Global gyrokinetic ion temperature gradient turbulence simulations of ITER

被引:24
|
作者
Villard, L. [1 ]
Angelino, P. [1 ]
Bottino, A. [2 ]
Brunner, S. [1 ]
Jolliet, S. [1 ]
McMillan, B. F. [3 ]
Tran, T. M. [1 ]
Vernay, T. [1 ]
机构
[1] Ecole Polytech Fed Lausanne, Ctr Rech Phys Plasmas, Assoc Euratom Switzerland, CH-1015 Lausanne, Switzerland
[2] Max Planck Inst Plasma Phys, EURATOM Assoc, Garching, Germany
[3] Univ Warwick, Ctr Fus Space & Astrophys, Warwick, England
关键词
D O I
10.1088/0741-3335/55/7/074017
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
Global gyrokinetic simulations of ion temperature gradient (ITG) driven turbulence in an ideal MHD ITER equilibrium plasma are performed with the ORB5 code. The noise control and field-aligned Fourier filtering procedures implemented in ORB5 are essential in obtaining numerically healthy results with a reasonable amount of computational effort: typical simulations require 10(9) grid points, 10(9) particles and, despite a particle per cell ratio of unity, achieve a signal to noise ratio larger than 50. As compared with a circular concentric configuration with otherwise similar parameters (same rho* = 1/720), the effective heat diffusivity is considerably reduced for the ITER MHD equilibrium. A self-organized radial structure appears, with long-lived zonal flows (ZF), modulating turbulence heat transport and resulting in a corrugated temperature gradient profile. The ratio of long-lived ZF to the fluctuating ZF is markedly higher for the ITER MHD equilibrium as compared with circular configurations, thereby producing a more effective ITG turbulence suppression, in spite of a higher linear growth rate. As a result, the nonlinear critical temperature gradient, R/L-Tcrit, (NL), is about twice the linear critical temperature gradient, R/L-Tcrit,L-lin. Moreover, the heat transport stiffness above the nonlinear threshold is considerably reduced as compared with circular cases. Plasma elongation is probably one of the essential causes of this behaviour: indeed, undamped ZF residual levels and geodesic acoustic mode damping are both increasing with elongation. Other possible causes of the difference, such as magnetic shear profile effects, are also investigated.
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页数:8
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