2015
DOI: 10.1016/j.jcp.2015.03.024
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A stable projection method for the incompressible Navier–Stokes equations on arbitrary geometries and adaptive Quad/Octrees

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Cited by 62 publications
(50 citation statements)
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“…We follow [23] in designing our finite volume scheme, and discretize (1) for every mesh K and component i = 1, 2 in the following way: The different equations (4) amount to a nonlinear system that can be written in matrix form (for example K ∇ • u ≈ D • U where D is a divergence matrix). We formally define the gradient matrix as −D t , that is, the discrete gradient is the dual operator of the discrete divergence [22,23,32].…”
Section: Pruningmentioning
confidence: 99%
“…We follow [23] in designing our finite volume scheme, and discretize (1) for every mesh K and component i = 1, 2 in the following way: The different equations (4) amount to a nonlinear system that can be written in matrix form (for example K ∇ • u ≈ D • U where D is a divergence matrix). We formally define the gradient matrix as −D t , that is, the discrete gradient is the dual operator of the discrete divergence [22,23,32].…”
Section: Pruningmentioning
confidence: 99%
“…English et al [2013a;2013b] constructed a nested (Chimera) grid scheme relying on the flexibility of the local Voronoi structure to stitch together the boundaries between regular grids of differing resolutions. Voronoi diagrams have similarly been exploited in computational physics: Guittet et al improved the ghost-fluid method for two-phase Poisson problems by aligning Voronoi faces with the fluid interface [Guittet et al 2015a], and separately used the Voronoi diagram of fluid face midpoints to treat viscosity on non-graded octrees [Guittet et al 2015b]. Fig.…”
Section: Tetrahedralmentioning
confidence: 99%
“…Another option to recover orthogonality would be the Voronoi diagram of the octree cell centers. For non-graded trees this can yield very general unstructured meshes that discard the regularity benefits of the tree structure (see e.g., [Guittet et al 2015b]). While the variety of mesh configurations can naturally be reduced by grading, the Voronoi topology still differs more strongly from the original tree than for the power diagram, even in the simpler 2D setting (see Figure 4(c)).…”
Section: Power Diagram Discretizationmentioning
confidence: 99%
“…The behavior of the fluid is described by the Navier-Stokes equations for incompressible flows. For details the interested reader can also see [20,10].…”
Section: Fsi Problemωmentioning
confidence: 99%