Application of the LS-STAG Immersed Boundary/Cut-Cell Method to Viscoelastic Flow Computations - Université de Lorraine Access content directly
Journal Articles Communications in Computational Physics Year : 2016

Application of the LS-STAG Immersed Boundary/Cut-Cell Method to Viscoelastic Flow Computations

Abstract

This paper presents the extension of a well-established Immersed Boundary (IB)/cut-cell method, the LS-STAG method (Y. Cheny & O. Botella, J. Comput. Phys. Vol. 229, 1043-1076, 2010), to viscoelastic flow computations in complex geometries. We recall that for Newtonian flows, the LS-STAG method is based on the finite-volume method on staggered grids, where the IB boundary is represented by its level-set function. The discretization in the cut-cells is achieved by requiring that global conservation properties equations be satisfied at the discrete level, resulting in a stable and accurate method and, thanks to the level-set representation of the IB boundary, at low computational costs. In the present work, we consider a general viscoelastic tensorial equation whose particular cases recover well-known constitutive laws such as the Oldroyd-B, White-Metzner and Giesekus models. Based on the LS-STAG discretization of the Newtonian stresses in the cut-cells, we have achieved a compatible velocity-pressure-stress discretization that prevents spurious oscillations of the stress tensor. Applications to popular benchmarks for viscoelastic fluids are presented: the four-to-one abrupt planar contraction flows with sharp and rounded re-entrant corners, for which experimental and numerical results are available. The results show that the LS-STAG method demonstrates an accuracy and robustness comparable to body-fitted methods.
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Dates and versions

hal-01408974 , version 1 (05-12-2016)

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Olivier Botella, Yoann Cheny, Farhad Nikfarjam, Marcela Stoica. Application of the LS-STAG Immersed Boundary/Cut-Cell Method to Viscoelastic Flow Computations. Communications in Computational Physics, 2016, 20 (04), pp.870 - 901. ⟨10.4208/cicp.080615.010216a⟩. ⟨hal-01408974⟩
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