A third-order compact gas-kinetic scheme on unstructured meshes for compressible Navier-Stokes solutions

In this paper, for the first time a third-order compact gas-kinetic scheme is proposed on unstructured meshes for the compressible viscous flow computations. The possibility to design such a third-order compact scheme is due to the high-order gas evolution model, where a time-dependent gas distribution function at cell interface not only provides the fluxes across a cell interface, but also presents a time accurate solution for flow variables at cell interface. As a result, both cell averaged and cell interface flow variables can be used for the initial data reconstruction at the beginning of next time step. A weighted least-square procedure has been used for the initial reconstruction. Therefore, a compact third-order gas-kinetic scheme with the involvement of neighboring cells only can be developed on unstructured meshes. In comparison with other conventional high-order schemes, the current method avoids the Gaussian point integration for numerical fluxes along a cell interface and the multi-stage Runge-Kutta method for temporal accuracy. The third-order compact scheme is numerically stable under CFL condition CFL ź 0.5 . Due to its multidimensional gas-kinetic formulation and the coupling of inviscid and viscous terms, even with unstructured meshes, the boundary layer solution and vortex structure can be accurately captured by the current scheme. At the same time, the compact scheme can capture strong shocks as well. A compact third-order gas-kinetic scheme is proposed on unstructured meshes for compressible viscous flow computations.Due to the high-order gas evolution model, both cell averaged values and point-wise values at cell interfaces among neighboring cells can be used for the reconstruction.Both smooth viscous flow solutions and strong shock interaction can be captured accurately by the compact scheme.

[1]  Kun Xu,et al.  The kinetic scheme for the full-Burnett equations , 2004 .

[2]  Yue-Hong Qian,et al.  Implicit gas-kinetic BGK scheme with multigrid for 3D stationary transonic high-Reynolds number flows , 2012 .

[3]  Song Jiang,et al.  An asymptotic preserving unified gas kinetic scheme for gray radiative transfer equations , 2015, J. Comput. Phys..

[4]  Song Fu,et al.  A high-order gas-kinetic Navier-Stokes flow solver , 2010, J. Comput. Phys..

[5]  Kun Xu,et al.  A gas-kinetic BGK scheme for the Navier-Stokes equations and its connection with artificial dissipation and Godunov method , 2001 .

[6]  O. Friedrich,et al.  Weighted Essentially Non-Oscillatory Schemes for the Interpolation of Mean Values on Unstructured Grids , 1998 .

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

[8]  Domenic D'Ambrosio,et al.  Numerical Instablilities in Upwind Methods: Analysis and Cures for the “Carbuncle” Phenomenon , 2001 .

[9]  Kun Xu,et al.  A Compact Third-order Gas-kinetic Scheme for Compressible Euler and Navier-Stokes Equations , 2014, 1412.4489.

[10]  Christian Tenaud,et al.  High order one-step monotonicity-preserving schemes for unsteady compressible flow calculations , 2004 .

[11]  Michael Dumbser,et al.  Quadrature-free non-oscillatory finite volume schemes on unstructured meshes for nonlinear hyperbolic systems , 2007, J. Comput. Phys..

[12]  Kyu Hong Kim,et al.  Accurate, efficient and monotonic numerical methods for multi-dimensional compressible flows Part II: Multi-dimensional limiting process , 2005 .

[13]  Kun Xu,et al.  A unified gas-kinetic scheme for continuum and rarefied flows IV: Full Boltzmann and model equations , 2011, J. Comput. Phys..

[14]  Luc Mieussens,et al.  On the asymptotic preserving property of the unified gas kinetic scheme for the diffusion limit of linear kinetic models , 2013, J. Comput. Phys..

[15]  Rémi Abgrall,et al.  On essentially non-oscillatory schemes on unstructured meshes: analysis and implementation , 1994 .

[16]  Chongam Kim,et al.  Accurate, efficient and monotonic numerical methods for multi-dimensional compressible flows Part I Spatial discretization , 2005 .

[17]  Kun Xu,et al.  A high-order multidimensional gas-kinetic scheme for hydrodynamic equations , 2013 .

[18]  T. G. Cowling,et al.  The mathematical theory of non-uniform gases : notes added in 1951 , 1951 .

[19]  Kun Xu,et al.  Comparison of Fifth-Order WENO Scheme and Finite Volume WENO-Gas-Kinetic Scheme for Inviscid and Viscous Flow Simulation , 2013 .

[20]  P. Frederickson,et al.  Higher order solution of the Euler equations on unstructured grids using quadratic reconstruction , 1990 .

[21]  P. Bhatnagar,et al.  A Model for Collision Processes in Gases. I. Small Amplitude Processes in Charged and Neutral One-Component Systems , 1954 .

[22]  Zhaoli Guo,et al.  Discrete unified gas kinetic scheme for all Knudsen number flows: low-speed isothermal case. , 2013, Physical review. E, Statistical, nonlinear, and soft matter physics.

[23]  Chi-Wang Shu,et al.  Efficient Implementation of Weighted ENO Schemes , 1995 .

[24]  Sharath S. Girimaji,et al.  WENO-enhanced gas-kinetic scheme for direct simulations of compressible transition and turbulence , 2013, J. Comput. Phys..

[25]  Kun Xu,et al.  Direct modeling for computational fluid dynamics , 2015, Acta Mechanica Sinica.

[26]  C. Ollivier-Gooch Quasi-ENO Schemes for Unstructured Meshes Based on Unlimited Data-Dependent Least-Squares Reconstruction , 1997 .

[27]  U. Ghia,et al.  High-Re solutions for incompressible flow using the Navier-Stokes equations and a multigrid method , 1982 .

[28]  Chang Liu,et al.  A unified gas-kinetic scheme for continuum and rarefied flows,direct modeling,and full Boltzmann collision term , 2014 .

[29]  J. Remacle,et al.  Shock detection and limiting with discontinuous Galerkin methods for hyperbolic conservation laws , 2004 .