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Nonlinear growth of marginally unstable tearing modes

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.2722306· OSTI ID:20974972
 [1]
  1. Associacao Euratom/IST, Centro de Fusao Nuclear, 1049-001 Lisbon (Portugal)
In this work, the nonlinear growth of the classical tearing mode is revisited, using reduced magnetohydrodynamic numerical simulations in cylindrical geometry, emphasizing the limiting scenario of a marginally unstable mode, i.e., 0{approx}{delta}{sup '}a<4, where a is the minor radius and {delta}{sup '} is the stability parameter [H. Furth, J. Killeen, and M. N. Rosenbluth, Phys. Fluids 6, 459 (1963)]. Conventionally, the mode becomes unstable when {delta}{sup '}>0 and, eventually, a steady state island width (saturated island width) is achieved. It is found that, contrary to theoretical predictions, no steady state solution is obtained for typically low temperature plasmas with perpendicular viscosity and magnetic Reynolds number below a certain threshold. Plasma inertial forces are identified as the physical mechanism behind such nonlinear evolution.
OSTI ID:
20974972
Journal Information:
Physics of Plasmas, Journal Name: Physics of Plasmas Journal Issue: 5 Vol. 14; ISSN PHPAEN; ISSN 1070-664X
Country of Publication:
United States
Language:
English

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