Skip to main content

1985 | Buch

The Boundary Value Problems of Mathematical Physics

verfasst von: O. A. Ladyzhenskaya

Verlag: Springer New York

Buchreihe : Applied Mathematical Sciences

insite
SUCHEN

Über dieses Buch

In the present edition I have included "Supplements and Problems" located at the end of each chapter. This was done with the aim of illustrating the possibilities of the methods contained in the book, as well as with the desire to make good on what I have attempted to do over the course of many years for my students-to awaken their creativity, providing topics for independent work. The source of my own initial research was the famous two-volume book Methods of Mathematical Physics by D. Hilbert and R. Courant, and a series of original articles and surveys on partial differential equations and their applications to problems in theoretical mechanics and physics. The works of K. o. Friedrichs, which were in keeping with my own perception of the subject, had an especially strong influence on me. I was guided by the desire to prove, as simply as possible, that, like systems of n linear algebraic equations in n unknowns, the solvability of basic boundary value (and initial-boundary value) problems for partial differential equations is a consequence of the uniqueness theorems in a "sufficiently large" function space. This desire was successfully realized thanks to the introduction of various classes of general solutions and to an elaboration of the methods of proof for the corresponding uniqueness theorems. This was accomplished on the basis of comparatively simple integral inequalities for arbitrary functions and of a priori estimates of the solutions of the problems without enlisting any special representations of those solutions.

Inhaltsverzeichnis

Frontmatter
Chapter I. Preliminary Considerations
Abstract
This chapter is of an introductory character and we shall present a series of concepts and theorems from functional analysis which will be used in the sequel for studying boundary value problems for differential equations. These facts will be stated without proof.
O. A. Ladyzhenskaya
Chapter II. Equations of Elliptic Type
Abstract
In this section we shall consider linear second-order equations
$$\begin{array}{*{20}{c}} {Lu = \sum\limits_{{i,j = 1}}^{n} {\frac{\partial }{{\partial {{x}_{i}}}}} ({{a}_{{ij}}}(x){{u}_{{{{x}_{j}}}}} + {{a}_{i}}(x)u(x))} \\ {\quad {\mkern 1mu} + \sum\limits_{{i = 1}}^{n} {{{b}_{i}}} (x){{u}_{{{{x}_{i}}}}} + a(x)u = f(x) + \sum\limits_{{i = 1}}^{n} {\frac{{\partial {{f}_{i}}(x)}}{{\partial {{x}_{i}}}}} ,\quad {{a}_{{ij}}}\left( x \right) = {{a}_{{ji}}}\left( x \right),} \\ \end{array}$$
(1.1)
with real coefficients which satisfy the condition of uniform ellipticity in a bounded domain Ω of Euclidean space R n .
O. A. Ladyzhenskaya
Chapter III. Equations of Parabolic Type
Abstract
In this chapter we shall consider second-order parabolic equations and prove the unique solvability of the initial-boundary value problem in the domains Q T =, (x, t): x ∈ Ω,t ∈ (0, T) for the first, second, and third boundary conditions. We shall assume that the domain Ω is bounded, although all the results, except for the representation of solutions by Fourier series, will be valid for an arbitrary unbounded domain Ω. Moreover, the methods of solution given for bounded Ω are applicable to unbounded Ω (in particular, for Ω = R n ),but need minor modification which we shall point out.
O. A. Ladyzhenskaya
Chapter IV. Equations of Hyperbolic Type
Abstract
Let us recall the information that we shall need from the general theory of hyperbolic equations.
O. A. Ladyzhenskaya
Chapter V. Some Generalizations
Abstract
In this chapter we shall be concerned with a number of more complicated problems which can be treated by the methods discussed in Chapters II–IV.
O. A. Ladyzhenskaya
Chapter VI. The Method of Finite Differences
Abstract
This method of investigating various problems for differential equations consists of reducing them to systems of algebraic equations in which the unknowns are the values of grid functions u Δ at the vertices of the grids ΩΔ, and then examining the limit process when the lengths of the sides of the cells in the grid tend to zero. This brings us to the aim if, in the limit, the functions u Δ, give us the solution of the original problem. Such a reduction of the problem to an infinite sequence of auxiliary finite-dimensional problems defining approximate solutions u Δ is neither unique nor uniform for problems of various types. In other words, for every problem we can construct different difference schemes converging to it, and for problems of various types such schemes differ essentially from each other. In this chapter we shall consider the same boundary value and initial-boundary value problems for the equations of the basic types that we studied in the earlier chapters, and for each of them construct a few elementary difference schemes, which give us in the limit the solutions of these problems. This will be done in such a way that the existence of these solutions will not be stipulated in advance, but, to the contrary, will be established by the method of finite differences. We shall restrict ourselves to “rectangular ” lattices in which the cells will be parallelopipeds with faces parallel to the coordinate planes.
O. A. Ladyzhenskaya
Backmatter
Metadaten
Titel
The Boundary Value Problems of Mathematical Physics
verfasst von
O. A. Ladyzhenskaya
Copyright-Jahr
1985
Verlag
Springer New York
Electronic ISBN
978-1-4757-4317-3
Print ISBN
978-1-4419-2824-5
DOI
https://doi.org/10.1007/978-1-4757-4317-3