Radial electric fields and improved confinement regimes in the TJ-II stellarator

The influence of plasma density and edge gradients in the development of perpendicular sheared flows and radial electric fields, has been investigated in the plasma edge region of the TJ-II stellarator. Experimental results show that the development of the “naturally occurring” velocity shear layer requires a minimum plasma density (or gradient). Near this critical density, the level of edge turbulent transport and the turbulent kinetic energy significantly increase in the plasma edge; once sheared flows are fully developed the level of fluctuations and turbulent transport slightly decreases whereas edge gradients and plasma density increase. Furthermore, the resulting shearing rate of the spontaneous sheared flows turns out to be close to the one needed to trigger a transition to an improved confinement regimen (H-mode like regimes), suggesting that spontaneous sheared flows and fluctuations keep themselves near marginal stability. These findings provide the first experimental evidence of coupling between the development of sheared flows and increasing in level of edge turbulence. Experimental results are consistent with the expectations of second-order transition models of turbulence driven sheared flows.

[1]  A. Ware,et al.  Experimental evidence of coupling between sheared-flow development and an increase in the level of turbulence in the TJ-II stellarator. , 2004, Physical review. E, Statistical, nonlinear, and soft matter physics.

[2]  Á. Cappa,et al.  Improved confinement regimes induced by limiter biasing in the TJ-II stellarator , 2004 .

[3]  A. López-Fraguas,et al.  Interplay between parallel and perpendicular sheared flows and fluctuations in the plasma boundary region of the TJ-II stellarator , 2004 .

[4]  I. Pastor,et al.  The spectrometer of the high-resolution multiposition Thomson scattering diagnostic for TJ-II , 2003 .

[5]  M. Ochando,et al.  Emissivity toroidal asymmetries induced by ECRH driven convective fluxes in the TJ-II stellarator , 2003 .

[6]  T. Estrada,et al.  Impact of wall conditioning and gas fuelling on the enhanced confinement modes in TJ-II , 2003 .

[7]  A. Loarte,et al.  Experimental evidence of fluctuations and flows near marginal stability and dynamical interplay between gradients and transport in the JET plasma boundary region , 2003 .

[8]  T. Estrada,et al.  Spontaneous improvement of TJ-II plasmas confinement , 2002 .

[9]  M. Pedrosa,et al.  Fluctuations, sheared radial electric fields and transport interplay in fusion plasmas , 2002 .

[10]  T. Estrada,et al.  Density profile measurements by AM reflectometry in TJ-II , 2001 .

[11]  V. Tribaldos,et al.  Edge characteristics and global confinement of electron cyclotron resonance heated plasmas in the TJ-II stellarator , 2001 .

[12]  P. Terry,et al.  Suppression of turbulence and transport by sheared flow , 2000 .

[13]  Á. López-Sánchez,et al.  Fast movable remotely controlled Langmuir probe system , 1999 .

[14]  P. Diamond,et al.  Dynamics of second-order phase transitions in resistive pressure-gradient- driven turbulence , 1995 .

[15]  Liang,et al.  Self-Regulating Shear Flow Turbulence: A Paradigm for the L to H Transition. , 1994, Physical review letters.

[16]  D. Brower,et al.  Advanced plasma fluctuation analysis techniques and their impact on fusion research (invited) , 1988 .

[17]  E. Powers,et al.  Turbulent structure in the edge plasma of the TEXT tokamak , 1984 .