Skip to main content
Top

Selected Chapters in the Calculus of Variations

  • 2003
  • Book
insite
SEARCH

About this book

0.1 Introduction These lecture notes describe a new development in the calculus of variations which is called Aubry-Mather-Theory. The starting point for the theoretical physicist Aubry was a model for the descrip­ tion of the motion of electrons in a two-dimensional crystal. Aubry investigated a related discrete variational problem and the corresponding minimal solutions. On the other hand, Mather started with a specific class of area-preserving annulus mappings, the so-called monotone twist maps. These maps appear in mechanics as Poincare maps. Such maps were studied by Birkhoff during the 1920s in several papers. In 1982, Mather succeeded to make essential progress in this field and to prove the existence of a class of closed invariant subsets which are now called Mather sets. His existence theorem is based again on a variational principle. Although these two investigations have different motivations, they are closely re­ lated and have the same mathematical foundation. We will not follow those ap­ proaches but will make a connection to classical results of Jacobi, Legendre, Weier­ strass and others from the 19th century. Therefore in Chapter I, we will put together the results of the classical theory which are the most important for us. The notion of extremal fields will be most relevant. In Chapter II we will investigate variational problems on the 2-dimensional torus. We will look at the corresponding global minimals as well as at the relation be­ tween minimals and extremal fields. In this way, we will be led to Mather sets.

Table of Contents

Frontmatter
Chapter 1. One-dimensional variational problems
Abstract
Let Ωbe an open region in ℝn+1. We assume that Ω is simply connected. A point in Ω has the coordinates (t, x1, ..., xn) = (t, x. Let F = F(t, x, p) ∈ C r (Ω × ℝ n ) with r ≥ 2 and let (t1a) and (t2b)be two points in Ω. The space
$$\Gamma : = \{ \gamma :t \to x(t) \in \Omega |x \in {{C}^{1}}[{{t}_{1}},{{t}_{2}}], x({{t}_{1}}) = a,x({{t}_{2}}) = b\}$$
consists of all continuously differentiable curves which start at (tla) and end at (t2b).On Г is defined the functional
$$I(\gamma ) = \int_{{{{t}_{1}}}}^{{{{t}_{2}}}} {F(t,x(t),\dot{x}(t))dt.}$$
Jürgen Moser, Oliver Knill
Chapter 2. Extremal fields and global minimals
Abstract
The two-dimensional torus has the standard representation \({{\mathbb{T}}^{2}} = {{\mathbb{R}}^{2}}/{{\mathbb{Z}}^{2}}\). We often will work on its covering surface ℝ2 where everything is invariant under its fundamental group ℤ2. In this chapter we deal with the variational principle ∫F(t,x,p) dt on ℝ2, whereF is assumed to satisfy the following properties:
i)
FC2(\({{\mathbb{T}}^{2}} \times {{\mathbb{R}}^{2}}\)):
$$\begin{array}{*{20}{c}} {a)F \in {{C}^{2}}({{\mathbb{R}}^{3}}),} \hfill \\ {b)F(t + 1,x,p) = F(t,x + 1,p) = F(t,x,p).} \hfill \\ \end{array}$$
(2.1)
 
ii)
F has quadratic growth: There exist δ > 0, c > 0 such that
$$\begin{array}{*{20}{c}} {c) \delta \leqslant {{F}_{{pp}}} \leqslant {{\delta }^{{ - 1}}},} \hfill \\ {d)|{{F}_{x}}| \leqslant c(1 + {{p}^{2}}),} \hfill \\ {e) |{{F}_{{tp}}}| + |{{F}_{{px}}}| \leqslant c(1 + |p|).} \hfill \\ \end{array}$$
(2.2)
 
Jürgen Moser, Oliver Knill
Chapter 3. Discrete Systems, Applications
Abstract
In this chapter we consider situations which are closely related to the questions in Chapter II. Indeed, they are more or less the same questions, even though the assumptions are not identical. The topics require some small changes. But the underlying ideas remain the same.
Jürgen Moser, Oliver Knill
Backmatter
Metadata
Title
Selected Chapters in the Calculus of Variations
Authors
Jürgen Moser
Oliver Knill
Copyright Year
2003
Publisher
Birkhäuser Basel
Electronic ISBN
978-3-0348-8057-2
Print ISBN
978-3-7643-2185-7
DOI
https://doi.org/10.1007/978-3-0348-8057-2