A High-Order Central ENO Finite-Volume Scheme for Three-Dimensional Turbulent Reactive Flows on Unstructured Mesh
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[1] I. Shepherd. Flame surface density and burning rate in premixed turbulent flames , 1995 .
[2] Claus-Dieter Munz,et al. A contribution to the construction of diffusion fluxes for finite volume and discontinuous Galerkin schemes , 2007, J. Comput. Phys..
[3] Carlos A. Felippa,et al. A compendium of FEM integration formulas for symbolic work , 2004 .
[4] S. Osher,et al. Uniformly high order accurate essentially non-oscillatory schemes, 111 , 1987 .
[5] Y. Saad,et al. GMRES: a generalized minimal residual algorithm for solving nonsymmetric linear systems , 1986 .
[6] Clinton P. T. Groth,et al. High-Order CENO Finite-Volume Schemes for Multi-Block Unstructured Mesh , 2011 .
[7] Chi-Wang Shu,et al. TVB Runge-Kutta local projection discontinuous galerkin finite element method for conservation laws. II: General framework , 1989 .
[8] C. Ollivier-Gooch,et al. A high-order-accurate unstructured mesh finite-volume scheme for the advection-diffusion equation , 2002 .
[9] Sergio Pirozzoli,et al. On the spectral properties of shock-capturing schemes , 2006, J. Comput. Phys..
[10] J. Sachdev,et al. A parallel solution-adaptive scheme for multi-phase core flows in solid propellant rocket motors , 2005 .
[11] Charles L. Lawson,et al. Solving least squares problems , 1976, Classics in applied mathematics.
[12] Y. Saad,et al. Krylov Subspace Methods on Supercomputers , 1989 .
[13] Clinton P. T. Groth,et al. A computational framework for predicting laminar reactive flows with soot formation , 2010 .
[14] K. Powell,et al. Solution-Adaptive Cartesian Cell Approach for Viscous and Inviscid Flows , 1996 .
[15] E. R. V. Driest. On Turbulent Flow Near a Wall , 1956 .
[16] Charles Merkle,et al. Time-accurate unsteady incompressible flow algorithms based on artificial compressibility , 1987 .
[17] Caskey,et al. GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS I . THE BASIC EXPERIMENT , 1962 .
[18] Lucian Ivan,et al. Development of High-order CENO Finite-volume Schemes with Block-based Adaptive Mesh Refinement (AMR) , 2011 .
[19] Ö. Gülder,et al. Investigation of Dynamics of Lean Turbulent Premixed Flames by Rayleigh Imaging , 2009 .
[20] Yousef Saad,et al. Hybrid Krylov Methods for Nonlinear Systems of Equations , 1990, SIAM J. Sci. Comput..
[21] U. Piomelli,et al. Two-layer approximate boundary conditions for large-eddy simulations , 1996 .
[22] Zhi J. Wang,et al. Spectral (Finite) Volume Method for Conservation Laws on Unstructured Grids. Basic Formulation , 2002 .
[23] Philip L. Roe,et al. Efficient construction and utilisation of approximate riemann solutions , 1985 .
[24] O. Friedrich,et al. Weighted Essentially Non-Oscillatory Schemes for the Interpolation of Mean Values on Unstructured Grids , 1998 .
[25] B. Hjertager,et al. On mathematical modeling of turbulent combustion with special emphasis on soot formation and combustion , 1977 .
[26] C. P. T. Groth,et al. High-Order CENO Finite-Volume Scheme for Low-Speed Viscous Flows on Three-Dimensional Unstructured Mesh , 2011 .
[27] Rémi Abgrall,et al. On essentially non-oscillatory schemes on unstructured meshes: analysis and implementation , 1994 .
[28] Seungsoo Lee,et al. Convergence Characteristics of Upwind Method for Modified Artificial Compressibility Method , 2011 .
[29] E. Cuthill,et al. Reducing the bandwidth of sparse symmetric matrices , 1969, ACM '69.
[30] Timothy J. Barth,et al. Recent developments in high order K-exact reconstruction on unstructured meshes , 1993 .
[31] D. Stanescu,et al. Essentially Nonoscillatory Euler Solutions on Unstructured Meshes Using Extrapolation , 1998 .
[32] George Karypis,et al. Parmetis parallel graph partitioning and sparse matrix ordering library , 1997 .
[33] S. Benhamadouche,et al. A synthetic-eddy-method for generating inflow conditions for large-eddy simulations , 2006 .
[34] Clinton P. T. Groth,et al. International Journal of Computational Fluid Dynamics a Parallel Adaptive Mesh Refinement Algorithm for Predicting Turbulent Non-premixed Combusting Flows a Parallel Adaptive Mesh Refinement Algorithm for Predicting Turbulent Non-premixed Combusting Flows , 2022 .
[35] Carl Ollivier-Gooch,et al. High-order ENO schemes for unstructured meshes based on least-squares reconstruction , 1997 .
[36] Rainald Löhner,et al. A Hermite WENO-based limiter for discontinuous Galerkin method on unstructured grids , 2007, J. Comput. Phys..
[37] R. Dembo,et al. INEXACT NEWTON METHODS , 1982 .
[38] Z. Wang,et al. Spectral (Finite) Volume Method for Conservation Laws on Unstructured Grids , 2002 .
[39] Stuart E. Rogers,et al. Steady and unsteady solutions of the incompressible Navier-Stokes equations , 1991 .
[40] V. Venkatakrishnan. On the accuracy of limiters and convergence to steady state solutions , 1993 .
