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Positively conservative high-resolution convection schemes for unstructured elements.(English)Zbl 0884.76048

Summary: Despite their geometric flexibility, unstructured mesh schemes for compressible gas dynamics do not usually resolve captured shocks and contact discontinuities as well as corresponding structured mesh schemes. The main reason for this appears to be the difficulty in constructing analogous extensions to higher-order accuracy. This issue is addressed in some detail and a new, compact stencil, maximum limited gradient (MLG) reconstruction technique is presented for unstructured elements. The MLG reconstruction turns out to be a multidimensional analogue of the one-dimensional Superbee slope. We then describe a simple and robust extension to systems of equations, which does not require any diagonalization of flux Jacobian matrices. An application to a blast wave hazard prediction problem is presented using the wave-by-wave extension of the MLG limiter to the Euler equations.

MSC:

76M20 Finite difference methods applied to problems in fluid mechanics
76M25 Other numerical methods (fluid mechanics) (MSC2010)
76N10 Existence, uniqueness, and regularity theory for compressible fluids and gas dynamics

Cite

References:

[1]Harten, J. Comput. Phys. 49 (1983)
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[4]’Unstructured Euler solvers and underlying algorithms for strongly unsteady shocked flows’, in Proc 19th ISSW, Marseille, France, (1993).
[5]and , ’The design and application of upwind schemes on unstructured meshes’, AIAA Paper 89-0366, 1989.
[6]Pan, Int. J. numer. methods fluids 16 pp 1079– (1993) ·Zbl 0780.76062 ·doi:10.1002/fld.1650161204
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[9]Liu, SIAM J. Numer. Anal. 30 pp 701– (1993) ·Zbl 0791.65068 ·doi:10.1137/0730034
[10]’Higher order upwind schemes on unstructured grids for the compressible Euler equations in time dependent geometries in 3D’, Ph.D. Thesis, University of Freiburg, 1994.
[11]and , ’Convergence of higher order finite volume schemes on unstructured grids for scalar conservation laws’, Preprint 1993, SFB256, Bonn, Germany.
[12]and , ’Adaptive finite volume methods for time-dependent PDE’s’, in (ed.), Modelling, Mesh Generation, and Adaptive Numerical Methods for Partial Differential Equations, Springer, Berlin, 1994.
[13]Van Leer, J. Comput. Phys. 32 pp 101– (1979) ·Zbl 1364.65223 ·doi:10.1016/0021-9991(79)90145-1
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[16]Durlofsky, J. Comput. Phys. 98 pp 64– (1992) ·Zbl 0747.65072 ·doi:10.1016/0021-9991(92)90173-V
[17]Numerical Computation of Internal and External Flows, Wiley, New York (1990).
[18]Toro, Shock Waves 4 pp 25– (1994) ·Zbl 0811.76053 ·doi:10.1007/BF01414629
[19]Einfeldt, SIAM J. Numer. Anal. 25 pp 294– (1988) ·Zbl 0642.76088 ·doi:10.1137/0725021
[20]Rivara, Int. J. numer. methods eng. 28 pp 2889– (1989) ·Zbl 0729.65092 ·doi:10.1002/nme.1620281212
[21], , and , ’A temporal refinement algorithm for unstructured mesh methods’, in Proc. ICFD, Oxford 1995, ed. and , Oxford University Press, 1996. ·Zbl 0923.76146
This reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. In some cases that data have been complemented/enhanced by data from zbMATH Open. This attempts to reflect the references listed in the original paper as accurately as possible without claiming completeness or a perfect matching.
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