A new method towards high-order weno schemes on structured and unstructured grids
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[1] Jun Zhu,et al. A new third order finite volume weighted essentially non-oscillatory scheme on tetrahedral meshes , 2017, J. Comput. Phys..
[2] K. Mcalister,et al. NACA 0015 Wing Pressure and Trailing Vortex Measurements , 1991 .
[3] Chaowei Hu,et al. No . 98-32 Weighted Essentially Non-Oscillatory Schemes on Triangular Meshes , 1998 .
[4] Chunhua Sheng,et al. A preconditioned method for rotating flows at arbitrary mach number , 2011 .
[5] Hong Q. Yang,et al. Development of Vertex-Centered High-Order Schemes and Implementation in FUN3D , 2015 .
[6] Jun Zhu,et al. A new fifth order finite difference WENO scheme for solving hyperbolic conservation laws , 2016, J. Comput. Phys..
[7] P. Roe. Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .
[8] Chi-Wang Shu,et al. A technique of treating negative weights in WENO schemes , 2000 .
[9] Jianxian Qiu,et al. On the construction, comparison, and local characteristic decomposition for high-Order central WENO schemes , 2002 .
[10] James P. Collins,et al. Numerical Solution of the Riemann Problem for Two-Dimensional Gas Dynamics , 1993, SIAM J. Sci. Comput..
[11] Chi-Wang Shu. Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .
[12] A. Harten. High Resolution Schemes for Hyperbolic Conservation Laws , 2017 .
[13] Jun Zhu,et al. A New Type of Finite Volume WENO Schemes for Hyperbolic Conservation Laws , 2017, J. Sci. Comput..
[14] Michael Dumbser,et al. Arbitrary high order non-oscillatory finite volume schemes on unstructured meshes for linear hyperbolic systems , 2007, J. Comput. Phys..
[15] Jianhua Pan,et al. High order sub-cell finite volume schemes for solving hyperbolic conservation laws I: basic formulation and one-dimensional analysis , 2017 .
[16] P. Moin,et al. A dynamic subgrid‐scale eddy viscosity model , 1990 .
[17] S. Osher,et al. Weighted essentially non-oscillatory schemes , 1994 .
[18] Mengping Zhang,et al. On the Order of Accuracy and Numerical Performance of Two Classes of Finite Volume WENO Schemes , 2011 .
[19] Michael Dumbser,et al. Efficient, high accuracy ADER-WENO schemes for hydrodynamics and divergence-free magnetohydrodynamics , 2008, Journal of Computational Physics.
[20] G. Russo,et al. Central WENO schemes for hyperbolic systems of conservation laws , 1999 .
[21] O. Friedrich,et al. Weighted Essentially Non-Oscillatory Schemes for the Interpolation of Mean Values on Unstructured Grids , 1998 .
[22] P. Spalart. A One-Equation Turbulence Model for Aerodynamic Flows , 1992 .
[23] 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..
[24] Dimitri J. Mavriplis,et al. Revisiting the Least-squares Procedure for Gradient Reconstruction on Unstructured Meshes , 2003 .
[25] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[26] S. Osher,et al. Uniformly high order accurate essentially non-oscillatory schemes, 111 , 1987 .
[27] Pierre Sagaut,et al. Large-Eddy Simulation for Acoustics: Contributors , 2007 .
[28] Sergio Pirozzoli,et al. On the spectral properties of shock-capturing schemes , 2006, J. Comput. Phys..
[29] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .