29 June 2026 to 3 July 2026
EICC, Edinburgh
Europe/London timezone

Disruption mitigation in EAST with metal walls: a comparative study of shattered pellet injection and massive gas injection

Not scheduled
20m
EICC, Edinburgh

EICC, Edinburgh

150 Morrison St, Edinburgh EH3 8EE
Oral Presentation Disruptions and Runaway Electrons (MCF)

Description

The EAST superconducting tokamak, with Mo first walls and ITER-like W divertors, has developed and tested a Shattered Pellet Injection (SPI) system [1,2] and two Massive Gas Injection (MGI) systems [3] for disruption mitigation. Neon SPI experiments revealed key disruption dynamics including helical impurity transport and radiation evolution. Compared with MGI, SPI shows superior performance: a shorter TQ, longer CQ, stronger core radiation, and ~40% lower electron temperature with ~50% reduced divertor heat flux [4]. It also generates a more uniform poloidal radiation profile near the plasma core and avoids cold VDEs seen in MGI disruptions. Impurity injection, by either SPI or MGI, can trigger MHD mode switching from an inherent n=1/2 to a new n=1 with reversed rotation, attributed to impurity–plasma interactions [5]. SPI parameter scans showed smaller fragments ablate rapidly at the edge, while larger ones penetrate deeper and ablate slowly. Although ISPI generated more uniform TQ radiation, its poorer assimilation caused a longer pre-TQ phase and weaker halo current mitigation [6]. Finally, RE plateau formation was achieved with Ar-MGI, critically dependent on pre-disruption non-Maxwellian seed electrons and suppressed by MHD activity during TQ. These EAST results provide key data and insights for ITER disruption mitigation system design and operation.
Reference
[1] Yuan J.S. et al 2023 Fusion Eng. Des. 191 113567
[2] Yuan J.S. et al 2024 Fusion Eng. Des. 205 114551
[3] Zhuang H.D. et al 2015 Rev. Sci. Instrum. 86 053502
[4] Yuan J.S. et al 2023 Nucl. Fusion 63 106008
[5] Zhao S.B. et al 2024 Nucl. Fusion 65 016048
[6] Li L. et al 2025 Nucl. Fusion 65 086012

Author

Jiansheng Hu (Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences)

Co-authors

Prof. Dalong Chen (Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences) Dr Guizhong Zuo (Institue of Plasma Physics, Chinese Academy of Sciences) Dr Jingsheng Yuan (Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences) Dr Li Li (University of Science and Technology of China) Prof. Long Zeng (Department of Engineering Physics, Tsinghua University) Dr Shengbo Zhao (University of Science and Technology of China) Dr Tian Tang (Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences) Prof. Yanmin Duan (Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences)

Presentation materials