|
" Convexity Methods in Hamiltonian Mechanics "
by Ivar Ekeland.
| Document Type
|
:
|
BL
|
| Record Number
|
:
|
753308
|
| Doc. No
|
:
|
b573269
|
| Main Entry
|
:
|
by Ivar Ekeland.
|
| Title & Author
|
:
|
Convexity Methods in Hamiltonian Mechanics\ by Ivar Ekeland.
|
| Publication Statement
|
:
|
Berlin, Heidelberg : Springer Berlin Heidelberg, 1990
|
| Series Statement
|
:
|
Ergebnisse der Mathematik und ihrer Grenzgebiete, A Series of Modern Surveys in Mathematics, 19.
|
| Page. NO
|
:
|
(x, 247 pages 4 illustrations)
|
| ISBN
|
:
|
3540506136
|
|
|
:
|
: 3642743315
|
|
|
:
|
: 9783540506133
|
|
|
:
|
: 9783642743313
|
| Contents
|
:
|
I. Linear Hamiltonian Systems --; 1. Floquet Theory and Stability --; 2. Krein Theory and Strong Stability --; 3. Time-Dependence of the Eigenvalues of R (t) --; 4. Index Theory for Positive Definite Systems --; 5. The Iteration Formula --; 6. The Index of a Periodic Solution to a Nonlinear Hamiltonian System --; 7. Examples --; 8. Non-periodic Solutions: The Mean Index --; II. Convex Hamiltonian Systems --; 1. Fundamentals of Convex Analysis --; 2. Convex Analysis on Banach Spaces --; 3. Integral Functionals on L? --; 4. The Clarke Duality Formula --; III. Fixed-Period Problems: The Sublinear Case --; 1. Subquadratic Hamiltonians --; 2. An Existence Result --; 3. Autonomous Systems --; 4. Nonautonomous Systems --; 5. Other Problems --; IV. Fixed-Period Problems: The Superlinear Case --; 1. Mountain-Pass Points --; 2. A Preliminary Existence Result --; 3. The Index at Mountain-Pass Points --; 4. Subharmonics --; 5. Autonomous Problems and Potential Wells --; V. Fixed-Energy Problems --; 1. Existence, Length, Stability --; 2. Multiplicity in the Pinched Case --; 3. Multiplicity in the General Case --; 4. Open Problems.
|
| Abstract
|
:
|
In the case of completely integrable systems, periodic solutions are found by inspection. For nonintegrable systems, such as the three-body problem in celestial mechanics, they are found by perturbation theory: there is a small parameter € in the problem, the mass of the perturbing body for instance, and for € = 0 the system becomes completely integrable. One then tries to show that its periodic solutions will subsist for € -# 0 small enough. Poincare also introduced global methods, relying on the topological properties of the flow, and the fact that it preserves the 2-form L~=l dPi 1\ dqi' The most celebrated result he obtained in this direction is his last geometric theorem, which states that an area-preserving map of the annulus which rotates the inner circle and the outer circle in opposite directions must have two fixed points. And now another ancient theme appear: the least action principle. It states that the periodic solutions of a Hamiltonian system are extremals of a suitable integral over closed curves. In other words, the problem is variational. This fact was known to Fermat, and Maupertuis put it in the Hamiltonian formalism. In spite of its great aesthetic appeal, the least action principle has had little impact in Hamiltonian mechanics. There is, of course, one exception, Emmy Noether's theorem, which relates integrals ofthe motion to symmetries of the equations. But until recently, no periodic solution had ever been found by variational methods.
|
| Subject
|
:
|
Differential equations, Partial.
|
| Subject
|
:
|
Mathematical optimization.
|
| Subject
|
:
|
Mathematics.
|
| LC Classification
|
:
|
QA614.83B958 1990
|
| Added Entry
|
:
|
Ivar Ekeland
|
| |