High order ADER schemes for a unified first order hyperbolic formulation of continuum mechanics: Viscous heat-conducting fluids and elastic solids

JOURNAL OF COMPUTATIONAL PHYSICS

卷:314

Article

Dumbser, Michael¹  Peshkov, Ilya²  Romenski, Evgeniy^3,4  Zanotti, Olindo¹ 

[1] Univ Trento, Dept Civil Environm & Mech Engn, Via Mesiano 77, I-38123 Trento, Italy

[2] Univ Pau & Pays Adour, Open & Expt Ctr Heavy Oil, Ave Univ, F-64012 Pau, France

[3] Sobolev Inst Math, 4 Acad Koptyug Ave, Novosibirsk 630090, Russia

[4] Novosibirsk State Univ, 2 Pirogova Str, Novosibirsk 630090, Russia

关键词: ADER-WENO finite volume schemes;    Arbitrary high-order discontinuous Galerkin schemes;    Path-conservative methods and stiff source terms;    Unified first order hyperbolic formulation of nonlinear continuum mechanics;    Fluid mechanics and solid mechanics;    Viscous compressible fluids and elastic solids;   

DOI  :  10.1016/j.jcp.2016.02.015

来源: Elsevier

【 摘 要 】

This paper is concerned with the numerical solution of the unified first order hyperbolic formulation of continuum mechanics recently proposed by Peshkov and Romenski [110], further denoted as HPR model. In that framework, the viscous stresses are computed from the so-called distortion tensor A, which is one of the primary state variables in the proposed first order system. A very important key feature of the HPR model is its ability to describe at the same time the behavior of inviscid and viscous compressible Newtonian and non-Newtonian fluids with heat conduction, as well as the behavior of elastic and visco-plastic solids. Actually, the model treats viscous and inviscid fluids as generalized visco-plastic solids. This is achieved via a stiff source term that accounts for strain relaxation in the evolution equations of A. Also heat conduction is included via a first order hyperbolic system for the thermal impulse, from which the heat flux is computed. The governing PDE system is hyperbolic and fully consistent with the first and the second principle of thermodynamics. It is also fundamentally different from first order Maxwell-Cattaneo-type relaxation models based on extended irreversible thermodynamics. The HPR model represents therefore a novel and unified description of continuum mechanics, which applies at the same time to fluid mechanics and solid mechanics. In this paper, the direct connection between the HPR model and the classical hyperbolic-parabolic Navier-Stokes-Fourier theory is established for the first time via a formal asymptotic analysis in the stiff relaxation limit. From a numerical point of view, the governing partial differential equations are very challenging, since they form a large nonlinear hyperbolic PDE system that includes stiff source terms and non-conservative products. We apply the successful family of one-step ADER-WENO finite volume (FV) and ADER discontinuous Galerkin (DG) finite element schemes to the HPR model in the stiff relaxation limit, and compare the numerical results with exact or numerical reference solutions obtained for the Euler and Navier-Stokes equations. Numerical convergence results are also provided. To show the universality of the HPR model, the paper is rounded-off with an application to wave propagation in elastic solids, for which one only needs to switch off the strain relaxation source term in the governing PDE system. We provide various examples showing that for the purpose of flow visualization, the distortion tensor Aseems to be particularly useful. (C) 2016 The Authors. Published by Elsevier Inc. This is an open access article under the CC BY-NC-ND license

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