A Direct ALE Multi-Moment Finite Volume Scheme for the Compressible Euler Equations

A direct Arbitrary Lagrangian Eulerian (ALE) method based on multi-moment finite volume scheme is developed for the Euler equations of compressible gas in 1D and 2D space. Both the volume integrated average (VIA) and the point values (PV) at cell vertices, which are used for high-order reconstructions, are treated as the computational variables and updated simultaneously by numerical formulations in integral and differential forms respectively. The VIAs of the conservative variables are solved by a finite volume method in the integral form of the governing equations to ensure the numerical conservativeness; whereas, the governing equations of differential form are solved for the PVs of the primitive variables to avoid the additional source terms generated from moving mesh, which largely simplifies the solution procedure. Numerical tests in both 1D and 2D are presented to demonstrate the performance of the proposed ALE scheme. The present multi-moment finite volume formulation consistent with moving meshes provides a high-order and efficient ALE computational model for compressible flows. AMS subject classifications: 76M12, 76N15, 35L55

[1]  Xiaodong Ren,et al.  A multi-dimensional high-order DG-ALE method based on gas-kinetic theory with application to oscillating bodies , 2016, J. Comput. Phys..

[2]  Guangwei Yuan,et al.  A robust and contact resolving Riemann solver on unstructured mesh, Part I, Euler method , 2014, J. Comput. Phys..

[3]  Feng Xiao,et al.  A hybrid pressure-density-based Mach uniform algorithm for 2D Euler equations on unstructured grids by using multi-moment finite volume method , 2017, J. Comput. Phys..

[4]  Michael Dumbser,et al.  A direct Arbitrary-Lagrangian-Eulerian ADER-WENO finite volume scheme on unstructured tetrahedral meshes for conservative and non-conservative hyperbolic systems in 3D , 2014, J. Comput. Phys..

[5]  Rémi Abgrall,et al.  A Cell-Centered Lagrangian Scheme for Two-Dimensional Compressible Flow Problems , 2007, SIAM J. Sci. Comput..

[6]  V. Guinot Approximate Riemann Solvers , 2010 .

[7]  Feng Xiao,et al.  Two and three dimensional multi-moment finite volume solver for incompressible Navier–Stokes equations on unstructured grids with arbitrary quadrilateral and hexahedral elements , 2014 .

[8]  C. W. Hirt,et al.  An Arbitrary Lagrangian-Eulerian Computing Method for All Flow Speeds , 1997 .

[9]  Z. Wang,et al.  Spectral (Finite) Volume Method for Conservation Laws on Unstructured Grids , 2002 .

[10]  Feng Xiao,et al.  High order multi-moment constrained finite volume method. Part I: Basic formulation , 2009, J. Comput. Phys..

[11]  T. Yabe,et al.  Completely conservative and oscillationless semi-Lagrangian schemes for advection transportation , 2001 .

[12]  P. Roe Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .

[13]  Chi-Wang Shu Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .

[14]  Jaime Peraire,et al.  Discontinuous Galerkin Solution of the Navier-Stokes Equations on Deformable Domains , 2007 .

[15]  P. Woodward,et al.  The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .

[16]  Pierre-Henri Maire,et al.  A high-order cell-centered Lagrangian scheme for two-dimensional compressible fluid flows on unstructured meshes , 2009, J. Comput. Phys..

[17]  T. Yabe,et al.  The constrained interpolation profile method for multiphase analysis , 2001 .

[18]  Rainald Löhner,et al.  On the computation of multi-material flows using ALE formulation , 2004 .

[19]  Pierre-Henri Maire,et al.  Multi-scale Godunov-type method for cell-centered discrete Lagrangian hydrodynamics , 2009, J. Comput. Phys..

[20]  P. Thomas,et al.  Geometric Conservation Law and Its Application to Flow Computations on Moving Grids , 1979 .

