A nominally second-order accurate finite volume cell-centered scheme for anisotropic diffusion on two-dimensional unstructured grids

In this paper, we describe a second-order accurate cell-centered finite volume method for solving anisotropic diffusion on two-dimensional unstructured grids. The resulting numerical scheme, named CCLAD (Cell-Centered LAgrangian Diffusion), is characterized by a local stencil and cell-centered unkno...

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Bibliographic Details
Published in:Journal of computational physics 2012-03, Vol.231 (5), p.2259-2299
Main Authors: Maire, Pierre-Henri, Breil, Jérôme
Format: Article
Language:English
Subjects:
Anisotropic diffusion
Anisotropy
Approximation
Cell-centered scheme
Computational techniques
Cylindrical geometry
Diffusion
Exact sciences and technology
Fluxes
Gas dynamics
Isotropic diffusion
Mathematical analysis
Mathematical methods in physics
Mathematical models
Physics
Second-order accurate finite volume method
Two dimensional
Two-dimensional unstructured grid
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Summary:In this paper, we describe a second-order accurate cell-centered finite volume method for solving anisotropic diffusion on two-dimensional unstructured grids. The resulting numerical scheme, named CCLAD (Cell-Centered LAgrangian Diffusion), is characterized by a local stencil and cell-centered unknowns. It is devoted to the resolution of diffusion equation on distorted grids in the context of Lagrangian hydrodynamics wherein a strong coupling occurs between gas dynamics and diffusion. The space discretization relies on the introduction of two half-edge normal fluxes and two half-edge temperatures per cell interface using the partition of each cell into sub-cells. For each cell, the two half-edge normal fluxes attached to a node are expressed in terms of the half-edge temperatures impinging at this node and the cell-centered temperature. This local flux approximation can be derived through the use of either a sub-cell variational formulation or a finite difference approximation, leading to the two variants CCLADS and CCLADNS. The elimination of the half-edge temperatures is performed locally at each node by solving a small linear system which is obtained by enforcing the continuity condition of the normal heat flux across sub-cell interface impinging at the node. The accuracy and the robustness of the present scheme is assessed by means of various numerical test cases.
ISSN:0021-9991
1090-2716
DOI:10.1016/j.jcp.2011.11.029