non-equilibrium statistical operator | Academic Journals and Conferences

Statistical Approach to Describing the Processes of Transport of Lipoproteins and Other Components in Blood Vessels – I

To describe atherosclerotic processes in the intima of blood vessels, a statistical approach to describing non-equilibrium processes of blood component transport in the lumen-endothelium-intima system of blood vessels has been proposed, which involves taking into account the nature of interactions between blood components. Using the method of non-equilibrium statistical operator for the parameters of the abbreviated description, a system of transport equations has been obtained, which, within the framework of the selected model of component interaction, can describe no

Kinetic description of ion transport in the system "ionic solution – porous environment"

A kinetic approach based on a modified chain of BBGKI equations for nonequilibrium particle distribution functions was used to describe the ion transfer processes in the ionic solution – porous medium system. A generalized kinetic equation of the revised Enskog–Vlasov–Landau theory for the nonequilibrium ion distribution function in the model of charged solid spheres is obtained, taking into account attractive short-range interactions for the ionic solution – porous medium system.

To the kinetic theory of dense gases and liquids. Calculation of quasi-equilibrium particle distribution functions by the method of collective variables

Based on a chain of BBGKI equations with a modified boundary condition that takes into account multiparticle correlations, kinetic equations in the approximate "pairs" collisions and in the polarization approximation, taking into account the interaction through the third particle, obtained. The specifics of the model representation of the pair potential of particle interaction through short-range and long-range parts were taken into account. In the case of the short-range potential in the form of the potential of solid spheres, the contribution of Enskog's revised theory to the complete i