Implicit large eddy simulation using the high‐order correction procedure via reconstruction scheme
暂无分享,去创建一个
[1] R. Alexander. Diagonally implicit runge-kutta methods for stiff odes , 1977 .
[2] Rolf Radespiel,et al. Dynamics of laminar separation bubbles at low-Reynolds-number aerofoils , 2009, Journal of Fluid Mechanics.
[3] G. Taylor,et al. Mechanism of the production of small eddies from large ones , 1937 .
[4] P. Moin,et al. Turbulence statistics in fully developed channel flow at low Reynolds number , 1987, Journal of Fluid Mechanics.
[5] John Kim,et al. DIRECT NUMERICAL SIMULATION OF TURBULENT CHANNEL FLOWS UP TO RE=590 , 1999 .
[6] Zhi Jian Wang,et al. A unifying lifting collocation penalty formulation including the discontinuous Galerkin, spectral volume/difference methods for conservation laws on mixed grids , 2009, J. Comput. Phys..
[7] M. Brachet. Direct simulation of three-dimensional turbulence in the Taylor–Green vortex , 1991 .
[8] Nikolaus A. Adams,et al. On implicit subgrid-scale modeling in wall-bounded flows , 2007 .
[9] Alistair Revell,et al. DESider A European Effort on Hybrid RANS-LES Modelling: Results of the European-Union Funded Project, 2004 - 2007 , 2009 .
[10] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[11] Miguel R. Visbal,et al. High-fidelity simulations of moving and flexible airfoils at low Reynolds numbers , 2009 .
[12] Chi-Wang Shu,et al. The Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws. IV. The multidimensional case , 1990 .
[13] Ye Zhou,et al. A note on kinetic energy, dissipation and enstrophy , 1998 .
[14] John H. Kolias,et al. A CONSERVATIVE STAGGERED-GRID CHEBYSHEV MULTIDOMAIN METHOD FOR COMPRESSIBLE FLOWS , 1995 .
[15] U. Piomelli,et al. Subgrid-Scale Models for Compressible Large-Eddy Simulations , 2000 .
[16] Uranga Cabrera,et al. Investigation of transition to turbulence at low Reynolds numbers using Implicit Large Eddy Simulations with a Discontinuous Galerkin method , 2010 .
[17] R. B. Dean. Reynolds Number Dependence of Skin Friction and Other Bulk Flow Variables in Two-Dimensional Rectangular Duct Flow , 1978 .
[18] S. Corrsin,et al. Simple Eulerian time correlation of full-and narrow-band velocity signals in grid-generated, ‘isotropic’ turbulence , 1971, Journal of Fluid Mechanics.
[19] Zhi Jian Wang,et al. A conservative correction procedure via reconstruction formulation with the Chain-Rule divergence evaluation , 2013, J. Comput. Phys..
[20] M. Selig,et al. High-Lift Low Reynolds Number Airfoil Design , 1997 .
[21] Paul G. Tucker,et al. Canonical Test Cases for High-Order Unstructured Implicit Large Eddy Simulation , 2014 .
[22] Ulrich Rist,et al. Investigations on controlled transition development in a laminar separation bubble by means of LDA and PIV , 2004 .
[23] P. Moin,et al. A dynamic localization model for large-eddy simulation of turbulent flows , 1995, Journal of Fluid Mechanics.
[24] Sanjiva K. Lele,et al. Large eddy simulation of a Mach 0.9 turbulent jet , 1999 .
[25] H. T. Huynh,et al. A Reconstruction Approach to High -Order Schemes Including Discontinuous Galerkin for Diffusion , 2009 .
[26] Z. Wang,et al. Implicit Large Eddy Simulation of Low Reynolds Number Transitional Flow over a Wing Using High-Order Spectral Difference Method , 2010 .
[27] H. T. Huynh,et al. A Flux Reconstruction Approach to High-Order Schemes Including Discontinuous Galerkin Methods , 2007 .
[28] Brian C. Vermeire,et al. ILES Using the Correction Procedure via Reconstruction Scheme , 2013 .
[29] Zhi J. Wang,et al. Spectral (Finite) Volume Method for Conservation Laws on Unstructured Grids. Basic Formulation , 2002 .
[30] L. Bricteux,et al. Implicit LES of free and wall‐bounded turbulent flows based on the discontinuous Galerkin/symmetric interior penalty method , 2015 .
