By Joseph L. Steger (auth.), M. Y. Hussaini, A. Kumar, M. D. Salas (eds.)
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In Laminar and Turbulent flows. C. G. Habashi, H. Hafez eds. Pinneridge Press, 1987.  J. Peraire, J. Peiro, L. Formaggia, K. Morgan, O. Zienkiewicz: Finite Element Euler Computations in three dimensions. Int. J. Numer. Meth. in Eng. 26: 2135-2159, 1988. J. Baker: Automatic mesh generation for complex three dimensional regions using a constrained Delaunay triangulation, Eng. Compo 5: 161-175, 1989. , Hecht, F. , Saltel, E. 1990. Automatic 3D Mesh Generation with Prescribed Mesh Boundaries. IEEE Trans.
Nicolaides  showed that Voronoi meshes are well adapted to flux based Finite Volume Methods because of the orthogonality be- 41 tween the Voronoi polygons and the edges of the mesh. In particular it solves the problem of how to apply boundary conditions when the viscous terms are present. T are not known, it is not obvious how to impose the boundary condition. In  convergence is shown (for the incompressible NavierStokes equations also) if one proceeds as follows. n. T = u x n is done through a given boundary integral in the formulation.
Composite meshes have been used at Boeing (YoUng et al ) where the matrices are stored only in regions where the mesh is not structured. Theoretical studies (Scott) show that multigrids can be used even if the grids are not imbeded into one another. Only parallel computing on machines like the eM (see Fezoui  for example) are more difficult with unstructured meshes, so far. 40 3. 1 Flux based methods. The Flux based Finite volume method is most successful for the discretization of (1) on unstructured meshes.
Algorithmic Trends in Computational Fluid Dynamics by Joseph L. Steger (auth.), M. Y. Hussaini, A. Kumar, M. D. Salas (eds.)