Bulletin of the American Physical Society
63rd Annual Meeting of the APS Division of Plasma Physics
Volume 66, Number 13
Monday–Friday, November 8–12, 2021; Pittsburgh, PA
Session PO07: MFE: MHD and Energetic Particles
2:00 PM–5:00 PM,
Wednesday, November 10, 2021
Room: Rooms 315-316
Chair: Valerie Izzo, Fiat Lux
Abstract: PO07.00006 : Modelling sawteeth in tokamak plasma as a sequence of Multi-region Relaxed MHD equilibria*
3:00 PM–3:12 PM
Presenter:
Zhisong Qu
(Australian Natl Univ)
Authors:
Zhisong Qu
(Australian Natl Univ)
Yao Zhou
(Princeton Plasma Physics Laboratory)
Robert Dewar
(Australian Natl Univ)
Arunav Kumar
(Australian National University)
Joshua Doak
(Australian National University)
Joaquim Loizu
(Ecole Polytechnique Federale de Lausanne)
Matthew Hole
(Australian National University)
A sawtooth [3] is a spontaneous energy relaxation process in tokamak plasma. In the early phase of a sawtooth crash with a relatively small resistivity, the reconnection velocities are not too fast compared with the Alfven speed. One can model the plasma globally as a sequence of equilibria, treating the reconnection layer as an infinitely thin current sheet [4]. Starting with an unstable axisymmetic MRxMHD equilibrium, we found that a lower energy state exists with a helical core. The two interfaces bounding the volume containing the q=1 surface clash together to form a “cusp-type” current sheet [5]. We then construct a sequence of equilibrium by removing the interfaces one by one. The result is compared to a M3D-C1 [6] simulation.
[1] M. Hole, S. Hudson, and R. Dewar, Nucl. Fusion 47, 746 (2007).
[2] S.R. Hudson, R.L. Dewar et al., Phys. Plasmas 19, 112502-1–18, (2012).
[3] S. von Goeler, W. Stodiek, and N. Sauthoff, Phys. Rev. Lett. 33, 1201 (1974).
[4] R.M. Kulsrud, Phys. Plasmas 18, (2011).
[5] D.A. Uzdensky and R.M. Kulsrud, Phys. Plasmas 4, 3960 (1997).
[6] S.C. Jardin, N. Ferraro, J. Breslau, and J. Chen, Comput. Sci. Discov. 5, 014002 (2012).
*This research was undertaken with the assistance of resources and services from the National Computational Infrastructure (NCI), which is supported by the Australian Government.This work was supported by a grant from the Simons Foundation/SFARI (560651, AB). This work is partly funded by Australian Research Council project DP170102606.
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