[31] Jessica Gullbrand,et al. Grid-Independent Large-Eddy Simulation in Turbulent Channel Flow Using Three-Dimensional Explicit Filtering , 2003 .
[32] Xiaoqin Zhang,et al. Calibration of model and discretization parameters for turbulent channel flow , 2008 .
[33] Marcel Vinokur,et al. Discontinuous Spectral Difference Method for Conservation Laws on Unstructured Grids , 2004 .
[34] Andrew Pollard,et al. Evaluation of Turbulence Models Using Direct Numerical and Large-Eddy Simulation Data , 2011 .
[35] Chi-Wang Shu,et al. Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .
[36] Koen Hillewaert,et al. Assessment of a discontinuous Galerkin method for the simulation of vortical flows at high Reynolds number , 2014 .
[37] Per-Olof Persson,et al. Implicit Large Eddy Simulation of transition to turbulence at low Reynolds numbers using a Discontinuous Galerkin method , 2011 .
[38] A. Jameson,et al. Discrete filter operators for large‐eddy simulation using high‐order spectral difference methods , 2013 .
[39] F. Grinstein,et al. Large Eddy simulation of high-Reynolds-number free and wall-bounded flows , 2002 .
[40] Haiyang Gao,et al. A High-Order Unifying Discontinuous Formulation for the Navier-Stokes Equations on 3D Mixed Grids , 2011 .
[41] Antony Jameson,et al. Insights from von Neumann analysis of high-order flux reconstruction schemes , 2011, J. Comput. Phys..
[42] W. J. Gordon,et al. Construction of curvilinear co-ordinate systems and applications to mesh generation , 1973 .
[43] Petros Koumoutsakos,et al. A comparison of vortex and pseudo-spectral methods for the simulation of periodic vortical flows at high Reynolds numbers , 2011, J. Comput. Phys..
[44] S. Rebay,et al. A High-Order Accurate Discontinuous Finite Element Method for the Numerical Solution of the Compressible Navier-Stokes Equations , 1997 .
[45] Miguel R. Visbal,et al. Implicit Large Eddy Simulation of Low Reynolds Number Flow Past the SD7003 Airfoil , 2008 .
[46] Antony Jameson,et al. A New Class of High-Order Energy Stable Flux Reconstruction Schemes , 2011, J. Sci. Comput..
[47] C. Meneveau,et al. Decaying turbulence in an active-grid-generated flow and comparisons with large-eddy simulation , 2003, Journal of Fluid Mechanics.
[48] Sylvain Lardeau,et al. Applied large eddy simulation , 2009, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.
[49] Miguel R. Visbal,et al. Comparative study of implicit and subgrid‐scale model large‐eddy simulation techniques for low‐Reynolds number airfoil applications , 2013 .
[50] Zhi J. Wang,et al. Implicit Large Eddy Simulation of Transitional Flow over a SD7003 Wing Using High-order Spectral Difference Method , 2010 .
[51] Nikolaus A. Adams,et al. An adaptive local deconvolution method for implicit LES , 2005, J. Comput. Phys..
[52] Z. Wang. High-order methods for the Euler and Navier–Stokes equations on unstructured grids , 2007 .
[53] W. J. Gordon,et al. Transfinite mappings and their application to grid generation , 1982 .
[54] Rémi Abgrall,et al. High‐order CFD methods: current status and perspective , 2013 .
[55] Brian C. Vermeire,et al. Adaptive IMEX schemes for high-order unstructured methods , 2015, J. Comput. Phys..
[56] A. Beck,et al. On the accuracy of high-order discretizations for underresolved turbulence simulations , 2013 .
[57] Siva Nadarajah,et al. Adaptive IMEX Time-Stepping for the Correction Procedure via Reconstruction Scheme , 2013 .
[58] Neil D. Sandham,et al. Direct numerical simulation of ‘short’ laminar separation bubbles with turbulent reattachment , 2000, Journal of Fluid Mechanics.
[59] S. Orszag,et al. Small-scale structure of the Taylor–Green vortex , 1983, Journal of Fluid Mechanics.
[60] Paul G. Tucker,et al. LES of Impingement Heat Transfer on a Concave Surface , 2010 .
[61] Chi-Wang Shu,et al. TVB Runge-Kutta local projection discontinuous galerkin finite element method for conservation laws. II: General framework , 1989 .
[62] John A. Ekaterinaris,et al. High-order accurate, low numerical diffusion methods for aerodynamics , 2005 .