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Developing high poloidal beta scenarios with internal transport barriers at large radius on KSTAR

ORAL

Abstract

Recent high-βP experiments on KSTAR show promising results with ~25% improvement in βN and enhanced Ti gradient at mid-radius at constant power and gas puffing rate with both carbon divertor and tungsten divertor. The high-βP scenario with internal transport barriers (ITBs) at large radius is a candidate operating scenario for steady-state tokamak reactors [Ding, Rev. Mod. Plasma Phys. 2023; Ding, Nature 2024]. A joint high-βP experiment on DIII-D with KSTAR-like constraints achieved excellent confinement quality due to successful establishment of such ITBs [Jeon, 66th APS-DPP], and was used as the basis for the KSTAR experiment. Besides achieving higher βN and stronger Ti gradient, the new experiment also shows lower l­i than the values in the previous KSTAR long-pulse high-βP operation, indicating progress in broadening the current profile. However, it is important to note that the achieved confinement in the recent KSTAR experiment is lower than its counterpart in DIII-D. The Ti gradient is not as strong in the KSTAR case, and the location of the high gradient is inside ρ~0.4, instead of ρ>0.6. There is no sign of ITB in the Te and ne channels. Based on the experimental data, TGLF modeling shows that the magnetic shear is not low enough at mid-radius, leaving the plasma on the low αMHD (normalized pressure) side of an instability mountain. Further optimization on the early phase of the discharge is planned for the coming KSTAR experiment.

Presenters

  • S. Ding

    General Atomics, General Atomics, San Diego, CA, United States of America

Authors

  • S. Ding

    General Atomics, General Atomics, San Diego, CA, United States of America

  • Andrea M. MV Garofalo

    General Atomics

  • YoungMu Jeon

    Korea Institute of Fusion Energy

  • Qiming Hu

    Princeton Plasma Physics Laboratory (PPPL), Princeton University

  • Huiqian Wang

    General Atomics

  • SangKyeun Kim

    Princeton Plasma Physics Laboratory (PPPL)