We consider the Boltzmann equation for a gas in a horizontal slab, subject to a gravitational force. The boundary conditions are of diffusive type, specifying the wall temperatures, so that the top temperature is lower than the bottom one (Benard setup). We consider a 2-dimensional convective stationary solution, which is close for small Knudsen number to the convective stationary solution of the OberbeckBoussinesq equations, near above the bifurcation point, and prove its stability under 2-d small perturbations, for Rayleigh number above and close to the bifurcation point and for small Knudsen number.
This paper deals with mathematical questions for Bose gases below the temperature T BEC where Bose-Einstein condensation sets in. The model considered is of two-component type, consisting of a kinetic equation for the distribution function of a gas of (quasi-)particles interacting with a Bose condensate, which is described by a Gross-Pitaevskii equation. Existence results and moment estimates are proved in the space-homogeneous, isotropic case.
The stationary Povzner equation is considered in a bounded and strictly convex domain of R " . Existence theorems are established for a class of collision kernels in the case of hard forces and for diffuse reflection boundary c o n d itio n s. Generalizations with respect to the collision kernel a n d boundary conditions are discussed.
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