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Title: Neoclassical quasilinear transport theory of fluctuations in toroidal plasmas: Further considerations

Journal Article · · Physics of Fluids B; (USA)
DOI:https://doi.org/10.1063/1.859576· OSTI ID:6962950
 [1]
  1. Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831 (USA)

The effects of the radial electric field {ital E}{sub {ital r}} on fluctuation-induced transport fluxes and the fluctuation spectrum in toroidal plasmas are further studied to clarify the ideas originally developed in an earlier paper (Phys. Fluids {bold 31}, 2249 (1988)). A specific tokamak example is employed in the discussion. It is found that even in the presence of fluctuations, the parallel flow in tokamaks is damped by the neoclassical viscosity on a time scale of the order of {nu}{sub {ital ii}}{sup {minus}1}, with {nu}{sub {ital ii}} the collision frequency. The toroidal flow is damped by the anomalous ion viscosity on a time scale of the order of the confinement time. The radial electric field always has an effect on the fluctuation spectrum and fluctuation-induced transport fluxes in tokamaks except when {ital d}({ital E}{sub {ital r}}q/{ital r})/{ital dr}=0 (where {ital q} is the safety factor and {ital r} is the minor radius) if the radial dependence of the toroidal magnetic field is neglected by considering the invariant property of the drift kinetic equation when there is a change in {ital E}{sub {ital r}}. The condition implies the rigid-body toroidal rotation associated with {bold E}{times}{bold B} drift, with {bold E} ({bold B}) the electric (magnetic) field. The fact that the fluctuation-induced transport fluxes can depend on {ital E}{sub {ital r}} through the fluctuation spectrum and the thermodynamic force does not contradict their intrinsic ambipolarity property. The results are shown to be invariant under Galilean transformation.

DOE Contract Number:
AC05-84OR21400
OSTI ID:
6962950
Journal Information:
Physics of Fluids B; (USA), Vol. 2:4; ISSN 0899-8221
Country of Publication:
United States
Language:
English