Three-dimensional numerical simulations of the relaxation process in spheromak plasmas
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
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MAGNETIC FLUX
NUMERICAL ANALYSIS
SIMULATION
THREE-DIMENSIONAL CALCULATIONS
TOROIDAL CONFIGURATION
ANNULAR SPACE
CLOSED PLASMA DEVICES
CONFIGURATION
CONFINEMENT
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INSTABILITY
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TOKAMAK DEVICES
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