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Nonlinear tearing modes in the reversed field pinch

Journal Article · · Phys Fluids B; (United States)
DOI:https://doi.org/10.1063/1.859151· OSTI ID:6547914
Finite-amplitude islands, which are the saturated states of tearing modes in the reversed field pinch, are calculated. These states are bifurcated noncylindrical equilibrium states. With sigma(r) (sigmaequivalentj x B/B/sup 2/) nonuniform across the plasma, as is consistent with experiment, a variety of m = 1 and m = 0 bifurcated equilibria are possible, instead of just the m = 1 helix calculated for uniform sigma(r) by Taylor (in Pulsed High Beta Plasmas, edited by D. Evans (Pergamon, Oxford, 1976), p. 59). Assuming the magnetic field lines in the reversed field pinch are weakly stochastic, the growth time of an unstable tearing mode is on the inertial time scale, as in the Taylor model, in constrast to growth on the resistive time scale predicted from nonlinear tearing mode theory when magnetic surfaces exist. The dependence of the saturated island width on radius of a conducting shell is investigated. Islands in the reversed field pinch often have magnetic wells in the island interior, which may result in improved confinement in the island regions.
Research Organization:
Los Alamos National Laboratory, Los Alamos, New Mexico 87545
OSTI ID:
6547914
Journal Information:
Phys Fluids B; (United States), Journal Name: Phys Fluids B; (United States) Vol. 1:2; ISSN PFBPE
Country of Publication:
United States
Language:
English