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Title: Impact of E × B shear flow on low-n MHD instabilities

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.4984257· OSTI ID:1566033
 [1]; ORCiD logo [2];  [3];  [3]; ORCiD logo [4];  [1]
  1. Peking Univ., Beijing (China). School of Physics, State Key Lab. of Nuclear Physics
  2. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  3. Peking Univ., Beijing (China). School of Physics, State Key Lab. of Nuclear Physics; Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  4. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States); Chinese Academy of Sciences (CAS), Hefei (China). Inst. of Plasma Physics

Recently, the stationary high confinement operations with improved pedestal conditions have been achieved in DIII-D [K. H. Burrell et al., Phys. Plasmas 23, 056103 (2016)], accompanying the spontaneous transition from the coherent edge harmonic oscillation (EHO) to the broadband MHD turbulence state by reducing the neutral beam injection torque to zero. It is crucial for the burning plasma devices such as ITER. Simulations about the effects of E×B shear flow on the quiescent H-mode (QH-mode) are carried out using the three-field two-fluid model in the field-aligned coordinate under the BOUT++ framework. Using the shifted circular cross-section equilibriums including bootstrap current, the results demonstrate that the E×B shear flow strongly destabilizes low-n peeling modes, which are mainly driven by the gradient of parallel current in peeling-dominant cases and are sensitive to the Er shear. Adopting the much more general shape of E×B shear (ωE=Er/RBθ) profiles, the linear and nonlinear BOUT++ simulations show qualitative consistence with the experiments. The stronger shear flow shifts the most unstable mode to lower-n and narrows the mode spectrum. At the meantime, the nonlinear simulations of the QH-mode indicate that the shear flow in both co- and counter directions of diamagnetic flow has some similar effects. The nonlinear mode interaction is enhanced during the mode amplitude saturation phase. These findings reveal that the fundamental physics mechanism of the QH-mode may be shear flow and are significant for understanding the mechanism of EHO and QH-mode.

Research Organization:
Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)
Sponsoring Organization:
USDOE National Nuclear Security Administration (NNSA)
Grant/Contract Number:
AC52-07NA27344; AC52-7NA27344
OSTI ID:
1566033
Alternate ID(s):
OSTI ID: 1375646
Report Number(s):
LLNL-JRNL-721760; 868466; TRN: US2000963
Journal Information:
Physics of Plasmas, Vol. 24, Issue 5; ISSN 1070-664X
Publisher:
American Institute of Physics (AIP)Copyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 19 works
Citation information provided by
Web of Science

References (23)

Energy loss for grassy ELMs and effects of plasma rotation on the ELM characteristics in JT-60U journal July 2005
Quiescent H-Mode Plasmas with Strong Edge Rotation in the Cocurrent Direction journal April 2009
Nonlinear MHD simulations of Quiescent H-mode plasmas in DIII-D journal September 2015
Influence of equilibrium shear flow on peeling-ballooning instability and edge localized mode crash journal September 2012
Nonlinear Simulations of Peeling-Ballooning Modes with Anomalous Electron Viscosity and their Role in Edge Localized Mode Crashes journal October 2010
Edge-localized-modes in tokamaks journal September 2014
Impact of a large density gradient on linear and nonlinear edge-localized mode simulations journal September 2013
The quiescent H-mode regime for high performance edge localized mode-stable operation in future burning plasmasa) journal May 2015
Impact of toroidal rotation on ELM behaviour in the H-mode on JT-60U journal April 2004
Digital Bispectral Analysis and Its Applications to Nonlinear Wave Interactions journal January 1979
NIMROD modeling of quiescent H-mode: reconstruction considerations and saturation mechanism journal September 2016
Rotational shear effects on edge harmonic oscillations in DIII-D quiescent H-mode discharges journal June 2016
Investigation of pellet-triggered MHD events in ASDEX Upgrade and JET journal August 2008
Reactor-relevant quiescent H-mode operation using torque from non-axisymmetric, non-resonant magnetic fields journal May 2012
Stability and dynamics of the edge pedestal in the low collisionality regime: physics mechanisms for steady-state ELM-free operation journal August 2007
Advances in understanding quiescent H-mode plasmas in DIII-D journal May 2005
Effects of E×B velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices journal May 1997
Studies of the ‘Quiescent H-mode’ regime in ASDEX Upgrade and JET journal July 2005
Erratum: “Neoclassical conductivity and bootstrap current formulas for general axisymmetric equilibria and arbitrary collisionality regime” [Phys. Plasmas 6 , 2834 (1999)] journal December 2002
3D vacuum magnetic field modelling of the ITER ELM control coil during standard operating scenarios journal August 2013
Edge localized modes and the pedestal: A model based on coupled peeling–ballooning modes journal May 2002
Boundary plasma turbulence simulations for tokamaks journal January 2014
Discovery of stationary operation of quiescent H-mode plasmas with net-zero neutral beam injection torque and high energy confinement on DIII-D journal March 2016

Cited By (4)


Figures / Tables (8)