Validation of single-fluid and two-fluid magnetohydrodynamic models of the helicity injected torus spheromak experiment with the NIMROD code

被引:13
作者
Akcay, Cihan [1 ]
Kim, Charlson C. [2 ]
Victor, Brian S. [1 ]
Jarboe, Thomas R. [1 ]
机构
[1] Univ Washington, Seattle, WA 98195 USA
[2] FAR TECH Inc, San Diego, CA 92121 USA
关键词
EQUILIBRIA; RELAXATION; PLASMA; DRIVE;
D O I
10.1063/1.4817951
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
We present a comparison study of 3-D pressureless resistive MHD (rMHD) and 3-D presureless two-fluid MHD models of the Helicity Injected Torus with Steady Inductive helicity injection (HIT-SI). HIT-SI is a current drive experiment that uses two geometrically asymmetric helicity injectors to generate and sustain toroidal plasmas. The comparable size of the collisionless ion skin depth d(i) to the resistive skin depth predicates the importance of the Hall term for HIT-SI. The simulations are run with NIMROD, an initial-value, 3-D extended MHD code. The modeled plasma density and temperature are assumed uniform and constant. The helicity injectors are modeled as oscillating normal magnetic and parallel electric field boundary conditions. The simulations use parameters that closely match those of the experiment. The simulation output is compared to the formation time, plasma current, and internal and surface magnetic fields. Results of the study indicate 2fl-MHD shows quantitative agreement with the experiment while rMHD only captures the qualitative features. The validity of each model is assessed based on how accurately it reproduces the global quantities as well as the temporal and spatial dependence of the measured magnetic fields. 2fl-MHD produces the current amplification I-tor/I-inj and formation time tau(f) demonstrated by HIT-SI with similar internal magnetic fields. rMHD underestimates I-tor/I-inj and exhibits much a longer tau(f). Biorthogonal decomposition (BD), a powerful mathematical tool for reducing large data sets, is employed to quantify how well the simulations reproduce the measured surface magnetic fields without resorting to a probe-by-probe comparison. BD shows that 2fl-MHD captures the dominant surface magnetic structures and the temporal behavior of these features better than rMHD. (C) 2013 AIP Publishing LLC.
引用
收藏
页数:18
相关论文
共 43 条
[1]   SPATIOTEMPORAL ANALYSIS OF COMPLEX SIGNALS - THEORY AND APPLICATIONS [J].
AUBRY, N ;
GUYONNET, R ;
LIMA, R .
JOURNAL OF STATISTICAL PHYSICS, 1991, 64 (3-4) :683-739
[2]  
Bellan P M., 2008, Fundamentals of Plasma Physics, DOI [10.1017/CBO9780511807183, DOI 10.1017/CBO9780511807183]
[3]   REVERSED-FIELD-PINCH RESEARCH [J].
BODIN, HAB ;
NEWTON, AA .
NUCLEAR FUSION, 1980, 20 (10) :1255-1324
[4]  
Braginskii S. I., 1965, REV PLASMA PHYS, V1
[5]  
Braginskii S. I., 1965, REV PLASMA PHYS, V1
[6]   The role of the nφ=1 column mode in spheromak formation [J].
Cohen, B. I. ;
Romero-Talamas, C. A. ;
Ryutov, D. D. ;
Hooper, E. B. ;
LoDestro, L. L. ;
McLean, H. S. ;
Stewart, T. L. ;
Wood, R. D. .
PHYSICS OF PLASMAS, 2009, 16 (04)
[7]  
DEWIT TD, 1994, PHYS PLASMAS, V1, P3288, DOI 10.1063/1.870481
[8]   The three-dimensional magnetohydrodynamics of ac helicity injection in the reversed field pinch [J].
Ebrahimi, F ;
Prager, SC ;
Sarff, JS ;
Wright, JC .
PHYSICS OF PLASMAS, 2003, 10 (04) :999-1014
[9]  
Ennis D. A., 2010, Nuclear Fusion, V50, DOI 10.1088/0029-5515/50/7/072001
[10]   Three-dimensional reconnection and relaxation of merging spheromak plasmas [J].
Gray, T. ;
Brown, M. R. ;
Cothran, C. D. ;
Lukin, V. S. .
PHYSICS OF PLASMAS, 2010, 17 (10)