Thermodynamic Framework for Compact q-Gaussian Distributions
arXiv:1708.00114 · doi:10.1016/j.physa.2017.09.013
Abstract
Recent works have associated systems of particles, characterized by short-range repulsive interactions and evolving under overdamped motion, to a nonlinear Fokker-Planck equation within the class of nonextensive statistical mechanics, with a nonlinear diffusion contribution whose exponent is given by . The particular case applies to interacting vortices in type-II superconductors, whereas covers systems of particles characterized by short-range power-law interactions, where correlations among particles are taken into account. In the former case, several studies presented a consistent thermodynamic framework based on the definition of an effective temperature (presenting experimental values much higher than typical room temperatures , so that thermal noise could be neglected), conjugated to a generalized entropy (with ). Herein, the whole thermodynamic scheme is revisited and extended to systems of particles interacting repulsively, through short-ranged potentials, described by an entropy , with , covering the (vortices in type-II superconductors) and (short-range power-law interactions) physical examples. The main results achieved are: (a) The definition of an effective temperature conjugated to the entropy ; (b) The construction of a Carnot cycle, whose efficiency is shown to be , where and are the effective temperatures associated with two isothermal transformations, with ; (c) Thermodynamic potentials, Maxwell relations, and response functions. The present thermodynamic framework, for a system of interacting particles under the above-mentioned conditions, and associated to an entropy , with , certainly enlarges the possibility of experimental verifications.
18 pages, 1 figure
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- Non-linear Fokker-Planck equations from conformal metrics and scalar curvature