Accuracy, temporal performance and stability comparisons of discretization methods for the numerical solution of Partial Differential Equations (PDEs) in the presence of steep moving fronts
暂无分享,去创建一个
[1] P. Lax,et al. Systems of conservation equations with a convex extension. , 1971, Proceedings of the National Academy of Sciences of the United States of America.
[2] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[3] L. Petzold,et al. Moving Mesh Methods with Upwinding Schemes for Time-Dependent PDEs , 1997 .
[4] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[5] N. Amundson,et al. A study of the shock layer in nonequilibrium exchange systems , 1971 .
[6] Doron Levy,et al. A Third-Order Semidiscrete Central Scheme for Conservation Laws and Convection-Diffusion Equations , 2000, SIAM J. Sci. Comput..
[7] Y. Lim,et al. Multiobjective Optimization in Terms of Economics and Potential Environment Impact for Process Design and Analysis in a Chemical Process Simulator , 1999 .
[8] Antonio Marquina,et al. Local Piecewise Hyperbolic Reconstruction of Numerical Fluxes for Nonlinear Scalar Conservation Laws , 1994, SIAM J. Sci. Comput..
[9] Martin Berzins,et al. Developing software for time-dependent problems using the method of lines and differential-algebraic integrators , 1989 .
[10] J. M. Sanz-Serna,et al. On simple moving grid methods for one-dimensional evolutionary partial differential equations , 1988 .
[11] Chi-Wang Shu. Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .
[12] Martin Berzins,et al. New NAG library software for first-order partial differential equations , 1994, TOMS.