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 CP11: Poster Session II: Basic Plasma Physics; Boundary, PMI, Proto-MPEX; International Tokamaks; Turbulence and Transport; Other Configurations; Z-pinch, Dense Plasma Focus and MagLIF (2:00pm-5:00pm)
Monday, November 5, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.CP11.192
Abstract: CP11.00192 : Recent progress in the PI3 spherical tokamak program
Presenter:
Kelly Epp
(General Fusion)
Authors:
Kelly Epp
(General Fusion)
Blake Rablah
(General Fusion)
Stephen J Howard
(General Fusion)
Michel Laberge
(General Fusion)
Meritt Reynolds
(General Fusion)
Peter O'Shea
(General Fusion)
William C. Young
(General Fusion)
Patrick Carle
(General Fusion)
Aaron Froese
(General Fusion)
Russ Ivanov
(General Fusion)
Achieving net energy gain with a Magnetized Target Fusion (MTF) system requires the plasma to satisfy a set of performance goals, such as particle inventory (~10^{21} ions), sufficient magnetic flux (~0.3 Wb) to confine the plasma without MHD instability, and initial energy confinement time several times longer than the compression time. To explore the physics of reactor-scale plasmas General Fusion (GF) has constructed Plasma Injector 3 (PI3). MTF relies on flux conservation by metal walls and so requires solenoid-free startup with no vertical field coils or toroidal field coils. Therefore the toroidal magnetic field in PI3 is produced by driving current along a single central conductor using a pulsed power supply that also provides a long low-voltage pulse to compensate resistive losses on multi-millisecond timescale. Once the toroidal field is established PI3 uses a short (20us) pulse coaxial helicity injection, from a magnetized Marshall gun, to produce a self-organized spherical tokamak plasma with minor radius 0.65m (the flux conserver radius is 1m). Plasma diagnostics include Mirnov probes, visible imaging, interferometers, optical spectroscopy, Doppler thermometry, Thomson scattering, and FIR polarimetry.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.CP11.192
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