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 GO5: SPARC, C-Mod, and High Field Tokamaks
9:30 AM–12:30 PM,
Tuesday, November 6, 2018
OCC
Room: B113-114
Chair: Carlos Paz-Soldan, General Atomics
Abstract ID: BAPS.2018.DPP.GO5.8
Abstract: GO5.00008 : Current Quench Avoidance using Lower Hybrid Current Drive in the Alcator C-Mod Tokamak
10:54 AM–11:06 AM
Presenter:
Matthew Reinke
(Oak Ridge National Laboratory)
Authors:
Matthew Reinke
(Oak Ridge National Laboratory)
Steve Scott
(Princeton Plasma Physics Laboratory)
Robert S Granetz
(Massachusetts Inst of Tech-MIT)
Cristina Rea
(Massachusetts Inst of Tech-MIT)
Jerry W Hughes
(Massachusetts Inst of Tech-MIT)
Kevin J Montes
(Massachusetts Inst of Tech-MIT)
Stephen James Wukitch
(Massachusetts Inst of Tech-MIT)
Experiments from Alcator C-Mod demonstrate that following a full thermal collapse due to a large impurity influx, a current quench (CQ) can be avoided using lower hybrid (LH) current drive. This existence proof shows a CQ does not necessarily follow a thermal quench (TQ) when the helicity is maintained externally via RF, opening new optimization strategies for disruption avoidance. In a 400 kA, ne,bar~ 0.5x1020 m-3, 5.4 T L-mode plasma, 700 kW of 4.6 GHz LH power is used to approach fully non-inductive operation, dropping Vloop from 0.8 V to ~0.1 V. A high-Z injection increases the PRAD above the input power, causing a cooling wave to propagate inward with temperatures dropping over ~100 ms to those resembling a post-TQ plasma. While the Ip and ne,bar remain fixed within ~10%, on-axis Te drops from 3 keV to 10’s of eV, and Te becomes peaked off-axis at r/a ~ 0.7 with values as low as 170 eV. As the impurity density decays, the plasma re-heats, the RF turns off and the plasma reverts to its pre-injection state over ~500 ms. During this event, Vloop reaches up to 1.5 V, corresponding to a max E/Ecrit ~ 9. Similar plasmas exhibit the high-Z cooling behavior, but MHD-induced loss of fast electrons and termination of LH power results in a transition to a standard CQ in < 10 ms.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.GO5.8
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