DIII-D research towards resolving key issues for ITER and steady-state tokamaks
Creators
- 1. Lawrence Livermore National Laboratory, Livermore, CA 94551 (United States)
Description
The DIII-D research program is addressing key ITER research needs and developing the physics basis for future steady-state tokamaks. Pellet pacing edge-localized mode (ELM) control in the ITER configuration reduces ELM energy loss in proportion to 1/fpellet by inducing ELMs at up to 12× the natural ELM rate. Complete suppression of ELMs with resonant magnetic perturbations has been extended to the q95 expected for ITER baseline scenario discharges, and long-duration ELM-free QH-mode discharges have been produced with ITER-relevant co-current neutral-beam injection (NBI) using external n = 3 coils to generate sufficient counter-Ip torque. ITER baseline discharges at βN ∼ 2 and scaled NBI torque have been maintained in stationary conditions for more than four resistive times using electron cyclotron current drive (ECCD) for tearing mode suppression and disruption avoidance; active tracking with steerable launchers and feedback control catch these modes at small amplitude, reducing the ECCD power required to suppress them. Massive high-Z gas injection into disruption-induced 300–600 kA 20 MeV runaway electron (RE) beams yield dissipation rates ∼10× faster than expected from e–e collisions and demonstrate the possibility of benign dissipation of such REs should they occur in ITER. Other ITER-related experiments show measured intrinsic plasma torque in good agreement with a physics-based model over a wide range of conditions, while first-time main-ion rotation measurements show it to be lower than expected from neoclassical theory. Core turbulence measurements show increased temperature fluctuations correlated with sharply enhanced electron transport when ∇Te/Te-1 exceeds a critical-gradient scale length. In H-mode, data show the pedestal height and width growing between ELMs with ∇P at the computed kinetic-ballooning limit, in agreement with the EPED model. Successful modification of a neutral-beam line to provide 5 MW of adjustable off-axis injection has enabled sustained operation at βN ∼ 3 with broader current and pressure profiles at higher qmin than previously possible, though energy confinement is lower than expected. Initial experiments aimed at developing integrated core and boundary solutions demonstrated heat flux reduction using enhanced edge radiation from neon injection and innovative divertor geometries (e.g. snowflake configuration). (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/0029-5515/53/10/104001Additional details
Identifiers
Publishing Information
- Journal Title
- Nuclear Fusion
- Journal Volume
- 53
- Journal Issue
- 10
- Journal Page Range
- [18 p.]
- ISSN
- 0029-5515
- CODEN
- NUFUAU
Conference
- Title
- 24. fusion energy conference
- Dates
- 8-13 Oct 2012
- Place
- San Diego, CA (United States)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 45014513
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- BALLOONING INSTABILITY; BEAM INJECTION; DOUBLET-3 DEVICE; ECR CURRENT DRIVE; EDGE LOCALIZED MODES; ENERGY LOSSES; GAS INJECTION; H-MODE PLASMA CONFINEMENT; ITER TOKAMAK; NEOCLASSICAL TRANSPORT THEORY; NEON; NEUTRAL CURRENTS; PERTURBED ANGULAR CORRELATION; RUNAWAY ELECTRONS; STEADY-STATE CONDITIONS; TEARING INSTABILITY; TORQUE
- Descriptors DEC
- ALGEBRAIC CURRENTS; ANGULAR CORRELATION; CHARGED-PARTICLE TRANSPORT THEORY; CLOSED PLASMA DEVICES; CONFINEMENT; CORRELATIONS; CURRENTS; ELECTRONS; ELEMENTARY PARTICLES; ELEMENTS; FERMIONS; FLUID INJECTION; FLUIDS; GASES; INSTABILITY; LEPTONS; LOSSES; MAGNETIC CONFINEMENT; NON-INDUCTIVE CURRENT DRIVE; NONMETALS; PLASMA CONFINEMENT; PLASMA INSTABILITY; PLASMA MACROINSTABILITIES; RARE GASES; THERMONUCLEAR DEVICES; THERMONUCLEAR REACTORS; TOKAMAK DEVICES; TOKAMAK TYPE REACTORS; TRANSPORT THEORY
Optional Information
- Collaborations
- DIII-D Team