Ionic diffusion through and near small domains is of considerable importance inmolecular biophysics in applications such as permeation through protein channelsand diffusion near the charged active sites of macromolecules. The motion of theions in these settings depends on the specific nanoscale geometry and chargedistribution in and near the domain, so standard continuum type approaches haveobvious limitations. The standard machinery of equilibrium statistical mechanicsincludes microscopic details, but is also not applicable, because these systems areusually not in equilibrium due to concentration gradients and to the presence of anexternal applied potential, which drive a non-vanishing stationary current throughthe system. We present a stochastic molecular model for the diffusive motion ofinteracting particles in an external field of force and a derivation of effective partialdifferential equations and their boundary conditions that describe the stationarynon-equilibrium system. The interactions can include electrostatic, Lennard-Jones andother pairwise forces. The analysis yields a new type of Poisson–Nernst–Planck equations,that involves conditional and unconditional charge densities and potentials. Theconditional charge densities are the non-equilibrium analogues of the well studied paircorrelation functions of equilibrium statistical physics. Our proposed theory isan extension of equilibrium statistical mechanics of simple fluids to stationarynon-equilibrium problems. The proposed system of equations differs from thestandard Poisson–Nernst–Planck system in two important aspects. First, the forceterm depends on conditional densities and thus on the finite size of ions, andsecond, it contains the dielectric boundary force on a discrete ion near dielectricinterfaces. Recently, various authors have shown that both of these terms areimportant for diffusion through confined geometries in the context of ion channels.
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