 LAWR LI
[3]   OHM LAW FOR MEAN MAGNETIC-FIELDS [J].
BOOZER, AH .
JOURNAL OF PLASMA PHYSICS, 1986, 35 :133-139
[4]   GALERKIN APPROXIMATIONS FOR DISSIPATIVE MAGNETOHYDRODYNAMICS [J].
CHEN, HD ;
SHAN, XW ;
MONTGOMERY, D .
PHYSICAL REVIEW A, 1990, 42 (10) :6158-6165
[5]  
COHEN RH, 1997, UCRLIK127002 LAWR LI
[6]   RESISTIVE FLUID TURBULENCE AND ENERGY CONFINEMENT [J].
CONNOR, JW ;
TAYLOR, JB .
PHYSICS OF FLUIDS, 1984, 27 (11) :2676-2681
[7]   Structure of the n=1 mode responsible for relaxation and current drive during sustainment of the SPHEX spheromak [J].
Duck, RC ;
Browning, PK ;
Cunningham, G ;
Gee, SJ ;
alKarkhy, A ;
Martin, R ;
Rusbridge, MG .
PLASMA PHYSICS AND CONTROLLED FUSION, 1997, 39 (05) :715-736
[8]   TEARING MODE INSTABILITY IN BESSEL FUNCTION MODEL [J].
GIBSON, RD ;
WHITEMAN, KJ .
PLASMA PHYSICS, 1968, 10 (12) :1101-&
[9]   The NIMROD code: a new approach to numerical plasma physics [J].
Glasser, AH ;
Sovinec, CR ;
Nebel, RA ;
Gianakon, TA ;
Plimpton, SJ ;
Chu, MS ;
Schnack, DD .
PLASMA PHYSICS AND CONTROLLED FUSION, 1999, 41 :A747-A755
[10]   Violating Suydam criterion produces feeble instabilities [J].
Gupta, S ;
Callen, JD ;
Hegna, CC .
PHYSICS OF PLASMAS, 2002, 9 (08) :3395-3401