The texts in this volume deal mostly with various aspects of the theory of nonlinear partial differential equations. They present both theoretical and applied results in many fields of growing importance such as Calculus of variations and optimal control, optimization, system theory and control, operations research, fluids and continuum mechanics, nonlinear dynamics, meteorology and climate, homogenization and material science, numerical analysis and scientific computations
The book is of interest to everyone from postgraduate, who wishes to follow the most recent progress in these fields.
18.07
This book contains the written versions of lectures delivered since 1997 in the well-known weekly seminar on Applied Mathematics at the College de France in Paris, directed by Jacques-Louis Lions. It is the 14th and last of the series, due to the recent and untimely death of Professor Lions. The texts in this volume deal mostly with various aspects of the theory of nonlinear partial differential equations. They present both theoretical and applied results in many fields of growing importance such as Calculus of variations and optimal control, optimization, system theory and control, operations research, fluids and continuum mechanics, nonlinear dynamics, meteorology and climate, homogenization and material science, numerical analysis and scientific computations The book is of interest to everyone from postgraduate, who wishes to follow the most recent progress in these fields.
Cover 1
Contents 7
Preface 9
Chapter 1. An introduction to critical points for integral functionals 10
Chapter 2. A semigroup formulation for electromagnetic waves in dispersive dielectric media 22
Chapter 3. Limite non visqueuse pour les fluides incompressibles axisymétriques 38
Chapter 4. Global properties of some nonlinear parabolic equations 66
Chapter 5. A model for two coupled turbulent flows. Part I: analysis of the system 78
Chapter 6. Détermination de conditions aux limites en mer ouverte par une méthode de controle optimal 112
Chapter 7. Effective diffusion in vanishing viscosity 142
Chapter 8. Vibration of a thin plate with a "rough" surface 156
Chapter 9. Anisotropy and dispersion in rotating fluids 180
Chapter 10. Integral equations and saddle point formulation for scattering problems 202
Chapter 11. Existence and uniqueness of a strong solution for nonhomogeneous micropolar fluids 222
Chapter 12. Homogenization of Dirichlet minimum problems with conductor type periodically distributed constraints 252
Chapter 13. Transport of trapped particles in a surface potential 282
Chapter 14. Diffusive energy balance models in climatology 306
Chapter 15. Uniqueness and stability in the Cauchy problem for Maxwell and elasticity systems 338
Chapter 16. On the unstable spectrum of the Euler equation 360
Chapter 17. Décomposition en profils des solutions de l'équation des ondes semi linéaire critique á l'extérieur d'un obstacle strictement convexe 376
Chapter 18. Upwind discretizations of a steady grade-two fluid model in two dimensions 402
Chapter 19. Stability of thin layer approximation of electromagnetic waves scattering by linear and non linear coatings 424
Chapter 20. Remarques sur la limite a -> 0 pour les fluides de grade 2
Chapter 21. Remarks on the Kompaneets equation, a simplified model of the Fokker-Planck equation 478
Chapter 22. Singular perturbations without limit in the energy space. Convergence and computation of the associated layers 498
Chapter 23. Optimal design of gradient fields with applications to electrostatics 518
Chapter 24. A blackbox reduced-basis output bound method for noncoercive linear problems 542
Chapter 25. Simulation of flow in a glass tank 580
Chapter 26. Control localized on thin structures for semilinear parabolic equations 600
Chapter 27. Stabilité des ondes de choc de viscosité qui peuvent être caractéristiques 656
An Introduction to Critical Points for Intergral Functionals
David Arcoya darcoya@ugr.es Departamento de Análisis Matemático, Universidad de Granada, 18071-Granada, Spain
Lucio Boccardo boccardo@mat.uniromal.it Dipartimento di Matematica, Università di Roma 1, Piazza A. Moro 2, 00185 Roma, Italy
1 Introduction
The study of minima of functionals defined in spaces of functions may be considered one of the keystones of the mathematical analysis. Remind the efforts by the great mathematicians of the last and present century to develop sufficient conditions on the functional for the existence of minimum. This theory is deeply related with the existence of solutions of boundary value problems. Indeed, this connection is estabilished by the well-known Euler-Lagrange equations associated to the functional.
However, there exist boundary value problems for which the associated functional is indefinite, i.e. it is unbounded from below and from above. This means that it has not global extrema and so we have to search the solutions of the problem among the critical points, i.e. the points for which the derivative of the functional vanishes.
From the abstract point of view there is a difference between the study of minima and of critical points. Indeed, for the existence of minima we need only assumptions on the functional. On the contrary, we point out that the results of existence of critical points involve additional hypotheses on the regularity of the functional to assure the existence of a derivative in some sense. This may explain why the theory of mimima handles classes of functionals with more general hypotheses of smoothness than the critical point theory.
