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Theory of dissipative density-gradient-driven turbulence in the tokamak edge

Journal Article · · Phys. Fluids; (United States)
DOI:https://doi.org/10.1063/1.864977· OSTI ID:5882901
A theory of resistive, density-gradient-driven turbulence is presented and compared with tokamak edge fluctuation measurements. In addition to linear driving, the theory accounts for relaxation of the density gradient through a nonlinear process associated with emission from localized density fluctuation elements. From a fluid model for isothermal electrons in toroidal geometry, equations are obtained and solved analytically, retaining both coherent and incoherent contributions. The effect of collisions on the density blobs is treated. A Reynolds number parameterizes the magnitude of the turbulent scattering relative to the collisional viscous diffusion. The analytic results indicate that the spectrum is characterized by linewidths which increase as a function of the Reynolds number and may reach ..delta omega../..omega..> or approx. =1. Energy lies predominantly in the small wavenumbers (k/sub perpendicular/ rho/sub s/approx.0.1). For larger wavenumbers and frequency, the spectrum decays as k/sup -17/6/ and ..omega../sup -2/. The fluctuation level scales as 1/k/sub perpendicular/L/sub n/ and may reach -30% for parameters typical of the pretext edge. Particle diffusion is Bohm-like in magnitude but does not follow Bohm scaling, going instead as n/sup 2//sup ///sup 3/T/sup 1/6//sub e/. The density fluctuations exhibit nonadiabatic character caused by the incoherent mode coupling. An expression for the departure from adiabaticity is given.
Research Organization:
Institute for Fusion Studies, University of Texas at Austin, Austin, Texas 78712
DOE Contract Number:
FG05-80ET53088
OSTI ID:
5882901
Journal Information:
Phys. Fluids; (United States), Journal Name: Phys. Fluids; (United States) Vol. 28:5; ISSN PFLDA
Country of Publication:
United States
Language:
English