Kinetic Profiles and Impurity Transport Response to 3D-Field Triggered ELMs in NSTX
Creators
- 1. Lawrence Livermore National Laboratory (LLNL), Livermore, CA 94550 (United States)
- 2. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN 37831 (United States)
- 3. Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ 08540 (United States)
Description
Full text: The response of kinetic plasma profiles to 3D-field triggered edge localized modes (ELMs) and the inter-ELM carbon impurity transport were analyzed in lithium-conditioned H-mode discharges in NSTX. ELM-free lithium-conditioned H-mode discharges were characterized by core accumulation of impurities as a result of near-neoclassical impurity transport, an edge inward pinch and the absence of impurity flushing mechanisms. Nonaxisymmetric magnetic perturbations (n = 3) were applied to trigger ELMs (triggering frequency fELM = 10–62.5 Hz), and mitigate core impurity buildup maintaining the positive effects of lithium on energy confinement. Edge impurity flushing increased with fELM, with a progressive reduction in the carbon density nC at the pedestal top. For ELMs triggered at 10 Hz, up to a 30% drop in nC was observed, with comparable effects in the ne, Ti, and toroidal velocity vθ profiles. The increase in fELM led to a reduction in the core carbon inventory and progressively modified edge profiles. Inside the pedestal top, nC and ne were reduced by up to 60% and 40%, respectively, while being unaffected in the steep gradient region. Ti and vθ normalized edge gradients increased by up to a factor of three. The ELM effect on the nC profiles was reproduced in simulations with the impurity transport code MIST with an inward convective perturbation and an outward diffusive/convective perturbation to the steady state carbon transport coefficients (inside and outside normalized volumetric radii RVOL of 0.6, respectively). The agreement of inter-ELM carbon transport with neoclassical estimates improved with the increase in fELM. The changes in Ti and nD profiles due to triggered ELMs led to changes in carbon neoclassical transport coefficients comparable and opposite to those observed with the transition from ELMy boronized discharges to ELM-free lithium-conditioned discharges. In particular, the carbon neoclassical convective velocity (evaluated via NCLASS) at the top of the pedestal changed direction (from inward to outward). Concomitantly, better agreement between the neoclassical transport predictions and experimental inter-ELM nC profile shapes was observed in lithium-conditioned discharges with triggered ELMs in a similar way to naturally ELMy discharges. (author)
Additional details
Identifiers
Publishing Information
- Imprint Title
- 26. IAEA Fusion Energy Conference. Programme, Abstracts and Conference Material
- Imprint Pagination
- 935 p.
- Journal Page Range
- p. 281
- Report number
- IAEA-CN--234
Conference
- Title
- 26. IAEA Fusion Energy Conference
- Acronym
- FEC 2016
- Dates
- 17-22 Oct 2016
- Place
- Kyoto (Japan)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 49089450
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- CARBON; DENSITY; DISTURBANCES; EDGE LOCALIZED MODES; EXPERIMENT RESULTS; H-MODE PLASMA CONFINEMENT; KINETICS; LITHIUM; NEOCLASSICAL TRANSPORT THEORY; NSTX DEVICE; PLASMA IMPURITIES; PLASMA RADIAL PROFILES; PLASMA SIMULATION; STEADY-STATE CONDITIONS
- Descriptors DEC
- ALKALI METALS; CHARGED-PARTICLE TRANSPORT THEORY; CLOSED PLASMA DEVICES; CONFINEMENT; ELEMENTS; IMPURITIES; INSTABILITY; MAGNETIC CONFINEMENT; METALS; NONMETALS; PHYSICAL PROPERTIES; PLASMA CONFINEMENT; PLASMA INSTABILITY; PLASMA MACROINSTABILITIES; SIMULATION; SPHEROMAK DEVICES; THERMONUCLEAR DEVICES; TOKAMAK DEVICES; TRANSPORT THEORY
Optional Information
- Contract/Grant/Project number
- Contract DE-AC02-09CH11466; DEAC05-00OR22725; DE-AC52-07NA27344
- Notes
- Abstract only
- Secondary number(s)
- IAEA-CN--234-0756