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Title: Characteristics of Ultralow Aspect Ratio Toroidal Plasmas and Non-Solenoidal Startup and Edge Stability Studies at Near-Unity Aspect Ratio (Final Report)

Technical Report ·
DOI:https://doi.org/10.2172/1597018· OSTI ID:1597018

This grant supported a long-term research and development program to explore the physics and technology of spherical tokamak (ST) plasma behavior at near-unity aspect ratio (A). The PEGASUS Toroidal Experiment is a university-scale (R) ~ 0.40 m, α ~ .35 m, Ip ≤ 0.3 MA, BT ≤ 0.15 T) experiment that accesses A → 1, to provide large values of the normalized plasma current, IN = IpBT, or equivalently the toroidal field utilization factor Ip/ITF. The research activities focused on: 1) developing the technique of Local Helicity Injection (LHI) as a viable means of initiating and growing an ST plasma without the use of a central solenoid; 2) exploring the equilibrium and stability properties of spherical tokamak plasmas at extremely low aspect ratio; and 3) obtaining new insights in the properties of the enhanced confinement H-mode regime at A ~ 1. The initial (Phase I) facility employed a unique high-stress central solenoid Ohmic for current drive and heating with simple magnet current waveforms. A subsequent major upgrade (Phase II) offered more flexible control of the plasma evolution along with a powerful LHI system for plasma initiation, heating and sustainment. The LHI technique consists of injection of high-density current streams into vacuum toroidal and vertical magnetic fields. These streams become unstable and support magnetic reconnection to allow the system to relax into a tokamak-like magnetic configuration. This program focused on: 1) development of electron current sources that provide sufficiently high injection currents in the challenging edge plasma region; 2) validation of theoretical limits to achievable Ip arising from magnetic helicity and energy conservation plus absolute limits arising from relaxation to a minimal energy states; 3) tests of a power balance model to describe the evolution of the plasma current Ip(t); and 4) study of magnetic fluctuations and their role in the Ip evolution. This culminated in the production of toroidal currents of Ip ≥ 0.2 MA with only ~8 kA of injected current. Operation with Ohmic induction alone in Phase I created plasmas with soft limits on the achievable Ip and field utilization (Ip/ITF ~ 1) due to the onset of large low-order (2/1 or 3/2) internal resonant tearing modes. With the expanded capabilities in Phase II operation, methods employed to mitigate those modes and achieve Ip/ITF > 1 were: 1) ITF ramp-downs; 2) non-solenoidal startup via LHI; and 3) extremely low ITF Ohmic operations assisted by LHI current injector pre-ionization. Extensive use of LHI-driven startup and drive for non-solenoidal operation produced favorable current profiles to stably operate tokamak plasmas with unprecedentedly high IN = Ip/aBT ~ 15 and Ip/ITF > 2. With strong reconnection-driven anomalous ion heating, this in turn provided access to tokamak plasmas with Bt up to 100%, a world record 2 times higher than that previously achieved in advanced or spherical tokamaks. This high Bt regime had a large fraction (~50%) of the plasma volume in a region of an absolute minimum-B configuration. The MHD stability limit in this regime was the ideal external kink mode without a stabilizing wall. These results provided the first demonstration of access to tokamak plasmas with very high Bt, high iN, high elongation κ, and low internal inductance ℓi, and as such served as a proof-ofprinciple for access to this long-sought ST regime. The naturally low BT needed for stability at A ≤ 1.2 reduces the L-H mode power threshold, PLH, so that H-mode plasmas were achieved with Ohmic heating alone. The power threshold for the transition to the H-mode regime was found to be 10× the accepted values from the ITER international scaling, confirming initial trends indicated by experiments on MAST and NSTX, and suggesting that the physics behind this transition is not yet fully understood. The density dependence of the transition and the observed insensitivity to whether the plasma is bounded by a limiter or magnetic divertor are consistent with the recent FM3 model. Multiple unstable toroidal magnetic modes were measured during ELM (Edge Localized Mode) crashes, with generally lower toroidal mode numbers than seen at higher A, which was attributed to the larger peeling mode instability drive at low A. First-ever edge current profile measurements through an ELM crash showed current-carrying filaments were generated, as seen in ELM simulations and in electromagnetic blob transport theory.

Research Organization:
Univ. of Wisconsin, Madison, WI (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Fusion Energy Sciences (FES)
DOE Contract Number:
FG02-96ER54375
OSTI ID:
1597018
Report Number(s):
DOE-UWMDSN-54375; TRN: US2102702
Country of Publication:
United States
Language:
English