Ion target impact energy during Type I edge localized modes in JET ITER-like Wall
Creators
- 1. EUROfusion Consortium, JET, Culham Science Centre, Abingdon, OX14 3DB (United Kingdom)
- 2. CEA, IRFM, F-13108 Saint-Paul-lez-Durance (France)
- 3. IPP.CR, Institute of Plasma Physics AS CR, Za Slovankou 3, 182 21 Praha 8 (Czech Republic)
- 4. CCFE, Culham Science Centre, Abingdon OX14 3DB (United Kingdom)
- 5. Max-Planck-Institut fur Plasmaphysik, Boltzmannstr. 2, D-85748 Garching (Germany)
- 6. Instiut für Energie und Klimaforschung—Plasmaphysik, Forschungszentrum Jülich, 52425 Jülich (Germany)
- 7. Laboratorio Nacional de Fusión, CIEMAT, 28040 Madrid (Spain)
- 8. Institut Jean Lamour, UMR7198 CNRS—Université de Lorraine, F-54506 Vandoeuvre-les-Nancy Cedex (France)
- 9. YPI, University of York, York YO10 5DQ (United Kingdom)
- 10. Department of Physics, University of Strathclyde, Glasgow G4 0NG (United Kingdom)
Description
The ITER baseline scenario, with 500 MW of DT fusion power and Q = 10, will rely on a Type I ELMy H-mode, with ΔW = 0.7 MJ mitigated edge localized modes (ELMs). Tungsten (W) is the material now decided for the divertor plasma-facing components from the start of plasma operations. W atoms sputtered from divertor targets during ELMs are expected to be the dominant source under the partially detached divertor conditions required for safe ITER operation. W impurity concentration in the plasma core can dramatically degrade its performance and lead to potentially damaging disruptions. Understanding the physics of plasma-wall interaction during ELMs is important and a primary input for this is the energy of incoming ions during an ELM event. In this paper, coupled Infrared thermography and Langmuir Probe (LP) measurements in JET-ITER-Like-Wall unseeded H-mode experiments with ITER relevant ELM energy drop have been used to estimate the impact energy of deuterium ions (D+) on the divertor target. This analysis gives an ion energy of several keV during ELMs, which makes D+ responsible for most of the W sputtering in unseeded H-mode discharges. These LP measurements were possible because of the low electron temperature (Te) during ELMs which allowed saturation of the ion current. Although at first sight surprising, the observation of low Te at the divertor target during ELMs is consistent with the 'Free-Streaming' kinetic model which predicts a near-complete transfer of parallel energy from electrons to ions in order to maintain quasi-neutrality of the ELM filaments while they are transported to the divertor targets. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/0741-3335/57/8/085006Additional details
Identifiers
Publishing Information
- Journal Title
- Plasma Physics and Controlled Fusion
- Journal Volume
- 57
- Journal Issue
- 8
- Journal Page Range
- [8 p.]
- ISSN
- 0741-3335
- CODEN
- PPCFET
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 47113603
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY;
- Descriptors DEI
- CONCENTRATION RATIO; DEUTERIUM IONS; DIVERTORS; EDGE LOCALIZED MODES; ELECTRON TEMPERATURE; FIRST WALL; H-MODE PLASMA CONFINEMENT; IMPURITIES; INFRARED THERMOGRAPHY; ITER TOKAMAK; JET TOKAMAK; KEV RANGE; LANGMUIR PROBE; PLASMA; SPUTTERING; TUNGSTEN
- Descriptors DEC
- CHARGED PARTICLES; CLOSED PLASMA DEVICES; CONFINEMENT; DIMENSIONLESS NUMBERS; ELECTRIC PROBES; ELEMENTS; ENERGY RANGE; INSTABILITY; IONS; MAGNETIC CONFINEMENT; MEASURING METHODS; METALS; PLASMA CONFINEMENT; PLASMA INSTABILITY; PLASMA MACROINSTABILITIES; PROBES; REFRACTORY METALS; THERMOGRAPHY; THERMONUCLEAR DEVICES; THERMONUCLEAR REACTOR WALLS; THERMONUCLEAR REACTORS; TOKAMAK DEVICES; TOKAMAK TYPE REACTORS; TRANSITION ELEMENTS