2016
DOI: 10.1103/physreve.94.040103
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Kinetic equation and nonequilibrium entropy for a quasi-two-dimensional gas

Abstract: A kinetic equation for a dilute gas of hard spheres confined between two parallel plates separated a distance smaller than two particle dimeters is derived. It is a Boltzmann-like equation, which incorporates the effect of the confinement on the particle collisions. A function S(t) is constructed by adding to the Boltzmann expression a confinement contribution. Then it is shown that for the solutions of the kinetic equation, S(t) increases monotonically in time, until the system reaches a stationary inhomogene… Show more

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Cited by 14 publications
(43 citation statements)
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“…The Boltzmann equation, describing the time evolution of the one-particle distribution function, f (r, v, t) for a dilute gas of inelastic hard spheres of mass m and diameter σ, confined between two large hard parallel plates separated a distance h smaller than twice the diameter of a particle, σ < h < 2σ, has the form [21][22][23] ∂f ∂t…”
Section: Description Of the System And Balance Equationsmentioning
confidence: 99%
See 1 more Smart Citation
“…The Boltzmann equation, describing the time evolution of the one-particle distribution function, f (r, v, t) for a dilute gas of inelastic hard spheres of mass m and diameter σ, confined between two large hard parallel plates separated a distance h smaller than twice the diameter of a particle, σ < h < 2σ, has the form [21][22][23] ∂f ∂t…”
Section: Description Of the System And Balance Equationsmentioning
confidence: 99%
“…The equation can be applied, to both elastic [21,22] and inelastic particles [23,24]. The only difference is in the collision rule used to determine the change of the velocities when two particles collide.…”
Section: Introductionmentioning
confidence: 99%
“…By using a slight modification of the standard way of deriving the usual (bulk) Boltzmann and Enskog kinetic equations [22], it has been shown that the one particle distribution function f (r, v, t) of the confined system of hard spheres in the low density limit satisfies the equation [23] …”
Section: Back To the Origins: Boltzmann-enskog Kinetic Equationmentioning
confidence: 99%
“…It is then proven [23] that in a system with elastic walls, H(t) is bounded from below, and that ∂ t H(t) ≤ 0, the equal sign holding only if…”
Section: Back To the Origins: Boltzmann-enskog Kinetic Equationmentioning
confidence: 99%
“…The remaining of this paper is organized as follows. In the next section the Boltzmann equation for a strongly confined gas of hard spheres [13,14] is shortly reviewed and extended to the case of smooth inelastic particles. Also, the inhomogeneous cooling state (ICS) is introduced and the condition of isotropic cooling rate is deduced.…”
Section: Introductionmentioning
confidence: 99%