In some papers [4], [5], [6], we overcame this difference by developing a critical point theory for nondifferentiable functionals. We observe explicitely that our model functionals does not involve similar functions to the modulus. In fact, the nondifferentiability of the considered functionals is due to the introduction of some smooth Carathéodory function A(x, u) (as smooth as you want). Specifically, we consider here functionals J defined in 01,2Ω (Ω ⊂ N open, N > 1) by
v=∫ΩAx,v|∇v|2dx−∫ΩFx,v+dx,v∈W01,2Ω,
(1)
with <α≤Ax,z≤β<∞,|A′zx,z|≤γ and f(x, z) ≡ F′(x, z)(derivative respect to z) a subcritical Carathéodory function. Observe that J is only differentiable along directions of 01,2Ω∩L∞Ω, even for smooth functions A (see [11]).
This note is devoted to present the critical point theory developed in [5] (see also [?, ?, ?, ?, ?, ?, ?]) for functionals which are not differentiable in all directions.
2 A mountain pass theorem for nondifferentiable functionals
Our abstract setting for the functionals J that we study is given by the following asumption:
(H)(X, || · ||X) is a Banach space and Y ⊂ X is a subspace which is a normed space endowed with a norm || · ||Y. Moreover, J : X → is a functional on X such that it is continuous in (Y, || · ||X + || · ||Y) and satisfies the following hypotheses:
a) J has a directional derivative 〈J′(u), v〉 at each u ∈ X through any direction v ∈ Y.
b) For fixed u ∈ X, the function 〈J′(u), v〉 is linear in v ∈ Y, and for fixed v ∈ Y, the function 〈J′(u), v〉 is continuous in u ∈ X.
Due to the lack of regularity of the functional, some words are needed in order to establish our definition of critical points.
Definition 2.1
A function u ∈ X is called a critical point of J if
J′u,v〉=0,∀v∈Y.
In this framework a suitable version of the Ambrosetti-Rabinowitz Theorem has been proved in [5]. Specifically,
Theorem 2.2
Assume (H) and that for e ∈ Y,
=infγ∈Γmaxt∈0,1Jγt>c1=max{J0,Je}
with Γ the set of the continuous paths γ : [0, 1] → (Y, || · ||X + || · ||Y), such that γ(0) = 0 and γ(1) = e. Suppose, in addition, that J satisñes the condition
(C) Any sequence {un} in the Banach space Y satisfying for some {Kn} ⊂ + and {εn} → 0 the conditions
Jun}isbounded,
(2)
un‖Y≤2Kn∀n∈Y,
(3)
〈J′un,v〉|≤εn[‖v‖YKn+‖v‖X]∀v∈Y,
(4)
possesses a convergent subsequence in X.
Then there exists a nonzero critical point u ∈ Y of J such that J(u) = c.
Remarks 2.3
1. The proof of this theorem is done by dividing it into two steps. In the first one, only the geometric hypotheses are used to deduce the existence of a sequence {un} in Y satisfying for some {Kn} ⊂ + and {εn} → 0 the conditions (2)–(4). The proof is then concluded by using condition (C).
2. In this way, condition (C) can be considered as a compactness condition on the functional J, which substitutes in the nondifferentiable case the role done by the well-known Palais-Smale condition in the regular case Y = X.
3. This compactness condition is connected with the coercivity of J extending the previous results for C1 functionals in [11]. To be specifìcal in [7] we prove
Theorem 2.4
In addition to (H), assume that Y is dense in X and that J is continuous in X and bounded from below. If J satisfies condition (C) then J is coercive, i.e.,
‖u‖x→∞Ju=∞.
3 A simple model
The application of the abstract result quoted in the previous section to the study of the functional J defined in (1) is very technical. In particular, the verification of the condition (C). For this reason, we present here a simple but not natural functional which is not differentiable in 01,2Ω, but for which the verification of condition (C) has not technical difficulties like for functionals studied in [5], [6]. Specifically, we consider the functional J defined in 01,2Ω by setting
v=12fΩ|∇v|2dx+1qfΩax,v|∇v|qdx−1mfΩv+mdx,v∈W01,2Ω,}
(5)
where 1 ≤ q < 2 < m < 2* (2* = 2N/(N – 2), if 2 < N; 2* = ∞ if N ≤ 2) and a : Ω × → is a function which is measurable respect to x ∈ Ω, C1 with respect to z ≠ 0 and such that
(a1) There exist β > α > 0 such that
≤ax,z≤β,
for almost every x ∈ Ω and z ∈ .
(a2) There exists γ > 0 such that
a′zx,z|≤γ,foralmosteveryx∈Ω,∀z>0,
and a′(x, z) = 0, z < 0.
(a3)...
Erscheint lt. Verlag | 21.6.2002 |
---|---|
Sprache | englisch |
Themenwelt | Mathematik / Informatik ► Mathematik ► Algebra |
Mathematik / Informatik ► Mathematik ► Analysis | |
Mathematik / Informatik ► Mathematik ► Angewandte Mathematik | |
Technik | |
ISBN-10 | 0-08-053767-7 / 0080537677 |
ISBN-13 | 978-0-08-053767-2 / 9780080537672 |
Haben Sie eine Frage zum Produkt? |
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