Modeling deep slot divertor concepts at DIII-D using SOLPS-ITER with drifts

R. Maurizio, A. W. Leonard, A. G. McLean, M. W. Shafer, P. C. Stangeby, D. Thomas, J. H. Yu

Research output: Contribution to journalArticlepeer-review

2 Scopus citations

Abstract

A staged divertor program is currently under discussion to advance DIII-D research on core-edge integration. One phase could address optimization of power and particle exhaust, and supporting modeling of several slot divertor options is underway, including variations in wall baffling, slot depth and divertor leg length. This paper focuses on the role of slot depth to achieve highly dissipative (detached) divertor conditions, in both BT directions. For ion B×∇B into the divertor and PSOL= 4 MW, SOLPS-ITER finds that increasing the slot depth from 18 to 50 cm reduces the upstream separatrix electron density needed to detach by 15%, due to increased divertor radiation. A dedicated run of the EIRENE neutral transport code, in which neutrals are launched from the outer target and followed until ionization, finds that neutral leakage is strongly reduced in the deep slot compared to the shallow slot, explaining the increased divertor radiation and, thus, lower detachment density threshold. Reversing the BT direction cools and densifies the plasma in the slot, such that both slot options are detached at all simulated densities. As for the opposite BT direction, the deep slot has lower target temperature compared to the shallow slot, as a result of lower neutral leakage. Increasing the depth of a slot divertor is, therefore, beneficial to achieve highly dissipative divertor conditions for both field directions. Additional modeling will build on these results to evaluate whether an increased slot depth can also improve trapping of low-Z radiating impurities.

Original languageEnglish
Article number101356
JournalNuclear Materials and Energy
Volume34
DOIs
StatePublished - Mar 2023

Funding

The authors would like to thank the entire DIII-D Divertor Science and Innovation team for their help and constructive discussions. This material is based upon work supported by the U.S. Department of Energy , Office of Science, Office of Fusion Energy Sciences, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Award(s) DE-FC02-04ER54698 and DE-AC05-00OR22725. The authors would like to thank the entire DIII-D Divertor Science and Innovation team for their help and constructive discussions. This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Fusion Energy Sciences, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Award(s) DE-FC02-04ER54698 and DE-AC05-00OR22725. This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.

FundersFunder number
United States Government
U.S. Department of Energy
Office of ScienceDE-AC05-00OR22725, DE-FC02-04ER54698
Fusion Energy Sciences

    Keywords

    • DIII-D
    • Detachment
    • Divertor
    • SOLPS-ITER
    • Slot divertor

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