Ecton Mechanism of Energy Load on ITER-Grade Tungsten Limiter T-10 Tokamak and Forecast for ITER
Creators
- 1. International Thermonuclear Experimental Reactor (ITER), Project Centre "ITER", Moscow (Russian Federation)
- 2. National Research University "Moscow Power Engineering Institute", Krasnokazarmennaya 14, Moscow (Russian Federation)
- 3. National Research Centre "Kurchatov Institute", Moscow (Russian Federation)
- 4. P. N. Lebedev Physical Institute, RAS, Moscow (Russian Federation)
Description
Full text: Extremely high heat loads, both during steady state and transient events, are expected on the tungsten divertor plates of the ITER facility, undertaken at Cadarache, France. In this paper non ambipolar plasma flow toward the surface, due to arcs and sparks, was investigated as mechanism of power exhaust, leading to enhanced heating of plasma facing materials (PFMs) at a very high heat load. This ecton mechanism results in the pulsed-periodic ignition of explosive electron emission events providing high enough electron current from the wall. Unlike standard thermionic emission, such mechanism can dramatically increase electron emission and, as a result, sparks and arcs activity, leads to a surface overheating and melting. Such phenomenon have been observed in experiments on the T-10 tokamak with ITER-grade tungsten (W) poloidal limiter under a powerful plasma electron cyclotron resonance heating (ECRH) and plasma ring shifted inside. In such conditions, the interior tungsten plates of limiter were heated up to temperature exceeded 2000° C, estimated local thermal load were of more than 40 MW/m2 on the plate edges, leading to surface melting. Intensive sparking and arcing, deep cracks and edge melting were observed on W tiles. Also, tile surfaces were flooded by recrystallized tungsten. All W tile surfaces are covered by two crater types: deep, (with dimensions from 10 to 100 μm) and acetabuliform type (with dimensions from 0.5–20 μm) arranged in "long chains"— vacuum arcs, and "short chains"— vacuum sparks. The reason for such sub-μs discharges ignition can be plasma-turbulence- driven fluctuations of particle and energy flux to the plasma-modified surface. The report analyzes consequences for ITER of the EEE appearance on the divertor W surface, the sharpening of SOL power width distribution, parallel to the magnetic field -λq; the melting of the W leading edges of divertor targets and the recrystallization of the W surface as a result of the superheated liquid metal droplets appearance. Melt tungsten can be subject to J x B force. EEE can lead to the erosion enhancement of the divertor plates. Microexplosions lead to droplets, which, like dust particles, can effectively deliver impurities to the central region of the plasma. (author)
Additional details
Identifiers
Publishing Information
- Imprint Title
- 27th IAEA Fusion Energy Conference. Programme and Book of Abstracts
- Imprint Pagination
- 844 p.
- Journal Page Range
- p. 311
- Report number
- IAEA-CN--258
Conference
- Title
- 27. IAEA Fusion Energy Conference
- Acronym
- FEC 2018
- Dates
- 22-27 Oct 2018
- Place
- Ahmedabad (India)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 50052373
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- CRACKS; DIVERTORS; ECR HEATING; ELECTRON EMISSION; EROSION; FIRST WALL; HEATING LOAD; ITER TOKAMAK; LIMITERS; LIQUID METALS; MAGNETIC FIELDS; MELTING; PLASMA IMPURITIES; PLASMA RINGS; PLATES; RECRYSTALLIZATION; STEADY-STATE CONDITIONS; T-10 TOKAMAK; THERMIONIC EMISSION; TUNGSTEN
- Descriptors DEC
- CLOSED PLASMA DEVICES; ELEMENTS; EMISSION; FLUIDS; HEATING; HIGH-FREQUENCY HEATING; IMPURITIES; LIQUIDS; METALS; PHASE TRANSFORMATIONS; PLASMA HEATING; REFRACTORY METALS; THERMONUCLEAR DEVICES; THERMONUCLEAR REACTOR WALLS; THERMONUCLEAR REACTORS; TOKAMAK DEVICES; TOKAMAK TYPE REACTORS; TRANSITION ELEMENTS
Optional Information
- Secondary number(s)
- IAEA-CN--258-384