Semi-implicit time integration for PN thermal radiative transfer

被引:52
作者
McClarren, Ryan G. [1 ]
Evans, Thomas M. [2 ]
Lowrie, Robert B. [1 ]
Densmore, Jeffery D. [1 ]
机构
[1] Los Alamos Natl Lab, Computat Phys Grp CCS 2, Los Alamos, NM 87545 USA
[2] Oak Ridge Natl Lab, Reactor Anal Grp, Oak Ridge, TN 37831 USA
关键词
thermal radiative transfer; P-N approximation; discontinuous Galerkin; asymptotic diffusion limit;
D O I
10.1016/j.jcp.2008.04.029
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
Implicit time integration involving the solution of large systems of equations is the current paradigm for time-dependent radiative transfer. In this paper we present a semi-implicit, linear discontinuous Galerkin method for the spherical harmonics (P-N) equations for thermal radiative transfer in planar geometry. Our method is novel in that the material coupling terms are treated implicitly (via linearizing the emission source) and the streaming operator is treated explicitly using a second-order accurate Runge-Kutta method. The benefit of this approach is that each time step only involves the solution of equations that are local to each cell. This benefit comes at the cost of having the time step limited by a CFL condition based on the speed of light. To guarantee positivity and avoid artificial oscillations, we use a slope-limiting technique. We present analysis and numerical results that show the method is robust in the diffusion limit when the photon mean-free path is not resolved by the spatial mesh. Also, in the diffusion limit the time step restriction relaxes to a less restrictive explicit diffusion CFL condition. We demonstrate with numerical results that away from the diffusion limit our method demonstrates second-order error convergence as the spatial mesh is refined with a fixed CFL number. (C) 2008 Elsevier Inc. All rights reserved.
引用
收藏
页码:7561 / 7586
页数:26
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