One-sweep moment-based semi-implicit-explicit integration for gray thermal radiation transport
Thermal radiation transport (TRT) is a time dependent, high dimensional partial integro-differential equation. In practical applications such as inertial confinement fusion, TRT is coupled to other physics such as hydrodynamics, plasmas, etc., and the timescales one is interested in capturing are of...
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Veröffentlicht in: | Journal of Computational Physics 2024-11, Vol.517, p.113349, Article 113349 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Thermal radiation transport (TRT) is a time dependent, high dimensional partial integro-differential equation. In practical applications such as inertial confinement fusion, TRT is coupled to other physics such as hydrodynamics, plasmas, etc., and the timescales one is interested in capturing are often much slower than the radiation timescale. As a result, TRT is treated implicitly, and due to its stiffness and high dimensionality, is often a dominant computational cost in multiphysics simulations. Here we develop a new approach for implicit-explicit (IMEX) integration of gray TRT in the deterministic SN setting, which requires only one sweep per stage, with the simplest first-order method requiring only one sweep per time step. The partitioning of equations is done via a moment-based high-order low-order formulation of TRT, where the streaming operator and first two moments are used to capture the asymptotic stiff regimes of the streaming limit and diffusion limit. Absorption-reemission is treated explicitly, and although stiff, is sufficiently damped by the implicit solve that we achieve stable accurate time integration without incorporating the coupling of the high order and low order equations implicitly. Due to nonlinear coupling of the high-order and low-order equations through temperature-dependent opacities, to facilitate IMEX partitioning and higher-order methods, we use a semi-implicit integration approach amenable to nonlinear partitions. Results are demonstrated on thick Marshak and crooked pipe benchmark problems, demonstrating orders of magnitude improvement in accuracy and wallclock compared with the standard first-order implicit integration typically used.
•Implicit-explicit Runge-Kutta integration for SN discretizations of gray thermal radiation transport.•One implicit sweep and one implicit low-order solve per time step/stage.•2nd-order accuracy observed on stiff thick Marshak and crooked pipe benchmark problems.•Orders of magnitude improvement in accuracy and wallclock time compared with standard first-order implicit integration. |
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ISSN: | 0021-9991 |
DOI: | 10.1016/j.jcp.2024.113349 |