Parametric dependence of the edge radial electric field in the DIII-D tokamak

High spatially resolved measurements of the radial electric field, Er, have been made across the transition from L mode to H mode plasmas for many different plasma parameters and conditions. The evolution of the well-like structure of the Er profile formed at the L-H transition has been investigated. No distinct variation in the shape or width of the Er well at the L-H transition is observed as a function of the plasma parameters investigated, such as the plasma current, the toroidal magnetic field and the plasma density. The value of Er is negative just inside the last closed flux surface (LCFS) for all the plasmas studied. There is a variation in the depth of the Er well for different conditions. The experimental results have been compared with theoretical predictions for suppression of plasma turbulence by sheared E × B plasma flow.

[1]  K. H. Burrell,et al.  Effects of E×B velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices , 1997 .

[2]  S. Coda,et al.  Constraints on theories provided by fast time response measurements across the L to H transition on DIII-D , 1996 .

[3]  S. Sen,et al.  Theory of drift waves in the presence of parallel and perpendicular flow curvature. I. Slab model , 1996 .

[4]  E. Doyle,et al.  Microturbulence reduction during counter neutral beam injection in the DIII-D tokamak , 1996 .

[5]  S. Coda,et al.  Beyond paradigm: Turbulence, transport, and the origin of the radial electric field in low to high confinement mode transitions in the DIII-D tokamak , 1995 .

[6]  P. Diamond,et al.  Dynamics of low to high (‘‘L’’ to ‘‘H’’) confinement bifurcation: Poloidal flow and ion pressure gradient evolution , 1994 .

[7]  E. Doyle,et al.  The phenomenology of the L-H transition in the DIII-D tokamak , 1994 .

[8]  Jonathan G. Watkins,et al.  Experimental survey of the L-H transition conditions in the DIII-D tokamak , 1994 .

[9]  V. Lebedev,et al.  Dynamics of L to H bifurcation , 1994 .

[10]  L. Lao,et al.  Role of the radial electric field in the transition from L (low) mode to H (high) mode to VH (very high) mode in the DIII‐D tokamak* , 1994 .

[11]  Wade,et al.  Rotation characteristics of main ions and impurity ions in H-mode tokamak plasma. , 1994, Physical review letters.

[12]  G. Staebler,et al.  Anomalous momentum transport from drift wave turbulence , 1993 .

[13]  R. J. Groebner,et al.  An emerging understanding of H-mode discharges in tokamaks , 1993 .

[14]  G. M. Staebler,et al.  Particle and energy confinement bifurcation in tokamaks , 1993 .

[15]  E. Doyle,et al.  Physics of the L-mode to H-mode transition in tokamaks , 1992 .

[16]  P. Diamond,et al.  Neoclassical poloidal and toroidal rotation in tokamaks , 1991 .

[17]  E. Doyle,et al.  Physics of the L to H transition in the DIII-D tokamak , 1990 .

[18]  E. C. Crume,et al.  Bifurcation theory of poloidal rotation in tokamaks: A model for L-H transition. , 1989, Physical review letters.

[19]  F. Hinton,et al.  Poloidal rotation in tokamaks with large electric field gradients , 1995 .

[20]  K. Shaing Ion orbit loss and poloidal plasma rotation in tokamaks , 1992 .

[21]  Paul W. Terry,et al.  Influence of sheared poloidal rotation on edge turbulence , 1990 .

[22]  Tadashi Sekiguchi,et al.  Plasma Physics and Controlled Nuclear Fusion Research , 1987 .