Bulletin of the American Physical Society
77th Annual Meeting of the Division of Fluid Dynamics
Sunday–Tuesday, November 24–26, 2024; Salt Lake City, Utah
Session S01: Poster Session & Refreshment Break (3:47 - 4:45 p.m.)
3:47 PM,
Monday, November 25, 2024
Room: Hall C & Hall 1
Abstract: S01.00035 : Kinetic spectral simulations with implicit-explicit time integration*
Presenter:
Oleksandr Chapurin
(Los Alamos National Laboratory)
Authors:
Oleksandr Chapurin
(Los Alamos National Laboratory)
Oleksandr Koshkarov
(Los Alamos National Laboratory (LANL))
Gian Luca Delzanno
(Los Alamos National Laboratory (LANL))
Cale Harnish
(Los Alamos National Laboratory (LANL))
Alexander A Hrabski
(Los Alamos National Laboratory (LANL))
Salomon Janhunen
(Los Alamos National Laboratory)
Ryan T Wollaeger
(Los Alamos National Laboratory (LANL))
Zach Jibben
(Los Alamos National Laboratory)
Peter T Brady
(Los Alamos National Laboratory (LANL))
Daniel Livescu
(Los Alamos National Laboratory (LANL))
We demonstrate the approach using a kinetic plasma / gas dynamics (GD) solver. For plasmas, we solve the Vlasov-Maxwell (VM) system, where the stiff parts are the particle acceleration term and current source in Maxwell's equation. For GD, we solve the Boltzmann equation with the Bhatnagar-Gross-Krook (BGK) collision operator (stiff term). The spatial dynamics are treated explicitly, thus the procedure ensures locality in physical space for the implicit part, making it particularly efficient where standard physical space domain decomposition is used. Hence, the parallel implementation and preconditioning of implicit solvers are significantly easier than for fully implicit methods which require global nonlinear iterations.
Both GD and VM systems use a spectral expansion in velocity space that leverages Hermite basis (featuring fluid-kinetic coupling that enables its multi-physics application), and finite differences for spatial discretization.For plasma applications, we present the evolution of a large magnetohydrodynamics scale ion-acoustic and Alfvén waves with IMEX time stepping few orders larger than the electron plasma period (the fastest scale). For GD, we recover the correct dynamics of a shock wave propagation (Sedov problem) with IMEX time stepping exceeding ∼104 times the collision period.
*This work was supported by the Laboratory Directed Research and Development Program of Los Alamos National Laboratory under project number 20220104DR. Los Alamos National Laboratory is operated by Triad National Security,LLC, for the National Nuclear Security Administration ofU.S. Department of Energy (Contract No. 89233218CNA000001).Computational resources for the simulations were provided by the Los Alamos National Laboratory Institutional Computing Program.
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