[41] J. Smagorinsky,et al. GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS , 1963 .
[42] Andreas Haselbacher,et al. A WENO Reconstruction Algorithim for Unstructured Grids Based on Explicit Stencil Construction , 2005 .
[43] Carl Ollivier-Gooch,et al. A high-order accurate unstructured finite volume Newton-Krylov algorithm for inviscid compressible flows , 2008, J. Comput. Phys..
[44] U. Piomelli,et al. Wall-layer models for large-eddy simulations , 2008 .
[45] Chongam Kim,et al. Multi-dimensional limiting process for hyperbolic conservation laws on unstructured grids , 2005, J. Comput. Phys..
[46] D. Spalding. Mixing and chemical reaction in steady confined turbulent flames , 1971 .
[47] A. Chorin. A Numerical Method for Solving Incompressible Viscous Flow Problems , 1997 .
[48] Chi-Wang Shu,et al. The Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws. IV. The multidimensional case , 1990 .
[49] Scott Northrup,et al. Parallel solution-adaptive method for two dimensional non-premixed combusting flows , 2011 .
[50] Luc Vervisch,et al. DNS of a premixed turbulent V flame and LES of a ducted flame using a FSD-PDF subgrid scale closure with FPI-tabulated chemistry , 2005 .
[51] Scott Northrup,et al. Parallel Implicit Adaptive Mesh Refinement Scheme for Body-Fitted Multi-Block Mesh , 2005 .
[52] Clinton P. T. Groth,et al. High-Order Central ENO Finite-Volume Scheme with Adaptive Mesh Refinement , 2007 .
[53] J. D. Wilson,et al. Shape Functions for Velocity Interpolation in General Hexahedral Cells , 2002 .
[54] C. Lawson,et al. Solving least squares problems , 1976, Classics in applied mathematics.
[55] R. Hartmann,et al. Adaptive discontinuous Galerkin finite element methods for the compressible Euler equations , 2002 .
[56] John W. Goodrich,et al. Unsteady solution of incompressible Navier-Stokes equations , 1988 .
[57] Ö. Gülder,et al. Assessment of Presumed PDF Models for Large Eddy Simulation of Turbulent Premixed Flames , 2011 .
[58] Clinton P. T. Groth,et al. LES of a laboratory-scale turbulent premixed Bunsen flame using FSD, PCM-FPI and thickened flame models , 2011 .
[59] Zhi Jian Wang,et al. Spectral (Finite) Volume Method for Conservation Laws on Unstructured Grids III: One Dimensional Systems and Partition Optimization , 2004, J. Sci. Comput..
[60] Arnaud G. Malan,et al. An improved unsteady, unstructured, artificial compressibility, finite volume scheme for viscous incompressible flows: Part II. Application , 2002 .
[61] Arnaud G. Malan,et al. An improved unsteady, unstructured, artificial compressibility, finite volume scheme for viscous incompressible flows: Part I. Theory and implementation , 2002 .
[62] Dimitri J. Mavriplis,et al. Revisiting the Least-squares Procedure for Gradient Reconstruction on Unstructured Meshes , 2003 .
[63] Paul Kutler,et al. Implicit Finite-Difference Procedures for the Computation of Vortex Wakes , 1976 .
[64] Dochan Kwak,et al. High-Order Spectral Volume Method for 2D Euler Equations , 2003 .
[65] Stuart E. Rogers,et al. Upwind differencing scheme for the time-accurate incompressible Navier-Stokes equations , 1990 .
[66] D. Wilcox. Turbulence modeling for CFD , 1993 .
[67] Ö. Gülder,et al. Premixed turbulent flame front structure investigation by Rayleigh scattering in the thin reaction zone regime , 2009 .
[68] P. Roe. Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .
[69] K. Rhee,et al. Blackbody radiation functions , 1984 .
[70] Yousef Saad,et al. Iterative methods for sparse linear systems , 2003 .
[71] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[72] Clinton P. T. Groth,et al. High-Order Solution-Adaptive Central Essentially Non-Oscillatory (CENO) Method for Viscous Flows , 2011 .
[73] Chaowei Hu,et al. No . 98-32 Weighted Essentially Non-Oscillatory Schemes on Triangular Meshes , 1998 .
[74] Z. Qian,et al. Preconditioned pseudo-compressibility methods for incompressible Navier-Stokes equations , 2010 .
[75] Clinton P. T. Groth,et al. Solution of the equation of radiative transfer using a Newton-Krylov approach and adaptive mesh refinement , 2012, J. Comput. Phys..
[76] A. Jameson. Time dependent calculations using multigrid, with applications to unsteady flows past airfoils and wings , 1991 .
[77] Clinton P. T. Groth,et al. A parallel solution - adaptive method for three-dimensional turbulent non-premixed combusting flows , 2010, J. Comput. Phys..
[78] J. D. Wilson,et al. Test functions for three-dimensionalcontrol-volume mixed finite element methods on irregular grids , 2000 .
[79] J. Murthy,et al. A PRESSURE-BASED METHOD FOR UNSTRUCTURED MESHES , 1997 .
[80] Yuzhi Sun,et al. Spectral (finite) volume method for conservation laws on unstructured grids VI: Extension to viscous flow , 2006, J. Comput. Phys..
[81] Thomas Sonar,et al. On the construction of essentially non-oscillatory finite volume approximations to hyperbolic conservation laws on general triangulations : polynomial recovery, accuracy and stencil selection , 1997 .
[82] E. Turkel,et al. Preconditioned methods for solving the incompressible low speed compressible equations , 1987 .