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Tokamak-edge toroidal rotation due to inhomogeneous transport and geodesic curvature
Author(s) -
T. Stoltzfus-Dueck
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 - 10.1063/1.4718335
Subject(s) - physics , pedestal , toroid , rotation (mathematics) , current (fluid) , atomic physics , ion , tokamak , momentum diffusion , plasma , turbulence , neutral beam injection , mechanics , geometry , nuclear physics , mathematics , archaeology , quantum mechanics , history , thermodynamics
In a model kinetic ion transport equation for the pedestal and scrape-off layer, passing-ion drift orbit excursions interact with spatially inhomogeneous but purely diffusive transport to cause the orbit-averaged diffusivities to depend on the sign of ν∥, preferentially transporting counter-current ions for realistic parameter values. The resulting pedestal-top intrinsic rotation is typically co-current, reaches experimentally relevant values, and is proportional to pedestal-top ion temperature Ti|pt over plasma current Ip, as observed in experiment. The rotation drive is independent of the toroidal velocity and its radial gradient, representing a residual stress. Co-current spin-up at the L-H transition is expected due to increasing Ti|pt and a steepening of the turbulence intensity gradient. A more inboard (outboard) X-point leads to additional co- (counter-) current rotation drive. Beyond intrinsic rotation, comparison of heat and momentum transport reveals that neutral beam injection must be significa...

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