Quadrature-free non-oscillatory finite volume schemes on unstructured meshes for nonlinear hyperbolic systems
暂无分享,去创建一个
Michael Dumbser | Eleuterio F. Toro | Vladimir A. Titarev | Martin Käser | E. Toro | M. Dumbser | M. Käser | V. Titarev
[1] 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 .
[2] Chi-Wang Shu,et al. TVB Runge-Kutta local projection discontinuous galerkin finite element method for conservation laws. II: General framework , 1989 .
[3] J. V. D. Vegt,et al. Space--time discontinuous Galerkin finite element method with dynamic grid motion for inviscid compressible flows: I. general formulation , 2002 .
[4] R. Dyson. Technique for very High Order Nonlinear Simulation and Validation , 2002 .
[5] E. Toro,et al. Restoration of the contact surface in the HLL-Riemann solver , 1994 .
[6] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[7] H. Atkins,et al. Quadrature-Free Implementation of the Discontinuous Galerkin Method for Hyperbolic Equations , 1996 .
[8] P. Raviart,et al. An asymptotic expansion for the solution of the generalized Riemann problem Part I: General theory , 1988 .
[9] Eleuterio F. Toro,et al. ADER schemes for three-dimensional non-linear hyperbolic systems , 2005 .
[10] E. Toro,et al. Solution of the generalized Riemann problem for advection–reaction equations , 2002, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.
[11] Rémi Abgrall,et al. On essentially non-oscillatory schemes on unstructured meshes: analysis and implementation , 1994 .
[12] P. Woodward,et al. The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .
[13] Michael Dumbser,et al. Arbitrary high order non-oscillatory finite volume schemes on unstructured meshes for linear hyperbolic systems , 2007, J. Comput. Phys..
[14] Rosa Donat,et al. Shock-Vortex Interactions at High Mach Numbers , 2003, J. Sci. Comput..
[15] S. Rebay,et al. High-Order Accurate Discontinuous Finite Element Solution of the 2D Euler Equations , 1997 .
[16] Claus-Dieter Munz,et al. A Discontinuous Galerkin Scheme Based on a Space–Time Expansion. I. Inviscid Compressible Flow in One Space Dimension , 2007, J. Sci. Comput..
[17] Zhi J. Wang,et al. Extension of the spectral volume method to high-order boundary representation , 2006 .
[18] H. van der Ven,et al. Space-time discontinuous Galerkin finite element method with dynamic grid motion for inviscid compressible flows. Part II. Efficient flux quadrature , 2002 .
[19] Michael Dumbser,et al. A matrix stability analysis of the carbuncle phenomenon , 2004 .
[20] P. Lax. Weak solutions of nonlinear hyperbolic equations and their numerical computation , 1954 .
[21] E. Toro. Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .
[22] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[23] S. Osher,et al. Uniformly high order accurate essentially non-oscillatory schemes, 111 , 1987 .
[24] Michael Dumbser,et al. On Source Terms and Boundary Conditions Using Arbitrary High Order Discontinuous Galerkin Schemes , 2007, Int. J. Appl. Math. Comput. Sci..
[25] Armin Iske,et al. ADER schemes on adaptive triangular meshes for scalar conservation laws , 2005 .
[26] C. Ollivier-Gooch,et al. A high-order-accurate unstructured mesh finite-volume scheme for the advection-diffusion equation , 2002 .
[27] B. V. Leer,et al. Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .
[28] Chi-Wang Shu,et al. The Runge-Kutta local projection $P^1$-discontinuous-Galerkin finite element method for scalar conservation laws , 1988, ESAIM: Mathematical Modelling and Numerical Analysis.
[29] Chi-Wang Shu,et al. TVB Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws III: one-dimensional systems , 1989 .
[30] Chi-Wang Shu,et al. The Runge-Kutta Discontinuous Galerkin Method for Conservation Laws V , 1998 .
[31] Bernardo Cockburn. Discontinuous Galerkin methods , 2003 .
[32] Chaowei Hu,et al. No . 98-32 Weighted Essentially Non-Oscillatory Schemes on Triangular Meshes , 1998 .
[33] Arne Taube,et al. Arbitrary High-Order Discontinuous Galerkin Schemes for the Magnetohydrodynamic Equations , 2007, J. Sci. Comput..
[34] Michael Dumbser,et al. Arbitrary High Order Finite Volume Schemes on Unstructured Meshes , 2009 .
[35] P. Raviart,et al. An asymptotic expansion for the solution of the generalized Riemann problem. Part 2 : application to the equations of gas dynamics , 1989 .
[36] M. V. Dyke,et al. An Album of Fluid Motion , 1982 .
[37] Bernardo Cockburn,et al. The Runge-Kutta local projection P1-discontinuous-Galerkin finite element method for scalar conservation laws , 1988 .
[38] A. Stroud. Approximate calculation of multiple integrals , 1973 .
[39] Eleuterio F. Toro,et al. Towards Very High Order Godunov Schemes , 2001 .
[40] E. Toro,et al. An arbitrary high-order Discontinuous Galerkin method for elastic waves on unstructured meshes - V. Local time stepping and p-adaptivity , 2007 .
[41] J. Falcovitz,et al. A second-order Godunov-type scheme for compressible fluid dynamics , 1984 .
[42] Michael Dumbser,et al. Arbitrary high-order finite volume schemes for seismic wave propagation on unstructured meshes in 2D and 3D , 2007 .
[43] H. Huynh,et al. Accurate Monotonicity-Preserving Schemes with Runge-Kutta Time Stepping , 1997 .
[44] Jean-Marc Moschetta,et al. A Cure for the Sonic Point Glitch , 2000 .
[45] P. Roe,et al. On Godunov-type methods near low densities , 1991 .
[46] Chi-Wang Shu,et al. The Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws. IV. The multidimensional case , 1990 .
[47] Gianfranco Chiocchia. Chapter 4: Exact solutions to transonic and supersonic flows , 1984 .
[48] P. Lax,et al. On Upstream Differencing and Godunov-Type Schemes for Hyperbolic Conservation Laws , 1983 .
[49] George Karypis,et al. Multilevel k-way Partitioning Scheme for Irregular Graphs , 1998, J. Parallel Distributed Comput..
[50] Chi-Wang Shu,et al. Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .
[51] S. Osher,et al. Regular ArticleUniformly High Order Accurate Essentially Non-oscillatory Schemes, III , 1997 .
[52] Chi-Wang Shu,et al. A technique of treating negative weights in WENO schemes , 2000 .
[53] B. V. Leer,et al. Towards the ultimate conservative difference scheme. II. Monotonicity and conservation combined in a second-order scheme , 1974 .
[54] O. Friedrich,et al. Weighted Essentially Non-Oscillatory Schemes for the Interpolation of Mean Values on Unstructured Grids , 1998 .
[55] P. Roe. Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .
[56] P. Frederickson,et al. Higher order solution of the Euler equations on unstructured grids using quadratic reconstruction , 1990 .
[57] I. Bohachevsky,et al. Finite difference method for numerical computation of discontinuous solutions of the equations of fluid dynamics , 1959 .
[58] Michael Dumbser,et al. Building Blocks for Arbitrary High Order Discontinuous Galerkin Schemes , 2006, J. Sci. Comput..
[59] J Vandervegt,et al. Space–Time Discontinuous Galerkin Finite Element Method with Dynamic Grid Motion for Inviscid Compressible FlowsI. General Formulation , 2002 .
[60] Moshe Dubiner. Spectral methods on triangles and other domains , 1991 .