Metastability of stratified magnetohydrostatic equilibria and their relaxation

被引:0
|
作者
Hosking, D. N. [1 ,2 ]
Wasserman, D. [3 ]
Cowley, S. C. [4 ]
机构
[1] Princeton Ctr Theoret Sci, Princeton, NJ 08540 USA
[2] Gonville & Caius Coll, Trinity St, Cambridge CB2 1TA, England
[3] Northeastern Univ, Boston, MA 02115 USA
[4] Princeton Plasma Phys Lab, Princeton, NJ 08540 USA
关键词
plasma nonlinear phenomena; plasma instabilities; POTENTIAL-ENERGY STATE; STATISTICAL-MECHANICS; BUOYANCY INSTABILITIES; STABILITY; ASSIGNMENT; EQUATION;
D O I
10.1017/S0022377824001521
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
Motivated by explosive releases of energy in fusion, space and astrophysical plasmas, we consider the nonlinear stability of stratified magnetohydrodynamic equilibria against two-dimensional interchanges of straight magnetic-flux tubes. We demonstrate that, even within this restricted class of dynamics, the linear stability of an equilibrium does not guarantee its nonlinear stability: equilibria can be metastable. We show that the minimum-energy state accessible to a metastable equilibrium under non-diffusive two-dimensional dynamics can be found by solving a combinatorial optimisation problem. These minimum-energy states are, to good approximation, the final states reached by our simulations of destabilised metastable equilibria for which turbulent mixing is suppressed by viscosity. To predict the result of fully turbulent relaxation, we construct a statistical mechanical theory based on the maximisation of Boltzmann's mixing entropy. This theory is analogous to the Lynden-Bell statistical mechanics of collisionless stellar systems and plasma, and to the Robert-Sommeria-Miller theory of two-dimensional vortex turbulence. Our theory reproduces well the results of our numerical simulations for sufficiently large perturbations to the metastable equilibrium.
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页数:68
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