A very-high-order TENO scheme for all-speed gas dynamics and turbulence
暂无分享,去创建一个
[1] P. Woodward,et al. The Piecewise Parabolic Method (PPM) for Gas Dynamical Simulations , 1984 .
[2] D. Pullin,et al. Hybrid tuned center-difference-WENO method for large eddy simulations in the presence of strong shocks , 2004 .
[3] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[4] G. A. Gerolymos,et al. Very-high-order weno schemes , 2009, J. Comput. Phys..
[5] H. Huynh,et al. Accurate Monotonicity-Preserving Schemes with Runge-Kutta Time Stepping , 1997 .
[6] Lin Fu,et al. A low-dissipation finite-volume method based on a new TENO shock-capturing scheme , 2019, Comput. Phys. Commun..
[7] Nikolaus A. Adams,et al. A new class of adaptive high-order targeted ENO schemes for hyperbolic conservation laws , 2018, J. Comput. Phys..
[8] Chi-Wang Shu,et al. Strong Stability-Preserving High-Order Time Discretization Methods , 2001, SIAM Rev..
[9] Nikolaus A. Adams,et al. An adaptive central-upwind weighted essentially non-oscillatory scheme , 2010, J. Comput. Phys..
[10] Nikolaus A. Adams,et al. An adaptive local deconvolution method for implicit LES , 2005, J. Comput. Phys..
[11] S. Orszag,et al. Small-scale structure of the Taylor–Green vortex , 1983, Journal of Fluid Mechanics.
[12] Chi-Wang Shu,et al. Runge-Kutta Discontinuous Galerkin Method Using WENO Limiters , 2005, SIAM J. Sci. Comput..
[13] Sergio Pirozzoli,et al. Numerical Methods for High-Speed Flows , 2011 .
[14] Nikolaus A. Adams,et al. A physically consistent weakly compressible high-resolution approach to underresolved simulations of incompressible flows , 2013 .
[15] Chi-Wang Shu,et al. Anti-diffusive flux corrections for high order finite difference WENO schemes , 2005 .
[16] Stefan Hickel,et al. Subgrid-scale modeling for implicit large eddy simulation of compressible flows and shock-turbulence interaction , 2014 .
[17] Xiangxiong Zhang,et al. Positivity-preserving high order finite difference WENO schemes for compressible Euler equations , 2012, J. Comput. Phys..
[18] Xiangxiong Zhang,et al. On positivity-preserving high order discontinuous Galerkin schemes for compressible Euler equations on rectangular meshes , 2010, J. Comput. Phys..
[19] Soshi Kawai,et al. Assessment of localized artificial diffusivity scheme for large-eddy simulation of compressible turbulent flows , 2010, J. Comput. Phys..
[20] Nikolaus A. Adams,et al. A family of high-order targeted ENO schemes for compressible-fluid simulations , 2016, J. Comput. Phys..
[21] V. Gregory Weirs,et al. A bandwidth-optimized WENO scheme for the effective direct numerical simulation of compressible turbulence , 2006, J. Comput. Phys..
[22] Sergio Pirozzoli,et al. On the spectral properties of shock-capturing schemes , 2006, J. Comput. Phys..
[23] Nikolaus A. Adams,et al. Positivity-preserving method for high-order conservative schemes solving compressible Euler equations , 2013, J. Comput. Phys..
[24] Chi-Wang Shu,et al. On positivity preserving finite volume schemes for Euler equations , 1996 .
[25] Yuan Liu,et al. A Robust Reconstruction for Unstructured WENO Schemes , 2013, J. Sci. Comput..
[26] Björn Sjögreen,et al. Numerical dissipation control in high order shock-capturing schemes for LES of low speed flows , 2016, J. Comput. Phys..
[27] J. P. Boris,et al. New insights into large eddy simulation , 1992 .
[28] Lin Fu,et al. A Targeted ENO Scheme as Implicit Model for Turbulent and Genuine Subgrid Scales , 2019, Communications in Computational Physics.
[29] Raphaël Loubère,et al. A subcell remapping method on staggered polygonal grids for arbitrary-Lagrangian-Eulerian methods , 2005 .
[30] Wai-Sun Don,et al. An improved weighted essentially non-oscillatory scheme for hyperbolic conservation laws , 2008, J. Comput. Phys..
[31] Eleuterio F. Toro,et al. Finite-volume WENO schemes for three-dimensional conservation laws , 2004 .
[32] Klaus A. Hoffmann,et al. Minimizing errors from linear and nonlinear weights of WENO scheme for broadband applications with shock waves , 2013, J. Comput. Phys..
[33] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[34] S. Osher,et al. Uniformly high order accurate essentially non-oscillatory schemes, 111 , 1987 .
[35] Dimitris Drikakis,et al. On the implicit large eddy simulations of homogeneous decaying turbulence , 2007, J. Comput. Phys..
[36] Lei Luo,et al. A sixth order hybrid finite difference scheme based on the minimized dispersion and controllable dissipation technique , 2014, J. Comput. Phys..
[37] Soshi Kawai,et al. Localized artificial diffusivity scheme for discontinuity capturing on curvilinear meshes , 2008, J. Comput. Phys..
[38] Yuxin Ren,et al. A characteristic-wise hybrid compact-WENO scheme for solving hyperbolic conservation laws , 2003 .
[39] P. Woodward,et al. The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .
[40] Ivan Fedioun,et al. Comparison of improved finite-difference WENO schemes for the implicit large eddy simulation of turbulent non-reacting and reacting high-speed shear flows , 2014 .
[41] S. Osher,et al. Weighted essentially non-oscillatory schemes , 1994 .
[42] Nikolaus A. Adams,et al. Targeted ENO schemes with tailored resolution property for hyperbolic conservation laws , 2017, J. Comput. Phys..
[43] Nikolaus A. Adams,et al. Scale separation for implicit large eddy simulation , 2011, J. Comput. Phys..
[44] Yong-Tao Zhang,et al. Resolution of high order WENO schemes for complicated flow structures , 2003 .
[45] Sergio Pirozzoli,et al. Conservative Hybrid Compact-WENO Schemes for Shock-Turbulence Interaction , 2002 .
[46] Wai-Sun Don,et al. High order weighted essentially non-oscillatory WENO-Z schemes for hyperbolic conservation laws , 2011, J. Comput. Phys..
[47] Andrew W. Cook,et al. Artificial Fluid Properties for Large-Eddy Simulation of Compressible Turbulent Mixing , 2007 .
[48] Chi-Wang Shu,et al. TVB Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws III: one-dimensional systems , 1989 .
[49] Nail K. Yamaleev,et al. A systematic methodology for constructing high-order energy stable WENO schemes , 2009, J. Comput. Phys..
[50] F. Nicoud,et al. Large-Eddy Simulation of the Shock/Turbulence Interaction , 1999 .
[51] Chi-Wang Shu,et al. Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .
[52] Parviz Moin,et al. Assessment of high-resolution methods for numerical simulations of compressible turbulence with shock waves , 2010, J. Comput. Phys..
[53] Bruno Costa,et al. An improved WENO-Z scheme , 2016, J. Comput. Phys..
[54] J. M. Powers,et al. Mapped weighted essentially non-oscillatory schemes: Achieving optimal order near critical points , 2005 .