skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Extending the physics basis of quiescent H-mode toward ITER relevant parameters

Journal Article · · Nuclear Fusion
 [1];  [2];  [3];  [2];  [1];  [4];  [5];  [1];  [2];  [2]
  1. Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
  2. General Atomics, San Diego, CA (United States)
  3. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
  4. ITER Organization, St. Paul Lez Durance (France)
  5. Univ. of Wisconsin-Madison, Madison, WI (United States)

In recent experiments on DIII-D we addressed several long-standing issues needed to establish quiescent H-mode (QH-mode) as a viable operating scenario for ITER. In the past, QH-mode was associated with low density operation, but has now been extended to high normalized densities compatible with operation envisioned for ITER. Through the use of strong shaping, QH-mode plasmas have been maintained at high densities, both absolute ($$\bar{n}$$e ≈ 7 × 1019 m$$-$$3) and normalized Greenwald fraction ($$\bar{n}$$e/nG > 0.7). In these plasmas, the pedestal can evolve to very high pressure and edge current as the density is increased. High density QH-mode operation with strong shaping has allowed access to a previously predicted regime of very high pedestal dubbed ‘Super H-mode’. Calculations of the pedestal height and width from the EPED model are quantitatively consistent with the experimentally observed density evolution. The confirmation of the shape dependence of the maximum density threshold for QH-mode helps validate the underlying theoretical model of peeling-ballooning modes for edge localized mode (ELM) stability. Generally, QH-mode is found to achieve ELM-stable operation while maintaining adequate impurity exhaust, due to the enhanced impurity transport from an edge harmonic oscillation, thought to be a saturated kink-peeling mode driven by rotation shear. In addition, the impurity confinement time is not affected by rotation, even though the energy confinement time and measured E × B shear are observed to increase at low toroidal rotation. In conclusion, together with demonstrations of high beta, high confinement and low q95 for many energy confinement times, these results suggest QH-mode as a potentially attractive operating scenario for the ITER Q = 10 mission.

Research Organization:
Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States); Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Fusion Energy Sciences (FES); USDOE Advanced Research Projects Agency - Energy (ARPA-E)
Grant/Contract Number:
AC52-07NA27344; AC02- 09CH11466; FC02-04ER54698; FG02-95ER54309; FG02-89ER53296; FG02- 08ER54999; AC02-09CH11466; FG02-08ER54999
OSTI ID:
1305848
Alternate ID(s):
OSTI ID: 1238818; OSTI ID: 1345498
Report Number(s):
LLNL-JRNL-700389
Journal Information:
Nuclear Fusion, Vol. 55, Issue 7; ISSN 0029-5515
Publisher:
IOP ScienceCopyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 11 works
Citation information provided by
Web of Science

References (23)

Chapter 1: Overview and summary journal June 2007
Edge localized modes (ELMs) journal February 1996
Characteristics of type I ELM energy and particle losses in existing devices and their extrapolation to ITER journal August 2003
Quiescent double barrier high-confinement mode plasmas in the DIII-D tokamak journal May 2001
I-mode: an H-mode energy confinement regime with L-mode particle transport in Alcator C-Mod journal August 2010
Advances in understanding quiescent H-mode plasmas in DIII-D journal May 2005
Observation of Plasma Rotation Driven by Static Nonaxisymmetric Magnetic Fields in a Tokamak journal November 2008
Advances towards QH-mode viability for ELM-stable operation in ITER journal July 2011
Chapter 2: Plasma confinement and transport journal December 1999
The quiescent H-mode regime for high performance edge localized mode-stable operation in future burning plasmasa) journal May 2015
Response of impurity particle confinement time to external actuators in QH-mode plasmas on DIII-D journal November 2014
Density limits in toroidal plasmas journal July 2002
Stability and dynamics of the edge pedestal in the low collisionality regime: physics mechanisms for steady-state ELM-free operation journal August 2007
Access to a New Plasma Edge State with High Density and Pressures using the Quiescent H Mode journal September 2014
The tokamak Monte Carlo fast ion module NUBEAM in the National Transport Code Collaboration library journal June 2004
Development and validation of a predictive model for the pedestal height journal May 2009
Reactor-relevant quiescent H-mode operation using torque from non-axisymmetric, non-resonant magnetic fields journal May 2012
ITER predictions using the GYRO verified and experimentally validated trapped gyro-Landau fluid transport model journal June 2011
Burning Plasma Confinement Projections and Renormalization of the GLF23 Drift-Wave Transport Model journal December 2003
Quiescent H-Mode Plasmas with Strong Edge Rotation in the Cocurrent Direction journal April 2009
Mechanisms for generating toroidal rotation in tokamaks without external momentum input journal May 2010
Characterization of intrinsic rotation drive on DIII-D journal May 2011
Impurity confinement and transport in high confinement regimes without edge localized modes on DIII-Da) journal May 2015

Cited By (2)