21 research outputs found

    Approach to a stationary state in an external field

    Get PDF
    International audienceWe study relaxation towards a stationary out of equilibrium state by analizing a one-dimensional stochastic process followed by a particle accelerated by an external field and propagating through a thermal bath. The effect of collisions is described within Botlzmann's kinetic theory. We present analytical solutions for the Maxwell gas and for the very hard particle model. The exponentially fast relaxation of the velocity distribution toward the stationary form is demonstrated. In the reference frame moving with constant drift velocity the hydrodynamic diffusive mode is shown to govern the distribution in the position space. We show that the exact value of the diffusion coefficient for any value of the field is correctly predicted by Green-Kubo autocorrelation formula generalized to the stationary state

    Front localization in a ballistic annihilation model

    Full text link
    We study the possibility of localization of the front present in a one-dimensional ballistically-controlled annihilation model in which the two annihilating species are initially spatially separated. We construct two different classes of initial conditions, for which the front remains localized.Comment: Using elsart (Elsevier Latex macro) and epsf. 12 Pages, 2 epsf figures. Submitted to Physica

    Kinetic models of ion transport through a nanopore

    Full text link
    Kinetic equations for the stationary state distribution function of ions moving through narrow pores are solved for a number of one-dimensional models of single ion transport. Ions move through pores of length LL, under the action of a constant external field and of a concentration gradient. The interaction of single ions with the confining pore surface and with water molecules inside the pore are modelled by a Fokker-Planck term in the kinetic equation, or by uncorrelated collisions with thermalizing centres distributed along the pore. The temporary binding of ions to polar residues lining the pore is modelled by stopping traps or energy barriers. Analytic expressions for the stationary ion current through the pore are derived for several versions of the model, as functions of key physical parameters. In all cases, saturation of the current at high fields is predicted. Such simple models, for which results are analytic, may prove useful in the study of the current/voltage relations of ion channels through membranes

    Self-consistent equation for an interacting Bose gas

    Full text link
    We consider interacting Bose gas in thermal equilibrium assuming a positive and bounded pair potential V(r)V(r) such that 0<\int d\br V(r) = a<\infty. Expressing the partition function by the Feynman-Kac functional integral yields a classical-like polymer representation of the quantum gas. With Mayer graph summation techniques, we demonstrate the existence of a self-consistent relation ρ(μ)=F(μaρ(μ))\rho (\mu)=F(\mu-a\rho(\mu)) between the density ρ\rho and the chemical potential μ\mu, valid in the range of convergence of Mayer series. The function FF is equal to the sum of all rooted multiply connected graphs. Using Kac's scaling V_{\gamma}(\br)=\gamma^{3}V(\gamma r) we prove that in the mean-field limit γ0\gamma\to 0 only tree diagrams contribute and function FF reduces to the free gas density. We also investigate how to extend the validity of the self-consistent relation beyond the convergence radius of Mayer series (vicinity of Bose-Einstein condensation) and study dominant corrections to mean field. At lowest order, the form of function FF is shown to depend on single polymer partition function for which we derive lower and upper bounds and on the resummation of ring diagrams which can be analytically performed.Comment: 33 pages, 6 figures, submitted to Phys.Rev.

    The linearized kinetic equation for a classical gas

    No full text
    The linearized kinetic equation satisfied by the one-particle velocity distribution function of a classical gas is derived. The explicit dependence of the corresponding generalized Boltzmann operator on the equilibrium correlations is displayed. © 1972.SCOPUS: ar.jinfo:eu-repo/semantics/publishe

    Echelles de temps en théorie cinétique

    No full text
    corecore