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Nonlinear {omega}*-stabilization of the m = 1 mode in tokamaks
Author(s) -
B. N. Rogers,
L. Zakharov
Publication year - 1995
Publication title -
osti oai (u.s. department of energy office of scientific and technical information)
Language(s) - English
Resource type - Reports
DOI - 10.2172/100284
Subject(s) - sawtooth wave , tokamak , physics , magnetohydrodynamic drive , omega , nonlinear system , instability , magnetohydrodynamics , plasma , mode (computer interface) , amplitude , marginal stability , linear stability , atomic physics , quantum electrodynamics , mechanics , quantum mechanics , computer science , computer vision , operating system
Earlier studies of sawtooth oscillations in Tokamak Fusion Test Reactor supershots (Levinton et al, Phys. Rev. Lett. 72, 2895 (1994); Zakharov, et al, Plasma Phys. and Contr. Nucl. Fus. Res., Proc. 15th Int. Conf., Seville 1994, Vienna) have found an apparent contradiction between conventional linear theory and experiment: even in sawtooth-free discharges, the theory typically predicts instability due to a nearly ideal m = 1 mode. Here, the nonlinear evolution of such mode is analyzed using numerical simulations of a two-fluid magnetohydrodynamic (MHD) model. We find the mode saturates nonlinearly at a small amplitude provided the ion and electron drift-frequencies {omega}*{sub i,e} are somewhat above the linear stability threshold of the collisionless m = 1 reconnecting mode. The comparison of the simulation results to m = 1 mode activity in TFTR suggests additional, stabilizing effects outside the present model are also important

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