Two-Layer Viscous Shallow-Water Equations and Conservation Laws

H. Kanayama, Hiroshi Dan
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引用次数: 3

Abstract

In our previous papers, the two-layer viscous shallow-water equations were derived from the three-dimensional Navier-Stokes equations under the hydrostatic assumption. Also, it was noted that the combination of upper and lower equations in the two-layer model produces the classical one-layer equations if the density of each layer is the same. Then, the two-layer equations were approximated by a finite element method which followed our numerical scheme established for the one-layer model in 1978. Also, it was numerically demonstrated that the interfacial instability generated when the densities are the same can be eliminated by providing a sufficient density difference. In this paper, we newly show that conservation laws are still valid in the two-layer model. Also, we show results of a new physical experiment for the interfacial instability.
两层粘性浅水方程及守恒定律
在我们以前的文章中,两层粘性浅水方程是在流体静力假设下由三维Navier-Stokes方程导出的。此外,还注意到,如果每层的密度相同,则两层模型中上下方程的组合将产生经典的单层方程。然后,根据我们在1978年为单层模型建立的数值格式,用有限元法对两层方程进行近似。数值结果表明,密度相同时产生的界面不稳定性可以通过提供足够的密度差来消除。在本文中,我们新的证明了守恒定律在两层模型中仍然有效。此外,我们还展示了一个新的界面不稳定性物理实验的结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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