A positive and asymptotic preserving scheme for the linear transport equation on 2D unstructured meshes

In this paper, we propose a finite volume scheme for the linear transport equation in two space dimensions. This scheme is based on a second order upwind flux where the velocity is modified so as to recover the correct diffusion limit. A partially implicit time discretization is used. This allows to have good properties while keeping the computational cost per iteration very low. The resulting scheme is asymptotic preserving , positive under a classical CFL condition, conservative and second order consistent in all the regimes. These properties are valid on general unstructured meshes and the computational cost is similar to an explicit scheme. Eventually, the extension of this scheme to 3 D unstructured meshes is straightforward and its properties remain valid.

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Publication Details

Journal
Computers & Mathematics with Applications
Published
2026-01-29
DOI
https://doi.org/10.1016/j.camwa.2026.01.023
Primary Topic
Advanced Numerical Methods in Computational Mathematics
Type
article
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article

A positive and asymptotic preserving scheme for the linear transport equation on 2D unstructured meshes

Clément Lasuen
Computers & Mathematics with Applications
Advanced Numerical Methods in Computational Mathematics
article

A positive and asymptotic preserving scheme for the linear transport equation on 2D unstructured meshes

Clément Lasuen
article en

Abstract

In this paper, we propose a finite volume scheme for the linear transport equation in two space dimensions. This scheme is based on a second order upwind flux where the velocity is modified so as to recover the correct diffusion limit. A partially implicit time discretization is used. This allows to have good properties while keeping the computational cost per iteration very low. The resulting scheme is asymptotic preserving , positive under a classical CFL condition, conservative and second order consistent in all the regimes. These properties are valid on general unstructured meshes and the computational cost is similar to an explicit scheme. Eventually, the extension of this scheme to 3 D unstructured meshes is straightforward and its properties remain valid.

Computers & Mathematics with ApplicationsVol. 207
Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR), CEA DAM Île-de-France (FR)
Openalex Percentile: Top 72%
Advanced Numerical Methods in Computational Mathematics
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