Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session NP11: Poster Session V: Laser-plasma Particle Acceleration; HEDP; Turbulence and Transport; DIII-D Tokamak; Machine Learning, Data Science (9:30am-12:30pm)
Wednesday, November 7, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.NP11.122
Abstract: NP11.00122 : Rotating RMP stabilization of ``Neoclassical Tearing Modes''*
Presenter:
Linda Sugiyama
(Massachusetts Inst of Tech-MIT)
Authors:
Linda Sugiyama
(Massachusetts Inst of Tech-MIT)
Michio Okabayashi
(Princeton Plasma Phys Lab)
Liqing Xu
(IPP CAS)
In DIII-D, a slowly rotating nonaxisymmetric magnetic field (RMP) with toroidal harmonic n=1 can, using feedback, lock onto the rotation of an unstable m=2/n=1 neoclassical tearing mode (NTM) and prevent it from growing to a disruption[1]. Nonlinear simulation with the extended MHD code M3D shows a complex picture. The MHD evolves much faster than the RMP rotation. The background RMP-stabilized plasma has relatively high central beta. Without the RMP, it is unstable to a new type of instability over q=1, a nonlinear ideal-MHD unstable mode with coupled n=1 and 2 harmonics, that grows to an internal-kink-like sawtooth crash. A perturbation with n=1 and m=2/n=2 remains over q=1+ and couples to other harmonics across the entire plasma radius, consistent with observations of δTi and δTe. No large 2/1 magnetic island is seen in simulation or the experiment. The vacuum rotating field from the I-coil with 2.5 kA current is larger than the MHD mode on the large-R side of the plasma and comparable over q<1, suggesting that the RMP couples to, and influences, the full n=1 perturbation. These processes will be further studied.
[1] M. Okabayashi et al., Nuc. Fusion 57, 016035 (2017).
*Supported in part by U.S. DOE DE-SC-0007883 and DE-FC02-04ER54698.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.NP11.122
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