Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session GP12: Poster Session III:
Low Temperature Plasmas
Fundamental Plasma Physics I: computation, boundaries
Fundamental Plasma Physics II: dusty, diagnostics
MFE Measurement and Diagnostics Techniques, Technology, and Edge and Pedestal Physics
9:30 AM - 12:30 PM
Tuesday, October 8, 2024
Hyatt Regency
Room: Grand Hall West
Abstract: GP12.00142 : Adding a fluid neutrals model to the gyrokinetic code GENE-X for edge/SOL turbulence simulation in divertor geometries
Presenter:
Sabine Ogier-Collin
(IPP Garching)
Authors:
Sabine Ogier-Collin
(IPP Garching)
Frank Jenko
(University of Texas at Austin)
Wladimir Zholobenko
(IPP Garching)
Philipp Ulbl
(Max Planck Institute for Plasma Physics)
In this work a novel coupling of a continuum gyrokinetic model with a fluid neutrals model using the GENE-X code[1] is detailed. GENE-X is a global, full-f, electromagnetic, collisional gyrokinetic turbulence code for studying the edge and SOL in realistic geometries, including magnetic X-points. Neutrals are treated as a fluid to minimize computational cost, with density evolution (1-moment model) modeled by a pressure-diffusion equation, where diffusion is caused by charge exchange collisions. Two centered finite difference schemes, a 4th order and a 2nd order direct discretization of the divergence operator, are implemented to study trade-offs between accuracy and stability. Plasma-neutrals coupling is performed using conservative Krook operators to model ionization and recombination sources and sinks. A three-operator, 2nd-order Strang splitting algorithm allows explicit integration, treating the Vlasov plasma, Coulomb collisions, and neutrals independently. To lift the time-step constraints imposed by the diffusive nature of the latter two, a 2nd order RK-Chebyshev (RKC) scheme has been implemented, also allowing the number of steps to be chosen to maximize the possible time-step in the simulations. The implementation has been verified using the method of exact solutions, obtaining the expected order of accuracy in slab, circular and toroidal geometries, and first blob simulations are performed.
References
[1] D. Michels et al., Physics of Plasmas 29, 032307 (2022)
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