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High order conservative LDG-IMEX methods for the degenerate nonlinear non-equilibrium radiation diffusion problems

Shaoqin Zheng, Min Tang, Qiang Zhang, Tao Xiong

TL;DR

This work tackles non-equilibrium radiation diffusion modeled by a two-temperature system with stiff source terms and degenerate nonlinear diffusion. It introduces high-order conservative LDG-IMEX methods built on a predictor-corrector framework that uses an auxiliary variable $B=T^4$ to manage stiffness and enforces energy conservation through a conserved quantity $Q=E+T$. The schemes achieve high temporal accuracy (1st–3rd order) while maintaining stability with large time steps, thanks to mild nonlinear solves (via Picard iterations) and linear diffusion augmentation, and they incorporate positivity-preserving and TVB limiters to control oscillations. Numerical experiments in 1D and 2D, including homogeneous and heterogeneous media and Marshak-wave-type problems, demonstrate accurate front propagation, energy conservation, and robustness, with iterations per stage remaining modest. The methods extend naturally to other reaction-diffusion systems and offer a promising path toward efficient, large-scale radiation diffusion simulations.

Abstract

In this paper, we develop a class of high-order conservative methods for simulating non-equilibrium radiation diffusion problems. Numerically, this system poses significant challenges due to strong nonlinearity within the stiff source terms and the degeneracy of nonlinear diffusion terms. Explicit methods require impractically small time steps, while implicit methods, which offer stability, come with the challenge to guarantee the convergence of nonlinear iterative solvers. To overcome these challenges, we propose a predictor-corrector approach and design proper implicit-explicit time discretizations. In the predictor step, the system is reformulated into a nonconservative form and linear diffusion terms are introduced as a penalization to mitigate strong nonlinearities. We then employ a Picard iteration to secure convergence in handling the nonlinear aspects. The corrector step guarantees the conservation of total energy, which is vital for accurately simulating the speeds of propagating sharp fronts in this system. For spatial approximations, we utilize local discontinuous Galerkin finite element methods, coupled with positive-preserving and TVB limiters. We validate the orders of accuracy, conservation properties, and suitability of using large time steps for our proposed methods, through numerical experiments conducted on one- and two-dimensional spatial problems. In both homogeneous and heterogeneous non-equilibrium radiation diffusion problems, we attain a time stability condition comparable to that of a fully implicit time discretization. Such an approach is also applicable to many other reaction-diffusion systems.

High order conservative LDG-IMEX methods for the degenerate nonlinear non-equilibrium radiation diffusion problems

TL;DR

This work tackles non-equilibrium radiation diffusion modeled by a two-temperature system with stiff source terms and degenerate nonlinear diffusion. It introduces high-order conservative LDG-IMEX methods built on a predictor-corrector framework that uses an auxiliary variable to manage stiffness and enforces energy conservation through a conserved quantity . The schemes achieve high temporal accuracy (1st–3rd order) while maintaining stability with large time steps, thanks to mild nonlinear solves (via Picard iterations) and linear diffusion augmentation, and they incorporate positivity-preserving and TVB limiters to control oscillations. Numerical experiments in 1D and 2D, including homogeneous and heterogeneous media and Marshak-wave-type problems, demonstrate accurate front propagation, energy conservation, and robustness, with iterations per stage remaining modest. The methods extend naturally to other reaction-diffusion systems and offer a promising path toward efficient, large-scale radiation diffusion simulations.

Abstract

In this paper, we develop a class of high-order conservative methods for simulating non-equilibrium radiation diffusion problems. Numerically, this system poses significant challenges due to strong nonlinearity within the stiff source terms and the degeneracy of nonlinear diffusion terms. Explicit methods require impractically small time steps, while implicit methods, which offer stability, come with the challenge to guarantee the convergence of nonlinear iterative solvers. To overcome these challenges, we propose a predictor-corrector approach and design proper implicit-explicit time discretizations. In the predictor step, the system is reformulated into a nonconservative form and linear diffusion terms are introduced as a penalization to mitigate strong nonlinearities. We then employ a Picard iteration to secure convergence in handling the nonlinear aspects. The corrector step guarantees the conservation of total energy, which is vital for accurately simulating the speeds of propagating sharp fronts in this system. For spatial approximations, we utilize local discontinuous Galerkin finite element methods, coupled with positive-preserving and TVB limiters. We validate the orders of accuracy, conservation properties, and suitability of using large time steps for our proposed methods, through numerical experiments conducted on one- and two-dimensional spatial problems. In both homogeneous and heterogeneous non-equilibrium radiation diffusion problems, we attain a time stability condition comparable to that of a fully implicit time discretization. Such an approach is also applicable to many other reaction-diffusion systems.
Paper Structure (15 sections, 1 theorem, 62 equations, 16 figures, 5 tables, 1 algorithm)

This paper contains 15 sections, 1 theorem, 62 equations, 16 figures, 5 tables, 1 algorithm.

Key Result

Theorem 1

The matrix $A(\tilde{U}^{(i)})$ in algebraic system is an $\mathbf{M}$ matrix for piecewise constant $\mathcal{Q}^0$ finite elements if $\tilde{U}^{(i)} \geq 0$.

Figures (16)

  • Figure 4.1: The numerical results for Example \ref{['test_limiters']} with $\kappa=0$. 1st, 2nd, and 3rd order schemes are used. "WL’': with limiters, "NL'’: without limiters. "ref" represents the reference solutions. Top row: $N=64$; Bottom row: $N=128$. Left column: radiation temperature $T_r$; Right column: material temperature $T$. $t=1$, $\Delta t = \frac{h}{5}.$
  • Figure 4.2: The numerical results for Example \ref{['test_limiters']} with $\kappa=0.1,$ and $N=128$. 1st, 2nd, and 3rd order schemes are used. "WL’' : with limiters, "NL'’: without limiters. "ref" represents the reference solutions. Top row: $N=64$; Bottom row: $N=128$. Left column: radiation temperature $T_r$; Right column: material temperature $T$. $t=0.5$, $\Delta t = \frac{h}{5}.$
  • Figure 4.3: The numerical results for Example \ref{['exp_conservation']} with $\kappa=0.5$ and $N=128$. 1st, 2nd, and 3rd order schemes are used. "c": with a conservation corrector step; "nc": without a corrector step. Left: initial values; Right: time evolution of conservation errors. $\Delta t = \frac{1}{30}h$ for "2nd, nc", $\Delta t = \frac{1}{50}h$ for "3rd, nc" and $\Delta t = \frac{1}{5}h$ for all others.
  • Figure 4.4: The numerical results for Example \ref{['exp_conservation']} with $\kappa=0.5$ and $N=128$. 1st, 2nd, and 3rd order schemes are used. "c": with a conservation corrector step; "nc": without a corrector step. Left: radiation energy $E$; Right: material temperature $T$. $\Delta t = \frac{1}{30}h$ for "2nd, nc", $\Delta t = \frac{1}{50}h$ for "3rd, nc" and $\Delta t = \frac{1}{5}h$ for all others.
  • Figure 4.5: The numerical results of 1st, 2nd, and 3rd order schemes for Example \ref{['Marshak_homo_problem']} with $\kappa=0,$$\Delta t = \frac{h}{5},$ time $t=1$ and $t=2.$ "ref" represents the reference solutions. Top: $N=64$; Bottom: $N=128$. Left column: radiation temperature $T_r$; Right column: material temperature $T$.
  • ...and 11 more figures

Theorems & Definitions (1)

  • Theorem 1