Abstract | ||
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A macroscopic two-fluid model of compressible particle-laden gas flows is considered. The governing equations are discretized by a high-resolution finite element method based on algebraic flux correction. A multidimensional limiter of TVD type is employed to constrain the local characteristic variables for the continuous gas phase and conservative fluxes for a suspension of solid particles. Special emphasis is laid on the efficient computation of steady state solutions at arbitrary Mach numbers. To avoid stability restrictions and convergence problems, the characteristic boundary conditions are imposed weakly and treated in a fully implicit manner. A two-way coupling via the interphase drag force is implemented using operator splitting. The Douglas-Rachford scheme is found to provide a robust treatment of the interphase exchange terms within the framework of a fractional-step solution strategy. Two-dimensional simulation results are presented for a moving shock wave and for a steady nozzle flow. |
Year | DOI | Venue |
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2010 | 10.1016/j.cam.2009.07.041 | J. Computational Applied Mathematics |
Keywords | Field | DocType |
implicit high-resolution schemes,compressible particle-laden gas flow,euler equations,particle-laden gas flows,interphase drag force,tvd type,steady state solution,continuous gas phase,interphase exchange term,unstructured meshes,finite element simulation,characteristic boundary condition,inviscid two-fluid model,local characteristic variable,steady nozzle flow,douglas-rachford scheme,finite element method,drag force,shock wave,steady state,high resolution,euler equation | Drag,Compressibility,Boundary value problem,Mathematical analysis,Finite element method,Compressible flow,Euler equations,Mach number,Mathematics,Moving shock | Journal |
Volume | Issue | ISSN |
233 | 12 | 0377-0427 |
Citations | PageRank | References |
1 | 0.38 | 3 |
Authors | ||
3 |
Name | Order | Citations | PageRank |
---|---|---|---|
Marcel Gurris | 1 | 1 | 0.72 |
Dmitri Kuzmin | 2 | 167 | 23.90 |
S. Turek | 3 | 281 | 38.70 |