Scalar Conservation Laws

Baver Okutmustur
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引用次数: 4

Abstract

We present a theoretical aspect of conservation laws by using simplest scalar models with essential properties. We start by rewriting the general scalar conservation law as a quasilinear partial differential equation and solve it by method of characteristics. Here we come across with the notion of strong and weak solutions depending on the initial value of the problem. Taking into account a special initial data for the left and right side of a discontinuity point, we get the related Riemann problem. An illustration of this problem is provided by some examples. In the remaining part of the chapter, we extend this analysis to the gas dynamics given in the Euler system of equations in one dimension. The transformations of this system into the Lagrangian coordinates follow by applying a suitable change of coordinates which is one of the main issues of this section. We next introduce a first-order Godunov finite volume scheme for scalar conservation laws which leads us to write Godunov schemes in both Eulerian and Lagrangian coordinates in one dimension where, in particular, the Lagrangian scheme is reformulated as a finite volume method. Finally, we end up the chapter by providing a comparison of Eulerian and Lagrangian approaches.
标量守恒定律
我们用具有基本性质的最简单标量模型,从理论上给出了守恒定律。我们首先将一般标量守恒定律改写为拟线性偏微分方程,并用特征法求解。这里我们遇到了强解和弱解的概念,这取决于问题的初始值。考虑不连续点左右两侧的特殊初始数据,得到了相关的黎曼问题。通过一些例子来说明这个问题。在本章的其余部分,我们将这种分析扩展到一维欧拉方程组中给出的气体动力学。这个系统到拉格朗日坐标的变换是通过适当的坐标变换来实现的,这是本节的主要问题之一。接下来,我们引入标量守恒定律的一阶Godunov有限体积格式,它使我们在一维欧拉和拉格朗日坐标系中写出Godunov格式,特别是拉格朗日格式被重新表述为有限体积方法。最后,我们通过欧拉方法和拉格朗日方法的比较来结束本章。
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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