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2001 | Buch

Acoustic and Electromagnetic Equations

Integral Representations for Harmonic Problems

verfasst von: Jean-Claude Nédélec

Verlag: Springer New York

Buchreihe : Applied Mathematical Sciences

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Über dieses Buch

This book is devoted to the study of the acoustic wave equation and of the Maxwell system, the two most common wave equations encountered in physics or in engineering. The main goal is to present a detailed analysis of their mathematical and physical properties. Wave equations are time dependent. However, use of the Fourier trans­ form reduces their study to that of harmonic systems: the harmonic Helmholtz equation, in the case of the acoustic equation, or the har­ monic Maxwell system. This book concentrates on the study of these harmonic problems, which are a first step toward the study of more general time-dependent problems. In each case, we give a mathematical setting that allows us to prove existence and uniqueness theorems. We have systematically chosen the use of variational formulations related to considerations of physical energy. We study the integral representations of the solutions. These representa­ tions yield several integral equations. We analyze their essential properties. We introduce variational formulations for these integral equations, which are the basis of most numerical approximations. Different parts of this book were taught for at least ten years by the author at the post-graduate level at Ecole Poly technique and the University of Paris 6, to students in applied mathematics. The actual presentation has been tested on them. I wish to thank them for their active and constructive participation, which has been extremely useful, and I apologize for forcing them to learn some geometry of surfaces.

Inhaltsverzeichnis

Frontmatter
1. Some Wave Equations
Abstract
This book is devoted to the study of the acoustic wave equation and of the Maxwell system, the two most common wave equations that are encountered in physics or in engineering. Our objective is to present a detailed analysis of their mathematical and physical properties.
Jean-Claude Nédélec
2. The Helmholtz Equation
Abstract
The acoustic wave equation described the propagation of the sound in a medium like the air. It results, e.g., from the equation of the compressible gas dynamic, also called the compressible Navier-Stokes equations. In the case of small displacements of the gas, a linearization of these equations leads to an equation for the displacement and the small variation of the pressure in the gas. In the case of a homogeneous medium of mean density ρ 0, this is the well-known above system of equations
(2.1.1)
Where c is the speed of sound in the medium, the speed of displacement in the medium and p the pressure, which is supposed to be isotropic. Eliminating the displacement , we obtain a scalar wave equation for the pressure p:
(2.1.2)
Jean-Claude Nédélec
3. Integral Representations and Integral Equations
Abstract
We introduce in this chapter the integral representations of the solutions of the Helmholtz equation. We study the associated integral equations and their main properties. When the wave number k is zero, these integral representations are those associated with the Laplace equation. They have very specific properties. In particular some of the associated integral equations are coercive. We therefore devote special attention to this setting. We will see that they also are the principal parts of the equation associated with the Helmholtz equation.
Jean-Claude Nédélec
4. Singular Integral Operators
Abstract
We present in this chapter the definition and the main properties of the singular integral operator. These results are quite classical and were first studied by Giraud [78] in France and then Calderon and Zygmund in the United States and Michlin in Russia. The present exposition uses some ideas of the notes of V. Neri and the book of E.M. Stein [142]. We establish some continuity results in Sobolev spaces for a class of singular integral operators and then deduce similar properties for the integral operators that we have encountered in the previous chapter.
Jean-Claude Nédélec
5. Maxwell Equations and Electromagnetic Waves
Abstract
Electromagnetic waves are defined by the electric field E and the magnetic field H at each point in R 3. We start by describing their laws of propagation in an isotropic dielectric medium, which is characterized by the electric permittivity ε and the magnetic permeability μ.
Jean-Claude Nédélec
Backmatter
Metadaten
Titel
Acoustic and Electromagnetic Equations
verfasst von
Jean-Claude Nédélec
Copyright-Jahr
2001
Verlag
Springer New York
Electronic ISBN
978-1-4757-4393-7
Print ISBN
978-1-4419-2889-4
DOI
https://doi.org/10.1007/978-1-4757-4393-7