Published October 2010 | Version v1
Report

Turbulent Generation of Flows and Magnetic Field at the Rational Magnetic Surfaces of a Tokamak

  • 1. Russian Research Center 'Kurchatov Institute', 1 Kurchatov Sq., Moscow 123182 (Russian Federation)
  • 2. Peoples' Friendship University of Russia, 3 Ordzhonikidze Str., Moscow 117198 (Russian Federation)
  • 3. University of California at San-Diego, 9500 Gilman Drive, La Jolla, CA 92093 (United States)
  • 4. University of Saskatchewan, 116 Science Place, Saskatoon, S7N 5E2 (Canada)

Description

Full text: Comparative analysis of generation of large-scale structures, zonal flows and streamers, by drift wave turbulence is conducted for periodic systems with magnetic shear such as a tokamak. In a strong magnetic field dynamics of quasi two-dimensional perturbations strongly depends on the value of the wave vector along the magnetic field. When the parallel wave vector is significantly large, so that the parallel phase velocity of perturbation is small compared to electron thermal velocity, the parallel electron motion results in a finite electron density perturbation. It follows the Boltzmann distribution. However, for large-scale structures with poloidal and toroidal symmetry m = n = 0, and the parallel wave vector is zero. This results in strong reduction of density perturbation for m = n = 0. This difference has profound consequences for generation of large-scale zonal flows and streamers due to different structure of the nonlinear interaction matrix. The interaction term has a structure similar to the standard convective nonlinearity for zonal flows, while for streamers it has the structure of the Hasegawa-Mima nonlinearity (which is the higher order due to a small parameter associated with a finite ion Larmor radius). Respectively, zonal flows have the larger growth rate gamma(ZF) compared to that of the streamers. It is shown that 3D electromagnetic helical perturbations will have the growth rate comparable to that of zonal flows if their symmetry coincides with the symmetry of rational magnetic surface, m = nq. The field line bending provides a stabilizing effect and thus determines the radial localization of such structures. Therefore, it is expected that three-dimensional structures of flows and magnetic field will be preferentially generated at the rational magnetic surfaces of a tokamak with a growth rate of order gamma(ZF). This theoretical result may corroborate existing experimental correlations of large-scale shear flow structures with rational magnetic surfaces of a tokamak. (author)

Part of:
23. IAEA Fusion Energy Conference. Book of Abstracts

Additional details

Publishing Information

Imprint Title
23. IAEA Fusion Energy Conference. Book of Abstracts
Imprint Pagination
637 p.
Journal Page Range
p. 352
Report number
IAEA-CN--180

Conference

Title
23. IAEA Fusion Energy Conference
Acronym
FEC 2010
Dates
11-16 Oct 2010
Place
Daejeon (Korea, Republic of)

INIS

Country of Publication
International Atomic Energy Agency (IAEA)
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
43041070
Subject category
S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
Resource subtype / Literary indicator
Conference
Descriptors DEI
DISTURBANCES; ELECTRON DENSITY; IONS; LARMOR RADIUS; MAGNETIC FIELDS; MAGNETIC SURFACES; NONLINEAR PROBLEMS; PHASE VELOCITY; TOKAMAK DEVICES
Descriptors DEC
CHARGED PARTICLES; CLOSED PLASMA DEVICES; MAGNETIC FIELD CONFIGURATIONS; THERMONUCLEAR DEVICES; VELOCITY

Optional Information

Secondary number(s)
THS--P8-02