Mimetic finite difference operators for second-order tensors on unstructured grids
β Scribed by J.C. Campbell; J.M. Hyman; M.J. Shashkov
- Publisher
- Elsevier Science
- Year
- 2002
- Tongue
- English
- Weight
- 899 KB
- Volume
- 44
- Category
- Article
- ISSN
- 0898-1221
No coin nor oath required. For personal study only.
β¦ Synopsis
We use the support operators method to derive discrete approximations for tile gradient of a vector and divergence of a tensor on unstructured grids in two dimensions. These discrete operators satisfy discrete analogs of the integral identities of the differential operators on unstructured grids where vector functions are defined at the grid points, and tensor fimctions are defined as tangential projections to the zone edges, or as normal projections to the median mesh. We evaluate the accuracy of the discrete operators by determining the order of convergence of the truncation error on structured and unstructured grids, and show that the truncation error of the method is between first and second order depending on the smoothness of tile grid. In a test problem on a highly nonuniform grid, we confirm that the convergence rate is between first and second order.
π SIMILAR VOLUMES
This paper describes a finite volume discretization method to compute steady, twodimensional incompressible viscous recirculating flows using hybrid unstructured meshes, composed of triangles and quadrilaterals. However, the proposed formulation is not restricted to these topologies. The new method
A new second-order time-accurate fractional-step method for solving unsteady incompressible Navier-Stokes equations on hybrid unstructured grids is presented. The nonstaggered grid method, originally developed by Chow (1983, AIAA J. 21, 1525) for steady flow and further extended by Zang et al. (199
A second-order-accurate finite difference discretization of the incompressible Navier-Stokes is presented that discretely conserves mass, momentum, and kinetic energy (in the inviscid limit) in space and time. The method is thus completely free of numerical dissipation and potentially well suited to
Diagonal tensor flux approximations are commonly used in fluid dynamics. This approximation introduces an O(1) error in flux whenever the coordinate system is nonaligned with the principal axes of the tensor which is particularly common when employing curvilinear gridding. In general a consistent fu