EuroSummer SchoolInstructional Conference on
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Scientific programmeOn this page you will find a list of speakers and the timetable for the course. Lecture titles, some abstracts and background reading are listed by author below the timetable. Clicking on a speaker's name in the timetable will take you to the information relating to that speaker's lecture or seriesUpdated 18 December 2000 SPEAKERS
TIMETABLEInstructional Lectures will be delivered at three levels: introductory (I); intermediate (M) and advanced (A). Single invited lectures dealing with the application of PDEs are delivered at 4.15.The lectures will be held in the Cedar Suite. N.B. NEW TIMETABLE 18th December 2000
A Aftalion (ENS Paris) Maximum principles for elliptic and parabolic equations (2 lectures) ABSTRACT If u is a convex function in an interval I, then it is well known that u attains its maximum on the boundary of I. This property is a form of the Maximum Principle and can be generalized in dimension N for functions u with D u ³ 0 or more generally with Mu + c (x) u ³ 0 where M is an elliptic operator and c (x) £ 0. A form of the Maximum Principle is that u reaches its maximum on the boundary if it is not constant. Another form is that if Mu + c (x) u ³ 0 in the domain and u £ 0 on the boundary then u £ 0 in the whole domain. In these lectures, we will give a review of the various forms of the Maximum Principle (MP): weak MP, strong MP, Hopf MP. We will give sufficient conditions for the MP to hold for a general elliptic operator: a usual condition is c (x) £ 0 but we will see for instance that it also holds with any c (x) for narrow domains or domains with small volume. Then we will give applications of the Maximum Principle to derive uniqueness and symmetry properties for solutions of elliptic PDEs. For parabolic PDE's, the Maximum Principle states that the maximum is reached either on the boundary of the domain or at time t = 0. We will give various versions of the Maximum Principle for parabolic equations and give applications to uniqueness results.
L Ambrosio (Pisa)
J M Ball (Oxford) Microstructure and energy minimization (3 lectures) Many materials (e.g. alloys) undergo solid phase transformations involving a change of shape at some critical temperature. Such phase transformations result in patterns of fine microstructure, whose morphology is important for determining the macroscopic response of the material. A central model for such materials is nonlinear elasticity, with a stored-energy function that is 'non-elliptic'. The analysis of minimizers and minimizing sequences for the total elastic energy then provides key information about microstructure morphology. Crucial to this analysis are tools for passing from microscales to macroscales such a weak convergence, Young measures and quasiconvexity.
Y Brenier (Paris VI) Lect 1. Volume preserving maps and incompressible fluids I Lect 2. Volume preserving maps and incompressible fluids II Lect 3. Hydrodynamic limits of Plasma equations Return to timetable G R Burton (Bath) Lecture 1: Nonlinear Functional Analysis Weak convergence, weak compactness and convexity are important tools for proving existence in the Calculus of Variations. With this application in mind we will study weak continuity and semicontinuity in a nonlinear context. Preparation should include familiarity with the basics of linear functional analysis, including Banach spaces, the Hahn-Banach theorem, reflexivity, weak and weak* topologies, and the (Banach-Alaoglu) theorem on weak* compactness of a ball, as covered in:
The lectures will revolve around the notion of a rearrangement of a function. In the context of variational problems posed on Sobolev spaces, various symmetrisation procedures allow the functions in a given minimising sequence to be rearranged into more symmetrical versions to form a minimising sequence with better compactness properties. The set of all (generally unsymmetric) rearrangements of a given function is of interest in its own right, being a physically natural constraint set for some variational problems in fluid mechanics. Preparation should include familiarity with Lebesgue integration, the definitions of Sobolev spaces, and the statements of the Sobolev embedding theorem and the Rellich-Kondrachov compact embedding theorem, as covered in:
V Caselles (Barcelona) PDEs in image processing - statics & dynamics (2 lectures) Return to timetable N Dancer (Sydney) Peak solutions of nonlinear elliptic equations and their stability. Return to timetable M J Esteban (Paris Dauphine) Variational methods in mathematical physics (2 lectures) This course, which follows that of Professor C.A. Stuart, will be devoted to the presentation of the modern tools of non-compact variational problems. These problems appear quite often in the modelling of physical phenomena, and more particularly in quantum mechanics and atomic physics. Non-compact phenomena are also related to the consideration of the so-called critical exponents in equations coming from differential geometry. The main method to be described in this course is the so-called concentration-compactness method, introduced by P.-L. Lions to deal with general non-compact situation in variational situations. Previous ways to treat this difficulty include the work of some geometers like Uhlenbeck, Schoen, etc. and also in PDEs including the critical exponents, the work of Brezis and Nirenberg.
J Kristensen (Heriot Watt) Linear and multilinear algebra for nonlinear systems (3 lectures) Return to timetable C Le Bris (Ecole Nationale des Ponts et Chaussees) PDEs in physics and chemistry - variational methods in atomic physics (2 lectures) Return to timetable A Quarteroni (EPFL Lausanne) Mathematical models for blood dynamics Return to timetable C A Stuart (EPFL Lausanne) The calculus of variations (3 lectures) A .dvi file of the abstract is available to download here. Return to timetable J F Toland (Bath) PDEs in wave theories Return to timetable N Touzi (Paris) Mathematical modelling of the hedging problem in finance Return to timetable |
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