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1997 | Buch

G-Convergence and Homogenization of Nonlinear Partial Differential Operators

verfasst von: Alexander Pankov

Verlag: Springer Netherlands

Buchreihe : Mathematics and Its Applications

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Über dieses Buch

Various applications of the homogenization theory of partial differential equations resulted in the further development of this branch of mathematics, attracting an increasing interest of both mathematicians and experts in other fields. In general, the theory deals with the following: Let Ak be a sequence of differential operators, linear or nonlinepr. We want to examine the asymptotic behaviour of solutions uk to the equation Auk = f, as k ~ =, provided coefficients of Ak contain rapid oscillations. This is the case, e. g. when the coefficients are of the form a(e/x), where the function a(y) is periodic and ek ~ 0 ask~=. Of course, of oscillation, like almost periodic or random homogeneous, are of many other kinds interest as well. It seems a good idea to find a differential operator A such that uk ~ u, where u is a solution of the limit equation Au = f Such a limit operator is usually called the homogenized operator for the sequence Ak . Sometimes, the term "averaged" is used instead of "homogenized". Let us look more closely what kind of convergence one can expect for uk. Usually, we have some a priori bound for the solutions. However, due to the rapid oscillations of the coefficients, such a bound may be uniform with respect to k in the corresponding energy norm only. Therefore, we may have convergence of solutions only in the weak topology of the energy space.

Inhaltsverzeichnis

Frontmatter
Chapter 1. G-convergence of Abstract Operators
Abstract
Here we fix notations and recall some results concerning multivalued operators.
Alexander Pankov
Chapter 2. Strong G-convergence of Nonlinear Elliptic Operators
Abstract
Let (X, T) be a measurable space, i.e. X is a set and T is a σ-field of subsets of X, F: XR n a multivalued map with non-empty values. For any subset BR n we define the inverse image of B under F as
$${F^{ - 1}}(B) = \{ x \in X:B \cap Fx \ne \phi \}$$
.
Alexander Pankov
Chapter 3. Homogenization of Elliptic Operators
Abstract
We start with an analytic description of random homogeneous fields on R n . In the case n = 1 they are called, usually, random stationary processes. Let us consider a probability space Ω, i.e. a set equipped with a σ-algebra F of measurable subsets and a countably additive non-negative measure μ on F normalized by μ(Ω) = 1. We always assume the measure μ to be complete. An n-dimensional dynamical system is defined as a family of selfmaps
$$T\left( x \right):\Omega \to \Omega , x \in {R^n},$$
with the following properties:
(1)
T(x + y) = T (x)T (y), x, y ∈ R n, and T (0) = I;
 
(2)
the map T(x) is measure preserving, i.e. for any x ∈ R n and for any μ-measurable subset U ⊂ Ω, the set T(x)U is μ-measurable and
$$\mu \left( {T\left( x \right)u} \right) = \mu \left( u \right);$$
 
(3)
the map
$$T:{R^n} \times \Omega \to \Omega , T:\left( {x,\omega } \right) \mapsto T\left( x \right)\omega ,$$
is measurable, where R n × Ω is endowed with the measure dx ⨂μ,dx stands for the Lebesgue measure.
 
Alexander Pankov
Chapter 4. Nonlinear Parabolic Operators
Abstract
Let Q 0R n be a bounded open set and Q = (0, T) × Q 0. On Q, we shall consider evolution operators of the form
$$\angle u = {\partial _t}u - div a(t,x,u,\nabla u) + {a_0}(t,x,u,\nabla u),$$
(4.1.1)
where ∂ t = ∂/∂t. We assume that the functions
$$a:Q \times R \times {R^n} \to {R^n}$$
and
$${a_0}:Q \times R \times {R^n} \to R$$
satisfy the Catathéodory condition and the following inequalities:
Alexander Pankov
Backmatter
Metadaten
Titel
G-Convergence and Homogenization of Nonlinear Partial Differential Operators
verfasst von
Alexander Pankov
Copyright-Jahr
1997
Verlag
Springer Netherlands
Electronic ISBN
978-94-015-8957-4
Print ISBN
978-90-481-4900-1
DOI
https://doi.org/10.1007/978-94-015-8957-4