Skip to main content

1996 | Buch

Numerical Approximation of Hyperbolic Systems of Conservation Laws

verfasst von: Edwige Godlewski, Pierre-Arnaud Raviart

Verlag: Springer New York

Buchreihe : Applied Mathematical Sciences

insite
SUCHEN

Über dieses Buch

This work is devoted to the theory and approximation of nonlinear hyper­ bolic systems of conservation laws in one or two space variables. It follows directly a previous publication on hyperbolic systems of conservation laws by the same authors, and we shall make frequent references to Godlewski and Raviart (1991) (hereafter noted G. R. ), though the present volume can be read independently. This earlier publication, apart from a first chap­ ter, especially covered the scalar case. Thus, we shall detail here neither the mathematical theory of multidimensional scalar conservation laws nor their approximation in the one-dimensional case by finite-difference con­ servative schemes, both of which were treated in G. R. , but we shall mostly consider systems. The theory for systems is in fact much more difficult and not at all completed. This explains why we shall mainly concentrate on some theoretical aspects that are needed in the applications, such as the solution of the Riemann problem, with occasional insights into more sophisticated problems. The present book is divided into six chapters, including an introductory chapter. For the reader's convenience, we shall resume in this Introduction the notions that are necessary for a self-sufficient understanding of this book -the main definitions of hyperbolicity, weak solutions, and entropy­ present the practical examples that will be thoroughly developed in the following chapters, and recall the main results concerning the scalar case.

Inhaltsverzeichnis

Frontmatter
Introduction
Abstract
In this section, we present the general form of systems of conservation laws in several space variables and we give some important examples of such systems that arise in continuum physics.
Edwige Godlewski, Pierre-Arnaud Raviart
I. Nonlinear hyperbolic systems in one space dimension
Abstract
The main goal of this chapter is to study the Riemann problem for a general nonlinear hyperbolic system of conservation laws in one space dimension. We begin by considering the case of a linear hyperbolic system with constant coefficients for which the Riemann problem is easily solved. Next, in the nonlinear case we introduce the notions of rarefaction waves, shock waves, and contact discontinuities, which play an essential role in the explicit construction of the solution of the Riemann problem. These notions are illustrated on the examples of the p-system and the gas dynamics equations. Then, we prove the local existence of an entropy solution of the Riemann problem for a general system in the sense that the initial states are sufficiently close. In fact, in the case of the p-system, we are able to prove that the Riemann problem is always solvable. We shall show in the next chapter that this is also true for the gas dynamics equations. These two basic chapters present the results with detailed proofs, which could be easily shortened for a reader already familiar with the subject.
Edwige Godlewski, Pierre-Arnaud Raviart
II. Gas dynamics and reacting flows
Abstract
Let us consider a fluid in a local thermodynamical equilibrium. Then we know from thermodynamics that the thermodynamical state of the fluid is completely determined by any two thermodynamic variables. Most often, we shall note by the same letter the corresponding mathematical functions, though they differ. For instance, we shall use
Edwige Godlewski, Pierre-Arnaud Raviart
III. Finite difference schemes for one-dimensional systems
Abstract
Let us consider again the Cauchy problem for a general system of conservation laws
$$ \left\{ {\begin{array}{*{20}{c}} {\frac{{\partial u}}{{\partial t}} + \frac{\partial }{{\partial x}}f\left( u \right) = 0,\quad x \in \mathbb{R},t > 0,} \\ {u\left( {x,0} \right) = {u_0}\left( x \right),} \end{array}} \right. $$
(1.1)
, where u = (u 1,..., u p ) T is a p-vector. As usual, we assume that this system is hyperbolic, i.e., the Jacobian matrix A(u) = f′(u) of f(u) has p real eigenvalues ranked in increasing order,
, and a complete set of eigenvectors. Moreover, we shall assume that for all 1 ≤ kp, the kth characteristic field is either genuinely nonlinear or linearly degenerate. For the notations concerning the difference schemes, we refer to Chapter III of G.R..
Edwige Godlewski, Pierre-Arnaud Raviart
IV. The case of multidimensional systems
Abstract
We shall mainly consider in this section a two-dimensional p × p hyperbolic system
(1.1)
.
Edwige Godlewski, Pierre-Arnaud Raviart
V. An introduction to boundary conditions
Abstract
The aim of this chapter is to introduce the unfamiliar reader to the topic of boundary conditions: we just want to give some insight into this question and do not pretend to give an exhaustive study. We recall first the main features of the initial boundary value problem (I.B.V.P.) before we present the numerical treatment of the question.
Edwige Godlewski, Pierre-Arnaud Raviart
Backmatter
Metadaten
Titel
Numerical Approximation of Hyperbolic Systems of Conservation Laws
verfasst von
Edwige Godlewski
Pierre-Arnaud Raviart
Copyright-Jahr
1996
Verlag
Springer New York
Electronic ISBN
978-1-4612-0713-9
Print ISBN
978-1-4612-6878-9
DOI
https://doi.org/10.1007/978-1-4612-0713-9