In [18], the authors have designed a new finite-volume mapped WENO scheme by introducing a new criterion which is defined as order-preserving (OP) in the design of the mapping. With this new criterion, a new mapping function was devised and the relevant mapped WENO scheme enjoyed the advantage that has the capacity to attain high resolutions and avoid spurious oscillations near discontinuities when solving the one-dimensional linear advection problems, expecially for long output times. Moreover, this new scheme, dubbed as MOP-WENO-ACMk, can significantly reduce the post-shock oscillations in the simulations of the two-dimensional steady problems with strong shock waves. In this article, we take a closer look at various existing mapped WENO schemes in references to obtain a general formula for their mapping functions that allows the extension of the OP criterion to all existing mapped WENO schemes. The improved mapped WENO scheme considerring the OP criterion based on the existing mapped WENO-X scheme is named MOP-WENO-X. Numerical solutions of the one-dimensional linear advection equation with different initial conditions computed by the MOP-WENO-X schemes are compared with the ones generated by the corresponding WENO-X schemes and the WENO-JS scheme. Some standard numerical experiments of two-dimensional Euler system such as the shock-vortex interaction and the 2D Riemann problems are presented. To summarize, the MOP-WENO-X schemes also enjoy the advantages of the MOP-WENO-ACMk scheme proposed in [18].
翻译:在[18]中,作者们设计了一个新的数量有限、绘制WENO计划,在绘图设计中引入了一个新的标准,被定义为维持秩序(OP) 。有了这一新的标准,设计了一个新的绘图功能,相关的绘制WENO计划具有优势,在解决单维线性对流问题时,能够达到高分辨率,避免在离子线性对流问题接近于不连续状态的情况下出现虚假的振动。此外,这个称为MO-WENO-ACMk的新计划,可以大大减少在以强烈冲击波模拟二维稳定问题的模拟中出现的震动后振荡。在本篇文章中,我们更仔细地审视了现有的绘制WENO计划,以获得一个通用的公式,从而使得将OP标准对流对流性对流性对流性对流(WENO-NO-NO-NO-NO-NO-X) 计划加以扩展,以现有的WEO-NO-NO-NO-NO-S-S-VER-VER-S-S-I-I-I-S-VEMO-I-S-S-S-IL-IL-SUNO-IL-IL-IL-S-S-S-IL-S-I-S-IL-IL-IL-S-S-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-S-S-S-S-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I)-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I-I