Abstract

This paper is concerned with the homogenization of some particle systems with two-body interactions in dimension one and of dislocation dynamics in higher dimensions. The dynamics of our particle systems are described by some ODEs. We prove that the rescaled ``cumulative distribution function'' of the particles converges towards the solution of a Hamilton-Jacobi equation. In the case when the interactions between particles have a slow decay at infinity as $1/x$, we show that this Hamilton-Jacobi equation contains an extra diffusion term which is a half Laplacian. We get the same result in the particular case where the repulsive interactions are exactly $1/x$, which creates some additional difficulties at short distances. We also study a higher dimensional generalisation of these particle systems which is particularly meaningful to describe the dynamics of dislocations lines. One main result of this paper is the discovery of a satisfactory mathematical formulation of this dynamics, namely a Slepcev formulation. We show in particular that the system of ODEs for particle systems can be naturally imbedded in this Slepcev formulation. Finally, with this formulation in hand, we get homogenization results which contain the particular case of particle systems.

Highlights

  • 1.1 Homogenization of particle systemsIn this work, we study a system of ODEs describing the dynamics of particles with two-body interactions

  • We study a system of ODEs describing the dynamics of particles with two-body interactions

  • Where F is a constant given force, V0 is a 1-periodic potential and V is a potential taking into account two-body interactions

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Summary

Homogenization of particle systems

We study a system of ODEs describing the dynamics of particles with two-body interactions. The typical example we have in mind is the dynamics of dislocation straight lines In this case, the potential V (y) is given by − ln |y| and yi is the “position” of dislocation straight lines. We will prove that the limit ρ0 of ρε as ε → 0 exists and is the (unique) solution of a homogenized (or effective) equation. Where H0 is a continuous function and I1 is a Levy operator of order 1 associated with the function g0 appearing in (2). It is defined for any function U ∈ Cb2(R) for r > 0 by.

Homogenization of dislocation dynamics
General homogenization results
Physical derivation of the model for dislocation dynamics
Definition of viscosity solutions
Comparison principles
Existence results
Consistency of the definition of the geometric motion
Ergodicity
The proof of convergence
Qualitative properties of the effective Hamiltonian
Gradient estimates
Sub- and supercorrectors
Findings
The general case
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