2004
DOI: 10.1016/j.jcp.2004.02.016
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Mimetic finite difference methods for diffusion equations on non-orthogonal non-conformal meshes

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Cited by 95 publications
(71 citation statements)
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“…For problem (1.1), the mimetic technique uses discrete flux G and divergence DIV operators for the continuum operators −Kgrad and div, respectively, which are adjoint to each other, i.e., G = DIV * . It is straightforward to extend the MFD method to locally refined meshes with hanging nodes [16], unstructured three-dimensional meshes composed of hexahedra, tetrahedra, and any cell type having three faces intersecting at each vertex.…”
Section: Introductionmentioning
confidence: 99%
“…For problem (1.1), the mimetic technique uses discrete flux G and divergence DIV operators for the continuum operators −Kgrad and div, respectively, which are adjoint to each other, i.e., G = DIV * . It is straightforward to extend the MFD method to locally refined meshes with hanging nodes [16], unstructured three-dimensional meshes composed of hexahedra, tetrahedra, and any cell type having three faces intersecting at each vertex.…”
Section: Introductionmentioning
confidence: 99%
“…Although we were at first surprised by the second order accurate numerical results, [52] and the references therein indicate the plausibility of this. In fact, it was [52] (and personal communications with the authors) that directly led to our first attempts to define unique pressure gradients on cell faces that could be used for both the large cell and all the small cells incident on a particular face.…”
Section: Second Order Accuracy On Octreesmentioning
confidence: 86%
“…In fact, it was [52] (and personal communications with the authors) that directly led to our first attempts to define unique pressure gradients on cell faces that could be used for both the large cell and all the small cells incident on a particular face.…”
Section: Second Order Accuracy On Octreesmentioning
confidence: 99%
“…Note that if one applies weak condition for the currents and strong conditions for the scalar fluxes, it results in interface relationships that are not valid for the scalar fluxes varying linearly along cell interfaces [49]. For example, in 2D, if the left face of i-th cell is a common face with the m-th and p-th cells, then we define strong continuity conditions for the normal components of the currents 30) and the weak continuity condition for the face-average scalar fluxes 31) where h iω is the cell-edge length.…”
Section: Interface Continuity Conditionsmentioning
confidence: 99%