A non-modal analytical method to predict turbulent properties applied to the Hasegawa-Wakatani model

被引:9
作者
Friedman, B. [1 ,2 ]
Carter, T. A. [1 ]
机构
[1] Univ Calif Los Angeles, Dept Phys & Astron, Los Angeles, CA 90095 USA
[2] Lawrence Livermore Natl Lab, Livermore, CA 94550 USA
基金
美国国家科学基金会;
关键词
DRIFT-WAVE; STABILITY; INSTABILITY; TRANSITION;
D O I
10.1063/1.4905863
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
Linear eigenmode analysis often fails to describe turbulence in model systems that have non-normal linear operators and thus nonorthogonal eigenmodes, which can cause fluctuations to transiently grow faster than expected from eigenmode analysis. When combined with energetically conservative nonlinear mode mixing, transient growth can lead to sustained turbulence even in the absence of eigenmode instability. Since linear operators ultimately provide the turbulent fluctuations with energy, it is useful to define a growth rate that takes into account non-modal effects, allowing for prediction of energy injection, transport levels, and possibly even turbulent onset in the subcritical regime. We define such a non-modal growth rate using a relatively simple model of the statistical effect that the nonlinearities have on cross-phases and amplitude ratios of the system state variables. In particular, we model the nonlinearities as delta-function-like, periodic forces that randomize the state variables once every eddy turnover time. Furthermore, we estimate the eddy turnover time to be the inverse of the least stable eigenmode frequency or growth rate, which allows for prediction without nonlinear numerical simulation. We test this procedure on the 2D and 3D Hasegawa-Wakatani model [A. Hasegawa and M. Wakatani, Phys. Rev. Lett. 50, 682 (1983)] and find that the non-modal growth rate is a good predictor of energy injection rates, especially in the strongly non-normal, fully developed turbulence regime. (C) 2015 AIP Publishing LLC.
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页数:10
相关论文
共 38 条
[31]   The nonlinear drift wave instability and its role in tokamak edge turbulence [J].
Scott, BD .
NEW JOURNAL OF PHYSICS, 2002, 4 :52.1-52.30
[32]   SELF-SUSTAINED COLLISIONAL DRIFT-WAVE TURBULENCE IN A SHEARED MAGNETIC-FIELD [J].
SCOTT, BD .
PHYSICAL REVIEW LETTERS, 1990, 65 (26) :3289-3292
[33]   Role of stable eigenmodes in saturated local plasma turbulence [J].
Terry, PW ;
Baver, DA ;
Gupta, S .
PHYSICS OF PLASMAS, 2006, 13 (02)
[34]   HYDRODYNAMIC STABILITY WITHOUT EIGENVALUES [J].
TREFETHEN, LN ;
TREFETHEN, AE ;
REDDY, SC ;
DRISCOLL, TA .
SCIENCE, 1993, 261 (5121) :578-584
[35]  
Trefethen LN., 2005, Spectra and pseudospectra: the behavior of nonnormal matrices and operators, DOI 10.1515/9780691213101
[36]   Numerical simulation and analysis of plasma turbulence the Large Plasma Device [J].
Umansky, M. V. ;
Popovich, P. ;
Carter, T. A. ;
Friedman, B. ;
Nevins, W. M. .
PHYSICS OF PLASMAS, 2011, 18 (05)
[37]   TRANSITION IN SHEAR FLOWS - NONLINEAR NORMALITY VERSUS NONNORMAL LINEARITY [J].
WALEFFE, F .
PHYSICS OF FLUIDS, 1995, 7 (12) :3060-3066
[38]   SUBCRITICAL MAGNETOHYDRODYNAMIC TURBULENCE [J].
WALTZ, RE .
PHYSICAL REVIEW LETTERS, 1985, 55 (10) :1098-1101