Physics of Plasmas
   
 
 
 
Previous Article
Stability of negative central magnetic shear discharges in the DIII-D tokamak
Discharges with negative central magnetic shear (NCS) hold the promise of enhanced fusion performance in advanced tokamaks. However, stability to long wavelength magnetohydrodynamic modes is needed to...
Next Article
Observation of multiple mechanisms for stimulating ion waves in ignition scale plasmas
The laser and plasma conditions expected in ignition experiments using indirect drive inertial confinement have been studied experimentally. It has been shown that there are at least three ways in whi...

Gyrofluid simulations of turbulence suppression in reversed-shear experiments on the Tokamak Fusion Test Reactor

Phys. Plasmas 4, 1792 (1997); doi:10.1063/1.872279

Issue Date: May 1997

You are not logged in to this journal. Log in

M. A. Beer, G. W. Hammett, G. Rewoldt, E. J. Synakowski, and M. C. Zarnstorff
Princeton University Plasma Physics Laboratory, Princeton, New Jersey 08543

W. Dorland
Institute for Fusion Studies, Austin, Texas 78712-1060
The confinement improvement in reversed-shear experiments on the Tokamak Fusion Test Reactor [Plasma Phys. Controlled Fusion 26, 11 (1984)] is investigated using nonlinear gyrofluid simulations including a bounce-averaged trapped electron fluid model. This model includes important kinetic effects for both ions and electrons, and agrees well with linear kinetic theory. Both reversed shear and the Shafranov shift reverse the precession drifts of a large fraction of the trapped electrons, which significantly reduces the growth rate of the trapped electron mode, found to be the dominant instability in the core. Two positive feedback transition mechanisms for the sudden improvement in core confinement are discussed: (1) Shafranov shift suppression of the trapped electron mode, and (2) turbulence suppression by radially sheared E × B flows. While both effects appear to be playing roles in the transition dynamics in most experiments, we show that Shafranov shift stabilization alone can cause a transition. ©1997 American Institute of Physics.
History: Received 15 November 1996; accepted 5 February 1997
Permalink: http://link.aip.org/link/?PHPAEN/4/1792/1
BUY THIS ARTICLE   (US$28)
Download PDF (295 kB) View Cart

KEYWORDS and PACS

Keywords
PACS
  • 52.35.Ra
    Physics of plasmas and electric discharges Waves, oscillations, and instabilities in plasma Plasma turbulence
  • 52.55.Fa
    Physics of plasmas and electric discharges Magnetic confinement and equilibrium Tokamaks
  • 52.65.Kj
    Physics of plasmas and electric discharges Plasma simulation Magnetohydrodynamic and fluid equation
  • 52.25.Dg
    Physics of plasmas and electric discharges Plasma properties Plasma kinetic equations
  • YEAR: 1996-97

RELATED DATABASES


To view database links for this article,
you need to log in.
To view database links for this article,
you need to log in.

PUBLICATION DATA

ISSN:
1070-664X (print)   1089-7674 (online)
Publisher:
AIP is a member of CrossRef AIP

There are no references.

CITING ARTICLES

For access to citing articles, you need to log in.
For access to citing articles, you need to Log in.