Gyrokinetic turbulent heating
Abstract
Expressions for particle and energy fluxes and heating rates due to turbulence are derived. These fluxes and heating rates are identified from moments of an extended driftkinetic equation for the equilibrium distribution function. These include neoclassical as well as turbulent diffusion and heating. Phasespace conservation is demonstrated, allowing the driftkinetic equation to be expressed in conservative form. This facilitates taking moments with few approximations, mainly those consistent with drift kinetics for the equilibrium distribution function and the relative smallness of the fluctuations. The turbulent heating is uniquely defined by choosing the standard gyrokinetic definition for the energy flux. With this definition, most of the heating can be expressed in the form of ohmic heating from turbulent parallel and perpendicular current density perturbations. The latter current is identified with gradB and curvature drifts, plus terms involving magnetic perturbations (which are smaller for low beta). A small contribution to the heating comes from the divergence of an energy flux that is dependent on the finite gyroradius of the ions. The fluxes and heating rates are expressed in a form that can be easily evaluated from gyrokinetic turbulence simulations.
 Authors:
 General Atomics, P.O. Box 85608, San Diego, California 921865608 (United States)
 Publication Date:
 OSTI Identifier:
 20860292
 Resource Type:
 Journal Article
 Resource Relation:
 Journal Name: Physics of Plasmas; Journal Volume: 13; Journal Issue: 10; Other Information: DOI: 10.1063/1.2345179; (c) 2006 American Institute of Physics; Country of input: International Atomic Energy Agency (IAEA)
 Country of Publication:
 United States
 Language:
 English
 Subject:
 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; APPROXIMATIONS; CURRENT DENSITY; DISTRIBUTION FUNCTIONS; DISTURBANCES; ELECTRIC CURRENTS; EQUILIBRIUM; FLUCTUATIONS; HEATING RATE; IONS; KINETIC EQUATIONS; KINETICS; NEOCLASSICAL TRANSPORT THEORY; PHASE SPACE; PLASMA; PLASMA SIMULATION; RADIATION TRANSPORT; TURBULENCE; TURBULENT HEATING
Citation Formats
Hinton, F. L., and Waltz, R. E. Gyrokinetic turbulent heating. United States: N. p., 2006.
Web. doi:10.1063/1.2345179.
Hinton, F. L., & Waltz, R. E. Gyrokinetic turbulent heating. United States. doi:10.1063/1.2345179.
Hinton, F. L., and Waltz, R. E. 2006.
"Gyrokinetic turbulent heating". United States.
doi:10.1063/1.2345179.
@article{osti_20860292,
title = {Gyrokinetic turbulent heating},
author = {Hinton, F. L. and Waltz, R. E.},
abstractNote = {Expressions for particle and energy fluxes and heating rates due to turbulence are derived. These fluxes and heating rates are identified from moments of an extended driftkinetic equation for the equilibrium distribution function. These include neoclassical as well as turbulent diffusion and heating. Phasespace conservation is demonstrated, allowing the driftkinetic equation to be expressed in conservative form. This facilitates taking moments with few approximations, mainly those consistent with drift kinetics for the equilibrium distribution function and the relative smallness of the fluctuations. The turbulent heating is uniquely defined by choosing the standard gyrokinetic definition for the energy flux. With this definition, most of the heating can be expressed in the form of ohmic heating from turbulent parallel and perpendicular current density perturbations. The latter current is identified with gradB and curvature drifts, plus terms involving magnetic perturbations (which are smaller for low beta). A small contribution to the heating comes from the divergence of an energy flux that is dependent on the finite gyroradius of the ions. The fluxes and heating rates are expressed in a form that can be easily evaluated from gyrokinetic turbulence simulations.},
doi = {10.1063/1.2345179},
journal = {Physics of Plasmas},
number = 10,
volume = 13,
place = {United States},
year = 2006,
month =
}

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