Abstract

In this work an extremal principle driving the far from equilibrium evolution of a system of structureless particles is derived by using the stochastic quantum hydrodynamic analogy. For a classical phase (i.e., the quantum correlations decay on a distance smaller than the mean inter-molecular distance) the far from equilibrium kinetic equation can be cast in the form of a Fokker-Plank equation whose phase space velocity vector maximizes the dissipation of the energy-type function, named here, stochastic free energy.Near equilibrium the maximum stochastic free energy dissipation (SFED) is shown to be compatible with the Prigogine’s principle of minimum entropy production. Moreover, in quasi-isothermal far from equilibrium states, the theory shows that, in the case of elastic molecular collisions and in absence of chemical reactions, the maximum SFED reduces to the maximum free energy dissipation.When chemical reactions or relevant thermal gradients are present, the theory highlights that the Sawada enunciation of maximum free energy dissipation can be violated.The proposed model depicts the Prigogine’s principle of minimum entropy production near-equilibrium and the far from equilibrium Sawada’s principle of maximum energy dissipation as two complementary principia of a unique theory where the latter one is a particular case of the more general one of maximum stochastic free energy dissipation.Following the tendency to reach the highest rate of SFED, a system relaxing to equilibrium goes through states with higher order so that the matter self-organization becomes possible.

Highlights

  • The research in the field of order generation and matter self-assembling dates back to the thirties [1,2,3,4,5,6,7,8]

  • Šilhavý [4] offers the opinion that the extremal principle of [near-equilibrium] thermodynamics does not have any counterpart for far from-equilibrium steady states despite many claims in the literature

  • By using the stochastic quantum hydrodynamic analogy (SQHA) [12,13,14,15] as the microscopic model, the classical non-equilibrium kinetics has been derived for the macro-scale limit

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Summary

INTRODUCTION

The research in the field of order generation and matter self-assembling dates back to the thirties [1,2,3,4,5,6,7,8]. By using the stochastic quantum hydrodynamic analogy (SQHA) [12,13,14,15] as the microscopic model, the classical non-equilibrium kinetics has been derived for the macro-scale limit. The SQHA, where the structureless molecules are described by a pseudo-Gaussian wave function, allows deriving the farfrom-equilibrium phase-space evolutionary criterion for classical gas and fluid phases in term of maximum dissipation of an energy-based function. We use (30) since it holds even far from equilibrium and is more general than the Boltzmann kinetic equation (able to give the explicit form of the linear coefficients between flows and fluxes but just near local equilibrium). In order to elucidate the significance of the criterion given by (51), we analyze the spatial kinetics far and near equilibrium

Spatial kinetic equations
DISCUSSION AND CONCLUSIONS
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