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Kappa Entropy and its Thermodynamic Connection

J. A. S. Lima, M. H. Benetti

TL;DR

The paper addresses reconciling fat-tailed Kappa velocity distributions with thermodynamics by introducing a two-parameter nonadditive entropy $S_{\kappa\ell}$ and its linked distribution $F_{\kappa\ell}(v)$. Using a deformed logarithm $\ln_{\kappa\ell}$ and its inverse $e_{\kappa\ell}$, it derives a deformed Boltzmann counting framework and an equilibrium distribution that reduces to Boltzmann–Maxwell in the limit $\kappa \to \infty$. The key result is that thermodynamic consistency is achieved only for the subclass with $\ell = -\frac{5}{2}$, where the standard relations $dQ_{rev} = T dS$ and $P V = N k_B T$ hold under standard averaging. This work provides a bottom-up bridge between kinetic theory and thermodynamics for power-law systems and identifies the precise parameter regime where conventional thermodynamics applies.

Abstract

Adopting a bottom-up perspective, we propose a novel two-parametric nonadditive entropy, $S_{κ\ell}$, associated with a Kappa-type power-law velocity distribution, $F_{κ\ell}(v)$, recently derived in the literature. By formulating an extended Neo-Boltzmannian microstate counting procedure and employing standard averaging techniques, we demonstrate that the fundamental laws of thermodynamics are preserved within this generalized power-law framework only whether $\ell=-5/2$, regardless of the values assumed by the $κ$-parameter.

Kappa Entropy and its Thermodynamic Connection

TL;DR

The paper addresses reconciling fat-tailed Kappa velocity distributions with thermodynamics by introducing a two-parameter nonadditive entropy and its linked distribution . Using a deformed logarithm and its inverse , it derives a deformed Boltzmann counting framework and an equilibrium distribution that reduces to Boltzmann–Maxwell in the limit . The key result is that thermodynamic consistency is achieved only for the subclass with , where the standard relations and hold under standard averaging. This work provides a bottom-up bridge between kinetic theory and thermodynamics for power-law systems and identifies the precise parameter regime where conventional thermodynamics applies.

Abstract

Adopting a bottom-up perspective, we propose a novel two-parametric nonadditive entropy, , associated with a Kappa-type power-law velocity distribution, , recently derived in the literature. By formulating an extended Neo-Boltzmannian microstate counting procedure and employing standard averaging techniques, we demonstrate that the fundamental laws of thermodynamics are preserved within this generalized power-law framework only whether , regardless of the values assumed by the -parameter.

Paper Structure

This paper contains 5 sections, 22 equations, 2 figures, 1 table.

Figures (2)

  • Figure 1: Ratio between deformed and natural logarithms for different values of the parameter $\kappa$ and some selected values of the $\ell$ parameter ($\ell = 0, -1, \, \text{and} \, -5/2$). Black line in the bottom corresponds to the Boltzmannian limit $\kappa \to \infty$. Note that for different values of the deformation parameter $\kappa$, the resulting curves remain nearly parallel to the standard Boltzmannian case. This means that the deformed logarithm may likewise be approximated by a mildly corrected step-like function, analogous to the behaviour of the natural logarithm of Boltzmann' approach [cf. equations (\ref{['E8']})-(\ref{['E10']})].
  • Figure 2: Ratio between the derivative of the deformed logarithm of the partition function and the quantity $-U/N$ for the fat-tail case ($\kappa >0$), where the distribution has a high-energy tail ($0.1 < \beta \varepsilon_i < 1000$). The vertical dashed lines represent the cuts to avoid divergences in the KVD (\ref{['E2']}), for $\ell = -1 \,(\kappa > 3/2)$ and $\ell = 0 \,(\kappa > 5/2)$.