Author/Authors :
Pitts، نويسنده , , R.A. and Arnoux، نويسنده , , G. and Beurskens، نويسنده , , M. and Eich، نويسنده , , T. and Fundamenski، نويسنده , , W. M. Huber، نويسنده , , A. and Loarte، نويسنده , , A. and Marki، نويسنده , , J. and Stamp، نويسنده , , M.F. and Andrew، نويسنده , , P. and Brezinsek، نويسنده , , S. van Esser، نويسنده , , H.G. and Gulejova، نويسنده , , B. and Jachmich، نويسنده , , S. and Kreter، نويسنده , , A. and de la Luna، نويسنده , , E. and Matthews، نويسنده , , G.F. and Philipps، نويسنده , , V. and Solano، نويسنده , , E.، نويسنده ,
Abstract :
To ensure sufficient divertor target lifetime, the loss in plasma stored energy due to ELMs in ITER should be restricted to ΔWELM ⩽ 1 MJ. Only in JET, by virtue of its size, can such energies be approached. This contribution examines the impact of large, Type I ELMs in high current H-mode JET discharges with ITER-relevant pedestal characteristics. The ELMs provoke strong radiation losses, mostly confined to the inner divertor volume. Although the data are scattered, the average magnitude of this loss is ΔERAD ∼ 0.5ΔWELM, for ΔWELM < 0.55 MJ. For higher ΔWELM, greater fractional radiation losses occur, reaching ∼0.7ΔWELM at ΔWELM ∼ 0.9 MJ, indicating enhanced impurity release. Even at the highest ELM energies, peak divertor target surface temperatures are too low for carbon sublimation, suggesting that thermal decomposition and/or ablation of thick co-deposited layers on the inner target may be occurring. On average, across the range of energies studied, ELMs are found to deposit between 3–4.5% of ΔWELM on main wall limiters. When applied to the data for a specific discharge in the series, the model of ELM filament parallel energy losses developed at JET requires radial ELM velocities in the interval 0.1–0.65 km s−1 to explain these deposited energy fractions.