[21]  Jean-Michel Ghidaglia,et al.  A multi-dimensional finite volume cell-centered direct ALE solver for hydrodynamics , 2016, J. Comput. Phys..

[22]  S. Osher,et al.  Uniformly high order accuracy essentially non-oscillatory schemes III , 1987 .

[23]  Michael Dumbser,et al.  Direct Arbitrary-Lagrangian-Eulerian ADER-MOOD finite volume schemes for multidimensional hyperbolic conservation laws , 2015, J. Comput. Phys..

[24]  Feng Xiao,et al.  CIP/multi-moment finite volume method for Euler equations: A semi-Lagrangian characteristic formulation , 2007, J. Comput. Phys..

[25]  Zhi J. Wang,et al.  Spectral (Finite) Volume Method for Conservation Laws on Unstructured Grids. Basic Formulation , 2002 .

[26]  Chongam Kim,et al.  Multi-dimensional limiting process for hyperbolic conservation laws on unstructured grids , 2005, J. Comput. Phys..

[27]  Chi-Wang Shu,et al.  TVB Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws III: one-dimensional systems , 1989 .

[28]  F. Xiao,et al.  A finite volume multi-moment method with boundary variation diminishing principle for Euler equation on three-dimensional hybrid unstructured grids , 2017 .

[29]  Guangwei Yuan,et al.  A robust and contact resolving Riemann solver on unstructured mesh, Part II, ALE method , 2014, J. Comput. Phys..

[30]  Feng Xiao,et al.  A multi-moment constrained finite volume method on arbitrary unstructured grids for incompressible flows , 2016, J. Comput. Phys..

[31]  F. Xiao,et al.  Multimoment Finite Volume Solver for Euler Equations on Unstructured Grids , 2017 .

[32]  Feng Xiao,et al.  A multi-moment finite volume method for incompressible Navier-Stokes equations on unstructured grids: Volume-average/point-value formulation , 2014, J. Comput. Phys..

[33]  Dimitri J. Mavriplis,et al.  On the geometric conservation law for high-order discontinuous Galerkin discretizations on dynamically deforming meshes , 2008, J. Comput. Phys..

[34]  Michael Dumbser,et al.  On Arbitrary-Lagrangian-Eulerian One-Step WENO Schemes for Stiff Hyperbolic Balance Laws , 2012, 1207.6407.

[35]  Rémi Abgrall,et al.  A discontinuous Galerkin discretization for solving the two-dimensional gas dynamics equations written under total Lagrangian formulation on general unstructured grids , 2014, J. Comput. Phys..

[36]  Wang Chi-Shu,et al.  Essentially Non-Oscillatory and Weighted Essentially Non-Oscillatory Schemes for Hyperbolic Conservation Laws , 1997 .

[37]  R. LeVeque Finite Volume Methods for Hyperbolic Problems: Characteristics and Riemann Problems for Linear Hyperbolic Equations , 2002 .

[38]  Chi-Wang Shu,et al.  TVB Runge-Kutta local projection discontinuous galerkin finite element method for conservation laws. II: General framework , 1989 .

[39]  Chi-Wang Shu,et al.  A high order ENO conservative Lagrangian type scheme for the compressible Euler equations , 2007, J. Comput. Phys..

[40]  P. Lax,et al.  On Upstream Differencing and Godunov-Type Schemes for Hyperbolic Conservation Laws , 1983 .

[41]  E. Toro Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .

[42]  Changfu You,et al.  High-order ALE method for the Navier–Stokes equations on a moving hybrid unstructured mesh using flux reconstruction method , 2013 .

[43]  S. Osher,et al.  Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .

[44]  Juan Cheng,et al.  A Third Order Conservative Lagrangian Type Scheme on Curvilinear Meshes for the Compressible Euler Equations , 2008 .

[45]  Claus-Dieter Munz,et al.  On Godunov-type schemes for Lagrangian gas dynamics , 1994 .