A novel method for constructing high accurate and robust WENO-Z type scheme

A novel method for constructing robust and high-order accurate weighted essentially non-oscillatory (WENO) scheme is proposed in this paper. The method is mainly based on the WENO-Z type scheme, in which, an eighth-order global smoothness indicator (the square of the approximation of the fourth-order derivative on the five-point stencil used by the fifth-order WENO scheme) is used, and in order to keep the ENO property and robustness, the constant 1 used to calculate the un-normalized weights is replaced by a function of local smoothness indicators of candidate sub-stencils. This function is designed to have following adaptive property: if the five-point stencil contains a discontinuity, then the function approaches to a small value, otherwise, it approaches to a large value. Analysis and numerical results show that the resulted WENO-Z type (WENO-ZN) scheme is robust for capturing shock waves and, in smooth regions, achieves fifth-order accuracy at first-order critical point and fourth-order accuracy at second-order critical point.

[1]  Ming Yu,et al.  A new weighting method for improving the WENO‐Z scheme , 2018 .

[2]  Yiqing Shen,et al.  Discontinuity-Detecting Method for a Four-Point Stencil and Its Application to Develop a Third-Order Hybrid-WENO Scheme , 2019, J. Sci. Comput..

[3]  R. Rosner,et al.  On the miscible Rayleigh–Taylor instability: two and three dimensions , 2001, Journal of Fluid Mechanics.

[4]  Feng Xiao,et al.  A fifth-order shock capturing scheme with two-stage boundary variation diminishing algorithm , 2019, J. Comput. Phys..

[5]  A. Harten High Resolution Schemes for Hyperbolic Conservation Laws , 2017 .

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

[7]  S. Osher,et al.  Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .

[8]  Wai-Sun Don,et al.  Accuracy of the weighted essentially non-oscillatory conservative finite difference schemes , 2013, J. Comput. Phys..

[9]  Michael Dumbser,et al.  Efficient, high accuracy ADER-WENO schemes for hydrodynamics and divergence-free magnetohydrodynamics , 2008, Journal of Computational Physics.

[10]  J. Steger,et al.  Flux vector splitting of the inviscid gasdynamic equations with application to finite-difference methods , 1981 .

[11]  Chi-Wang Shu,et al.  Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .

[12]  Chi-Wang Shu,et al.  The Runge-Kutta Discontinuous Galerkin Method for Conservation Laws V , 1998 .

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

[14]  Bruno Costa,et al.  An improved WENO-Z scheme , 2016, J. Comput. Phys..

[15]  Gecheng Zha,et al.  A robust seventh-order WENO scheme and its applications , 2008 .

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

[17]  Yeon Ju Lee,et al.  An improved weighted essentially non-oscillatory scheme with a new smoothness indicator , 2013, J. Comput. Phys..

[18]  Chao Yang,et al.  A new smoothness indicator for improving the weighted essentially non-oscillatory scheme , 2014, J. Comput. Phys..

[19]  Yinghua Wang,et al.  Generalized Sensitivity Parameter Free Fifth Order WENO Finite Difference Scheme with Z-Type Weights , 2019, Journal of Scientific Computing.

[20]  J. M. Powers,et al.  Mapped weighted essentially non-oscillatory schemes: Achieving optimal order near critical points , 2005 .

[21]  Mehdi Dehghan,et al.  A high-order symmetrical weighted hybrid ENO-flux limiter scheme for hyperbolic conservation laws , 2014, Comput. Phys. Commun..

[22]  Wai-Sun Don,et al.  High order weighted essentially non-oscillatory WENO-Z schemes for hyperbolic conservation laws , 2011, J. Comput. Phys..

[23]  Nail K. Yamaleev,et al.  Third-order Energy Stable WENO scheme , 2008, J. Comput. Phys..

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

[25]  Yong-Tao Zhang,et al.  Resolution of high order WENO schemes for complicated flow structures , 2003 .

[26]  Jungho Yoon,et al.  Modified Non-linear Weights for Fifth-Order Weighted Essentially Non-oscillatory Schemes , 2016, J. Sci. Comput..

[27]  G. A. Gerolymos,et al.  Very-high-order weno schemes , 2009, J. Comput. Phys..

[28]  Chang-Yeol Jung,et al.  Fine structures for the solutions of the two-dimensional Riemann problems by high-order WENO schemes , 2018, Adv. Comput. Math..

[29]  Nikolaus A. Adams,et al.  An adaptive central-upwind weighted essentially non-oscillatory scheme , 2010, J. Comput. Phys..

[30]  Wai-Sun Don,et al.  An improved weighted essentially non-oscillatory scheme for hyperbolic conservation laws , 2008, J. Comput. Phys..