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10-15 May 2021
Virtual Event
Europe/Vienna timezone
The Conference will be held virtually from 10-15 May 2021

Verification and Validation of Particle Simulation of Turbulent Transport in FRC

14 May 2021, 08:30
4h
Virtual Event

Virtual Event

Regular Poster Magnetic Fusion Theory and Modelling P7 Posters 7

Speaker

Zhihong Lin (UC Irvine)

Description

Following the remarkable progress in magnetohydrodynamic (MHD) stability control in the advanced beam driven field-reversed configuration (FRC) at TAE Technologies, Inc., turbulent transport has become one of the foremost obstacles on the path towards an FRC-based fusion reactor. Significant efforts have been made to kinetic simulation capabilities in FRC magnetic geometry. The Gyrokinetic Toroidal Code (GTC) (1) has been upgraded to simulate driftwave instability in the realistic FRC magnetic geometry using Boozer coordinates (2). GTC local simulations of the C-2 FRC find that electrostatic driftwaves are locally stable in the core. The stabilization mechanisms include finite Larmor radius effects, magnetic well (negative grad-B), and fast electron short circuit effects (3). In the scrape-off layer (SOL), collisionless electrostatic drift-waves in the ion-to-electron-scale are destabilized by electron temperature gradients due to the resonance with locally barely trapped electrons. Collisions can suppress this instability, but a collisional drift-wave instability still exists at realistic pressure gradients. Simulation results are in qualitative agreement with C-2 FRC experiments (4). In particular, the lack of ion-scale instability in the core is not inconsistent with experimental measurements of a fluctuation spectrum showing a depression at ion-scales. The pressure gradient thresholds for the SOL instability from simulations are also consistent with the critical gradient behavior observed in experiments.

Nonetheless, experimental measurements (4) indicate the existence of fluctuations in both FRC core and SOL, with much lower amplitude fluctuations measured in the core. To study the turbulence coupling between core and SOL, we have developed two complementary global particle codes GTC-X and ANC for simulations coupling the core and SOL by using cylindrical coordinates with field aligned mesh. In both codes, ions can be simulated as either gyrokinetic (5D) or fully kinetic (6D) particles, and electrons as gyrokinetic or drift-kinetic particles. This paper reports the verification and validation for both codes, and highlights new physics learned in these FRC simulations including global structures of driftwave instabilities, turbulence spreading from SOL to core, effects of equilibrium sheared flows and self-generated zonal flows, and effects of kinetic electrons and fully kinetic ions.

Global mode structures of ITG instabilities in FRC-- We used GTC-X to simulate the global properties of drift waves in the C2-U FRC, in which the core and SOL plasmas are connected with formation sections and divertors. The ion temperature gradient (ITG) modes are globally connected and unstable across these regions, while linearly stable inside the separatrix (5). The unstable global drift waves in the SOL show an axially varying structure that is less intense near the central FRC region and the mirror throat areas, while being more robust in the bad curvature formation exit areas (Fig. 1).

Comparison of 2D poloidal mode structures of electrostatic potentials from GTC-X simulations of ITG instability using different parallel domains (5). The dashed lines show the flux surfaces with the maximum mode amplitude. The blue solid line is the separatrix.

Turbulence spreading from SOL to core in FRC-- With the updated cross-separatrix capabilities, ANC global nonlinear turbulence simulations find that linear ITG instabilities grow in the SOL, generating fluctuations which spread from SOL to core (6). After saturation of the linear instabilities, a balance of the inward spread and local damping in the core is achieved. The steady state toroidal wavenumber spectrum shows lower amplitude core fluctuations and larger SOL fluctuations with amplitude decreasing towards shorter wavelengths, which are consistent with experimental measurements (Fig. 2).

Comparison of electrostatic potential spectra from ANC nonlinear simulations (solid lines) and from measurements in C2-U experiments (data points) (6). Shaded regions indicate the standard deviation of the simulation spectrum over the period for which this data represents.

Effects of sheared flows-- Radial electron fields due to electrode biasing have been implemented in GTC-X and first verified in simulation of the ITG with a rigid toroidal rotation, which shows a Doppler shift in real frequency but little change in growth rate. Linear simulations with sheared flows find that the ITG is significantly suppressed with this equilibrium ExB shearing rate is comparable to the growth rate in the absence of the sheared flows (Fig. 3). Both negative and positive shear can stabilize ITG by tilting the mode structure on the radial-toroidal plane. Consistently, turbulent transport is greatly reduced by the sheared flows in nonlinear simulations. Self-generated zonal flows have also been found to significantly reduce the ITG saturation amplitude and transport level. Logical sheath boundary condition and presheath potential have been calculated in a simple geometry and will be implemented in GTC-X FRC geometry.

ITG growth rate as a function of ExB shearing rate.

Effects of kinetic electrons and fully kinetic ions-- GTC-X simulations using drift kinetic electrons (DKE) and gyrokinetic ions find that ITG real frequency and growth rate are larger than adiabatic simulation, and mode peak position moves slightly outward. A considerable component of the electrostatic potential with poloidal harmonic m=0 (e.g., parallel wavevector k||=0) appears in the DKE simulation, which implies that the DKE model is necessary in FRC simulation. Finally, GTC-X fully kinetic ion (FKI) simulations of the ITG instability in SOL find that both frequency and growth rate are close to gyrokinetic simulations, but radial mode structures are slightly different. We will utilize the new FKI capability to study effects of energetic particles and high frequency (e.g., lower hybrid) instabilities in FRC turbulence and transport.

References:
(1) Z. Lin et al., Science 281, 1835 (1998).
(2) D. P. Fulton et al., Phys. Plasma 23, 012509 (2016); Phys. Plasmas 23, 056111 (2016).
(3) C. K. Lau et al., Phys. Plasma 24, 082512 (2017).
(4) L. Schmitz et al., Nat. Comm. 7, 13860 (2016).
(5) J. Bao et al., Phys. Plasmas 26, 042506 (2019).
(6) C. K. Lau et al., Nuclear Fusion 59, 066018 (2019).

Country or International Organization United States
Affiliation University of California, Irvine

Primary author

Zhihong Lin (UC Irvine)

Presentation Materials