Nonlinear stability and instability in collisionless trapped electron mode turbulence

2002 ◽  
Vol 9 (8) ◽  
pp. 3318-3332 ◽  
Author(s):  
D. A. Baver ◽  
P. W. Terry ◽  
R. Gatto ◽  
Eduardo Fernandez
2005 ◽  
Vol 12 (7) ◽  
pp. 072309 ◽  
Author(s):  
Tilman Dannert ◽  
Frank Jenko

Author(s):  
shuyu Zheng ◽  
Debing Zhang ◽  
Erbing Xue ◽  
Limin Yu ◽  
Xianmei Zhang ◽  
...  

Abstract High poloidal beta scenarios with favorable energy confinement (β_p~1.9, H_98y2~1.4) have been achieved on Experimental Advanced Superconducting Tokamak (EAST) using only radio frequency waves heating. Gyrokinetic simulations are carried out with experimental plasma parameters and tokamak equilibrium data of a typical high β_p discharge by the GTC code. Linear simulations show that electron temperature scale length and electron density scale length destabilize the turbulence, collision effects stabilize the turbulence, and the instability propagates in the electron diamagnetic direction. These indicate that the dominant instability in the core of high β_p plasma is collisionless trapped electron mode. Ion thermal diffusivities calculated by nonlinear gyrokinetic simulations are consistent with the experimental value, in which the electron collision effects play an important role. Further analyses show that instabilities with k_θ ρ_s>0.38 are suppressed by collision effects and collision effects reduce the radial correlation length of turbulence, resulting in the suppression of the turbulence.


2021 ◽  
Vol 31 (07) ◽  
pp. 2150105
Author(s):  
Yongjian Liu ◽  
Chunbiao Li ◽  
Aimin Liu

Little is known about bifurcations in two-dimensional (2D) differential systems from the viewpoint of Kosambi–Cartan–Chern (KCC) theory. Based on the KCC geometric invariants, three types of static bifurcations in 2D differential systems, i.e. saddle-node bifurcation, transcritical bifurcation, and pitchfork bifurcation, are discussed in this paper. The dynamics far from fixed points of the systems generating bifurcations are characterized by the deviation curvature and nonlinear connection. In the nonequilibrium region, the nonlinear stability of systems is not simple but involves alternation between stability and instability, even though systems are invariably Jacobi-unstable. The results also indicate that the dynamics in the nonequilibrium region are node-like for three typical static bifurcations.


2016 ◽  
Vol 23 (4) ◽  
pp. 042309 ◽  
Author(s):  
Lu Wang ◽  
Shuitao Peng ◽  
P. H. Diamond

Mathematics ◽  
2020 ◽  
Vol 8 (7) ◽  
pp. 1049
Author(s):  
Dongfen Bian

This paper is concerned with the nonlinear stability and instability of the two-dimensional (2D) Boussinesq-MHD equations around the equilibrium state ( u ¯ = 0 , B ¯ = 0 , θ ¯ = θ 0 ( y ) ) with the temperature-dependent fluid viscosity, thermal diffusivity and electrical conductivity in a channel. We prove that if a + ≥ a − , and d 2 d y 2 κ ( θ 0 ( y ) ) ≤ 0 or 0 < d 2 d y 2 κ ( θ 0 ( y ) ) ≤ β 0 , with β 0 > 0 small enough constant, and then this equilibrium state is nonlinearly asymptotically stable, and if a + < a − , this equilibrium state is nonlinearly unstable. Here, a + and a − are the values of the equilibrium temperature θ 0 ( y ) on the upper and lower boundary.


2014 ◽  
Vol 54 (4) ◽  
pp. 043006 ◽  
Author(s):  
S.F. Liu ◽  
S.C. Guo ◽  
W. Kong ◽  
J.Q. Dong

1976 ◽  
Vol 19 (4) ◽  
pp. 561 ◽  
Author(s):  
J. C. Adam ◽  
W. M. Tang ◽  
P. H. Rutherford

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