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Investigation of the role of pedestal pressure and collisionality on type-I ELM divertor heat loads in DIII-D

Journal Article · · Nuclear Fusion
 [1];  [2];  [3];  [3];  [4];  [3];  [3];  [5];  [3];  [6];  [7];  [7];  [3];  [6];  [2];  [3];  [3];  [4]
  1. Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States); General Atomics
  2. Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)
  3. General Atomics, San Diego, CA (United States)
  4. Max Planck Inst. for Plasma Physics, Garching (Germany)
  5. Massachusetts Inst. of Technology (MIT), Cambridge, MA (United States)
  6. Univ. of California, San Diego, CA (United States)
  7. Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)

Here, a non-dimensional collisionality scan conducted on DIII-D confirms a model for ELM energy densities recently put forward by Eich [1], but also reveals key effects that may explain the large scatter typically observed about the scaling. Electron Cyclotron Heating (ECH) close to the plasma edge was used to raise electron temperatures at the pedestal top and lower collisionality to ITER level, while the power of Neutral Beam Injection (NBI) was decreased during discharges to operate closer to the L-H transition threshold. The scan reveals no explicit pedestal pressure dependence of the ELM energy densities. While collisionality does not play a decisive role, the ratio of heating power to the power over the L-H-threshold is identified as parameter determining the agreement with the model, with discharges marginally above the threshold showing the largest scatter in the database and exceeding the predicted ELM energy up to twofold. Operation close to the L-H-threshold is accompanied by low ELM frequency and large 2 ELM heat loads. Using linear stability calculations, ELM energy densities are shown to be inversely proportional to the most unstable linear mode number before the ELM crash. There are indications that the scatter in the data when compared with the Eich model prediction is caused by including only a limited set out of all quantities in the model that are considered by linear stability analysis. While further ELM studies near the LH threshold are of great priority, the overall agreement of DIII-D with the Eich model recommends its use in extrapolations towards ITER.

Research Organization:
General Atomics, San Diego, CA (United States). DIII-D National Fusion Facility (DIII-D); Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States); Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Fusion Energy Sciences (FES) (SC-24); USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22). Scientific User Facilities Division
Grant/Contract Number:
FC02-04ER54698; FG02-07ER54917; FG02-05ER54809
OSTI ID:
1460098
Alternate ID(s):
OSTI ID: 1542716
OSTI ID: 22929482
Journal Information:
Nuclear Fusion, Journal Name: Nuclear Fusion Journal Issue: 9 Vol. 58; ISSN 0029-5515
Publisher:
IOP ScienceCopyright Statement
Country of Publication:
United States
Language:
English

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