Abstract
We derive the Stokes-Fourier equations in dimension 2 as the limiting dynamics of a system of N hard spheres of diameter ε when N→∞, ε→0, Nε=α→∞, using the linearized Boltzmann equation as an intermediate step. Our proof is based on the strategy of Lanford [6], and on the pruning procedure developed in [3] to improve the convergence time. The main novelty here is that uniform a priori estimates come from a L2 bound on the initial data, the time propagation of which involves a fine symmetry argument and a systematic study of recollisions.
| Original language | English |
|---|---|
| Pages (from-to) | 623-627 |
| Number of pages | 5 |
| Journal | Comptes Rendus Mathematique |
| Volume | 353 |
| Issue number | 7 |
| DOIs | |
| Publication status | Published - 1 Jul 2015 |
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