a1 Department of Mechanical Engineering and Science and Advanced Research Institute of Fluid Science and Engineering, Graduate School of Engineering, Kyoto University, Kyoto 606-8501, Japan. aoki@aero.mbox.media.kyoto-u.ac.jp
a2 Dipartimento di Matematica, Università di Roma “La Sapienza", Piazzale A. Moro 2, 00185, Roma, Italy. cavallar@mat.uniroma1.it; marchior@mat.uniroma1.it; pulvirenti@mat.uniroma1.it
Abstract
We consider a body immersed in a perfect gas and moving under the action of a constant force.
Body and gas are in thermal equilibrium. We assume a stochastic interaction body/medium: when a particle of the medium hits the body,
it is absorbed and immediately re-emitted with a Maxwellian distribution. This system gives rise to a microscopic model of friction.
We study the approach of the body velocity V(t) to the limiting velocity
and prove that, under suitable smallness
assumptions, the approach to equilibrium is
where d is the dimension of the space, and C is a positive constant. This approach is not exponential, as typical in
friction problems, and even slower than for the same problem with elastic collisions.
(Received March 31 2007)
(Revised October 16 2007)
(Online publication March 27 2008)
Key Words:
Mathematics Subject Classification:
limit of interacting classical particles.
Comm. Math. Phys.
56 (1977) 101–113.
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