A Fourth-Order Central WENO Scheme for Multidimensional Hyperbolic Systems of Conservation Laws

We present the first fourth-order central scheme for two-dimensional hyperbolic systems of conservation laws. Our new method is based on a central weighted nonoscillatory approach. The heart of our method is the reconstruction step, in which a genuinely two-dimensional interpolant is reconstructed from cell averages by taking a convex combination of building blocks in the form of biquadratic polynomials. Similarly to other central schemes, our new method enjoys the simplicity of the black-box approach. All that is required in order to solve a problem is to supply the flux function and an estimate on the speed of propagation. The high-resolution properties of the scheme as well as its resistance to mesh orientation, and the effectiveness of the componentwise approach, are demonstrated in a variety of numerical examples.

[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]  Gabriella Puppo,et al.  High-Order Central Schemes for Hyperbolic Systems of Conservation Laws , 1999, SIAM J. Sci. Comput..

[3]  Chi-Wang Shu,et al.  Efficient Implementation of Weighted ENO Schemes , 1995 .

[4]  P. Lax Weak solutions of nonlinear hyperbolic equations and their numerical computation , 1954 .

[5]  P. Woodward,et al.  The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .

[6]  E. Tadmor,et al.  Third order nonoscillatory central scheme for hyperbolic conservation laws , 1998 .

[7]  Alexander Kurganov,et al.  Semidiscrete Central-Upwind Schemes for Hyperbolic Conservation Laws and Hamilton-Jacobi Equations , 2001, SIAM J. Sci. Comput..

[8]  S. Osher,et al.  Weighted essentially non-oscillatory schemes , 1994 .

[9]  G. Russo,et al.  NUMERICAL SOLUTION FOR HYDRODYNAMICAL MODELS OF SEMICONDUCTORS , 2000 .

[10]  Vittorio Romano,et al.  Extended Hydrodynamical Model of Carrier Transport in Semiconductors , 2000, SIAM J. Appl. Math..

[11]  Gabriella Puppo,et al.  A third order central WENO scheme for 2D conservation laws , 2000 .

[12]  E. Tadmor,et al.  New High-Resolution Central Schemes for Nonlinear Conservation Laws and Convection—Diffusion Equations , 2000 .

[13]  Vittorio Romano,et al.  Central Schemes for Balance Laws of Relaxation Type , 2000, SIAM J. Numer. Anal..

[14]  Chi-Wang Shu Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .

[15]  Eitan Tadmor,et al.  Solution of two‐dimensional Riemann problems for gas dynamics without Riemann problem solvers , 2002 .

[16]  Xu-Dong Liu,et al.  Solution of Two-Dimensional Riemann Problems of Gas Dynamics by Positive Schemes , 1998, SIAM J. Sci. Comput..

[17]  G. Sod A survey of several finite difference methods for systems of nonlinear hyperbolic conservation laws , 1978 .

[18]  B. V. Leer,et al.  Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .

[19]  Gabriella Puppo,et al.  Compact Central WENO Schemes for Multidimensional Conservation Laws , 1999, SIAM J. Sci. Comput..

[20]  Stanley Osher,et al.  Nonoscillatory high order accurate self-similar maximum principle satisfying shock capturing schemes I , 1996 .

[21]  James P. Collins,et al.  Numerical Solution of the Riemann Problem for Two-Dimensional Gas Dynamics , 1993, SIAM J. Sci. Comput..

[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]  Alexander Kurganov,et al.  A third-order semi-discrete genuinely multidimensional central scheme for hyperbolic conservation laws and related problems , 2001, Numerische Mathematik.

[25]  Richard Sanders,et al.  High resolution staggered mesh approach for nonlinear hyperbolic systems of conser-vation laws , 1992 .

[26]  P. Raviart,et al.  Numerical Approximation of Hyperbolic Systems of Conservation Laws , 1996, Applied Mathematical Sciences.

[27]  Eitan Tadmor,et al.  Nonoscillatory Central Schemes for Multidimensional Hyperbolic Conservation Laws , 1998, SIAM J. Sci. Comput..

[28]  E. Tadmor,et al.  Non-oscillatory central differencing for hyperbolic conservation laws , 1990 .

[29]  C. Schulz-Rinne,et al.  Classification of the Riemann problem for two-dimensional gas dynamics , 1991 .

[30]  M. Zennaro Natural continuous extensions of Runge-Kutta methods , 1986 .

[31]  Gabriella Puppo,et al.  On the behavior of the total variation in CWENO methods for conservation laws , 2000 .

[32]  Doron Levy,et al.  A Third-Order Semidiscrete Central Scheme for Conservation Laws and Convection-Diffusion Equations , 2000, SIAM J. Sci. Comput..

[33]  Equilibrium real gas computations using Marquina's scheme , 2003 .

[34]  G. Russo,et al.  Central WENO schemes for hyperbolic systems of conservation laws , 1999 .

[35]  E. Tadmor Approximate solutions of nonlinear conservation laws , 1998 .

[36]  S. Osher,et al.  Regular ArticleUniformly High Order Accurate Essentially Non-oscillatory Schemes, III , 1997 .