Avalanche transport of energetic-ions in magnetic confinement plasmas: Nonlinear multiple wave-number simulation

2021 ◽  
Author(s):  
Xiaolong Zhu ◽  
Wei Chen ◽  
Mario Podesta ◽  
Feng Wang ◽  
Deyong Liu ◽  
...  

Abstract Large burst activity, identified as toroidal Alfv\'{e}n eigenmode (TAE) avalanche, occurs frequently in neutral-beam heated plasmas in National Spherical Torus Experiment (NSTX). Based on the typical experimental observation of TAE avalanche on NSTX, a self-consistent nonlinear multiple wave-number ($k_{\parallel}\simeq n/R$, where $n$ toroidal mode-number and $R$ major radius) simulation associated with TAE avalanches is performed using the experimental parameters and profiles before the occurrence of TAE avalanche as the M3D-K input. The wave-wave nonlinear coupling among different modes and the resonant interaction between different modes and energetic-ions during TAE avalanches are identified in the nonlinear multiple wave-number simulations. The resonance overlap during the TAE avalanche is clearly observed in the simulation. It is found that the effective wave-wave coupling and a sufficiently strong drive are two important ingredients for the onset of TAE avalanches. TAE avalanche is considered to be a strongly nonlinear process and it is always accompanied by the simultaneous rapid frequency-chirping and large amplitude bursting of multiple modes and significant energetic-ion losses. The experimental phenomenon is observed on NSTX and is qualitatively reproduced by the simulation results in this work. These findings indicate that the onset of avalanche is triggered by nonlinearity of the system, and are also conducive to understanding the underlying mechanism of avalanche transport of energetic particles in the future burning plasmas, such as ITER.

1994 ◽  
Vol 73 (26) ◽  
pp. 3548-3551 ◽  
Author(s):  
M. Zharnikov ◽  
M. Weinelt ◽  
P. Zebisch ◽  
M. Stichler ◽  
H. -P. Steinrück

1994 ◽  
Vol 312 (1-2) ◽  
pp. 82-96 ◽  
Author(s):  
M. Zharnikov ◽  
D. Mehl ◽  
M. Weinelt ◽  
P. Zebisch ◽  
H.-P. Steinrück

2007 ◽  
Vol 122 (5) ◽  
pp. 3034
Author(s):  
Dalcio K. Dacol ◽  
Gregory J. Orris

2000 ◽  
Vol 18 (2) ◽  
pp. 183-187
Author(s):  
J.G. LOMINADZE

A new conception of subcritical transition to turbulence in unbounded smooth shear flows is discussed. According to this scenario, the transition to turbulence is caused by the interplay between the four basic phenomena: (a) linear “drift” of spatial Fourier harmonics (SFH) of disturbances in wave-number space (k-space); (b) transient growth of SFH; (c) viscous dissipation; (d) nonlinear process that closes a feedback loop of transition by angular redistribution of SFH in k-space; The key features of the concept are: transition to turbulence only by the finite amplitude vortex disturbances; anisotropy of the process in k-space; onset on chaos due to the dynamic (not stochastic) process. The evolution of 2D small-scale vortex disturbances in the parallel flows with uniform shear of velocity is analyzed in the framework of the weak turbulence approach. This numerical test analysis is carried out to prove the most problematic statement of the conception—existence of positive feedback caused by the nonlinear process (d). Numerical calculations also show the existence of a threshold: if amplitude of the initial disturbance exceeds the threshold value, the self maintenance of disturbances becomes realistic. The latter, in turn, is the characteristic feature of the flow transition to the turbulent state and its self maintenance.


2000 ◽  
Vol 64 (3) ◽  
pp. 235-247 ◽  
Author(s):  
I. BALLAI ◽  
R. ERDÉLYI ◽  
M. GOOSSENS

The theory of resonant nonlinear magnetohydrodynamic (MHD) waves in dissipative steady plasmas developed by Ballai and Erdélyi is used to study the effect of steady flows on nonlinear resonant heating of MHD waves in (a) linear, (b) weakly and (c) strongly nonlinear approximations. Nonlinear connection formulae for slow MHD waves are derived. This nonlinear theory of driven MHD waves is then used to study the interaction of sound waves with one-dimensional isotropic steady plasmas. We find that a steady equilibrium flow can significantly influence the efficiency of resonant absorption in the considered limits. In the case of strong nonlinearity, the efficiency of the resonant coupling is found to be proportional to the counterpart obtained in linear theory. The factor of proportion is approximately of the order of unity, justifying the commonly applied linear approximations.


2019 ◽  
Vol 59 (9) ◽  
pp. 096037
Author(s):  
W. Chen ◽  
X.L. Zhu ◽  
F. Wang ◽  
M. Jiang ◽  
X.Q. Ji ◽  
...  

1995 ◽  
Vol 334 (1-3) ◽  
pp. 114-134 ◽  
Author(s):  
M. Zharnikov ◽  
M. Weinelt ◽  
P. Zebisch ◽  
M. Stichler ◽  
H.-P. Steinrück

1977 ◽  
Vol 44 (4) ◽  
pp. 657-662 ◽  
Author(s):  
S. K. Datta

This paper deals with the scattering of plane longitudinal and shear waves by a distribution of elastic ellipsoidal inclusions. The scattered field is determined correct to O(ε3) where ε is a nondimensional wave number, assumed small. Assuming then that the distribution of scatterer centers is random homogeneous function of position and using a self-consistent (“quasi-crystalline”) approximation effective wave speeds are determined for the case of preferred orientation. Various limiting cases, viz., spherical inclusions and voids, elliptic and penny-shaped cracks, and fluid-filled cavities, are derived.


1990 ◽  
Vol 57 (4) ◽  
pp. 937-940 ◽  
Author(s):  
J. L. Nowinski

After a brief review of the main concepts of the nonlocal theory of elasticity, the equations of the nonlocal elastic moduli are derived, and the constitutive equations of the nonlocal medium established. Propagation of a longitudinal time-periodic wave normal to the laminae of the layered medium is then analyzed, and the equation of the wave dispersion determined. The dispersion originates from two sources: the configuration (discreteness) of the structure, and the nonlocal constitution of the material of the laminae. A numerical example accompanied by a graph illustrates the dependence of the effective wave velocity on the wave number in the entire Brillouin zone. It is found that for very short waves the wave velocity decreases to about 64 percent of its conventional value established for waves of long wavelength.


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