Density limit disruptions in tokamaks

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Abstract

Magnetohydrodynamic simulations are presented which reproduce the rapid drop in the central temperature observed during density limit disruptions in tokamaks. The loss of central confinement is triggered by edge radiation which destabilizes a q = 1 kink mode. A bubble of cold plasma is injected from the edge into the center by the q = 1 kink. This bubble bears a striking resemblance to the cold plasma that is observed to move from the edge into the center during density limit disruptions on the JET tokamak [Plasma Physics and Controlled Nuclear Fusion Research 1986 (IAEA, Vienna, 1987), Vol. 1, p. 433], initiating the loss of central confinement. The bubble profile produced by the q = 1 kink is unstable to a broad spectrum of modes which progressively reduce the magnetic shear between the q = 2 surface and the center. The q = 2 mode then grows across the center, broadening the current and throwing the hot plasma to the wall. © 1991 American Institute of Physics.

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APA

Kleva, R. G., & Drake, J. F. (1991). Density limit disruptions in tokamaks. Physics of Fluids B, 3(2), 372–383. https://doi.org/10.1063/1.859747

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