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Title: Three-dimensional numerical simulations of the relaxation process in spheromak plasmas

Journal Article · · Phys. Fluids; (United States)
DOI:https://doi.org/10.1063/1.865621· OSTI ID:5705965

Nonlinear evolution of three-dimensional magnetohydrodynamic (MHD) instabilities of a toroidal spheromak in a cylindrical flux conserver has been studied by numerical simulations for various initial equilibrium states with different q profiles. In spheromaks with q/sub a/>1, where q/sub a/ is the safety factor on the magnetic axis, nonlinear evolution of the resonant internal kink mode dominates with a poloidal mode number m = 1 and a toroidal mode number n = 1 that causes the poloidal flux amplification. This process corresponds to that of the internal disruption model for tokamaks by Kadomtsev (Sov. J. Plasma Phys. 1, 389 (1975)). In spheromaks with a very high q/sub a/, namely q/sub a/> or approx. =3, the gross n = 1 kink mode grows extensively in the region including the major axis of the torus, which causes the flux conversion from the toroidal to poloidal directions. For spheromaks with a low q/sub a/, namely q/sub a/< or approx. =0.5, the internal kink mode with a toroidal mode number napprox.1/q/sub a/ is first destabilized, and the excitation of the modes with lower n numbers down to n = 1 proceeds, while the n = 2 mode saturates. Nonlinear coupling of various modes leads to the flux conversion from the poloidal to toroidal directions. When a center conductor is present in this case, a reversed-field pinch (RFP) configuration once formed is sustained. Relaxations through pressure-driven modes are also discussed. All final states obtained in our simulations are quite near the Taylor state with an excess magnetic energy less than 10% of that of the Taylor state.

Research Organization:
Department of Electronic Engineering, University of Tokyo, Tokyo 113, Japan
OSTI ID:
5705965
Journal Information:
Phys. Fluids; (United States), Vol. 29:6
Country of Publication:
United States
Language:
English