Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session KI03: Invited: MFE III - International Tokamak Overviews
3:00 PM–5:00 PM,
Tuesday, October 8, 2024
Hyatt Regency
Room: Centennial IV
Chair: Rajesh Maingi, Princeton Plasma Physics Laboratory (PPPL)
Abstract: KI03.00003 : Commencement of the plasma operation in JT-60SA: the world's largest test bed for ITER and DEMO
4:00 PM–4:30 PM
Presenter:
Takuma Wakatsuki
(National Institutes for Quantum Science and Technology)
Author:
Takuma Wakatsuki
(National Institutes for Quantum Science and Technology)
Collaboration:
the JT-60SA Integrated Project Team
The first plasma of JT-60SA was achieved in a challenging situation, where appliable toroidal electric field E|| is restricted under 0.15 V/m because its operation was started without using a high-voltage power supply system for safer operation. This result is noteworthy since the establishment of the discharge scenario at a limited power supply voltage accompanied by increasing the machine size is a crucial issue for future large superconducting tokamaks including ITER. The Trapped Particle Configuration (TPC) start-up method, which utilized the mirror-trap of EC-heated electrons, proved effective in low E|| start-up.
The wall conditioning technique compatible with the superconducting machine was employed. It was demonstrated that the first plasma can be achieved with baking and H2 and He glow discharge cleaning. EC wall cleaning was also tried, and the dependence of cleaning efficiency on the poloidal magnetic field configuration was investigated.
The magnetic control of JT-60SA was efficiently developed using the Magnetohydrodynamic Equilibrium Control Simulator (MECS). A novel control scheme was developed using MECS code, facilitating the swift attainment of a MA-class diverted plasma. Despite the relatively limited diagnostic tools available during JT-60SA's initial operation, key plasma parameters were measured to estimate the basic confinement characteristics. The electron temperature was estimated to reach the keV range at the core region and the line-averaged electron density was increased to 1x1019 m-3.
Since this development of the MA-class discharge scenario was consistently carried out under constraints specific to large superconducting devices for the first time, the solutions that made the first plasma operation of JT-60SA successful will have significant contribution to ITER and DEMO reactors.
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