We consider a gas in a horizontal slab in which the top and bottom wal
ls are kept at different temperatures. The system is described by the
Boltzmann equation (BE) with Maxwellian boundary conditions specifying
the wall temperatures. We study the behavior of the system when the K
nudsen number epsilon is small and the temperature difference between
the walls as well as the velocity field is of order epsilon, while the
gravitational force is of order epsilon(2). We prove that there exist
s a solution to the BE for t is an element of(0, t) which is near a gl
obal Maxwellian, and whose moments are close, up to order epsilon(2),
to the density, velocity and temperature obtained from the smooth solu
tion of the Oberbeck-Boussinesqequations assumed to exist for t less t
han or equal to (t) over bar.