“…. from a solid surface [1,2]. To each atom A j , one assigns its mass m j > 0, its radius R j > 0, a sequence of "collisional" masses {M n,j } n≥1 (0 < M n,j ≤ +∞), a sequence of "Maxwellian" masses {µ n,j } n≥1 (0 < µ n,j ≤ +∞), and a sequence {L n,j } n≥1 of laws of the change in the "horizontal" component of the atom velocity (of course, it is assumed that the choice of these masses and laws is physically motivated).…”