Ohmic energy confinement saturation and core toroidal rotation reversal in Alcator C-Mod plasmas
Author(s) -
J. E. Rice,
M. Greenwald,
Y. Podpaly,
M.L. Reinke,
P. H. Diamond,
J. W. Hughes,
N. T. Howard,
Y. Ma,
I. Cziegler,
B.P. Duval,
P. Ennever,
D. R. Ernst,
C. L. Fiore,
C. Gao,
J. Irby,
E. S. Marmar,
M. Porkoláb,
N. Tsujii,
S. Wolfe
Publication year - 2012
Publication title -
physics of plasmas
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.75
H-Index - 160
eISSN - 1089-7674
pISSN - 1070-664X
DOI - 10.1063/1.3695213
Subject(s) - alcator c mod , physics , collisionality , toroid , ohmic contact , plasma , tokamak , saturation (graph theory) , rotation (mathematics) , joule heating , condensed matter physics , magnetic confinement fusion , current density , atomic physics , magnetohydrodynamics , nuclear physics , geometry , quantum mechanics , mathematics , electrode , combinatorics
Ohmic energy confinement saturation is found to be closely related to core toroidal rotation reversals in Alcator C-Mod tokamak plasmas. Rotation reversals occur at a critical density, depending on the plasma current and toroidal magnetic field, which coincides with the density separating the linear Ohmic confinement regime from the saturated Ohmic confinement regime. The rotation is directed co-current at low density and abruptly changes direction to counter-current when the energy confinement saturates as the density is increased. Since there is a bifurcation in the direction of the rotation at this critical density, toroidal rotation reversal is a very sensitive indicator in the determination of the regime change. The reversal and confinement saturation results can be unified, since these processes occur in a particular range of the collisionality.United States. Dept. of Energy (Contract DE-FC02-99ER54512
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