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20 April 2024
 
  » arxiv » 2010.10971

 Article overview


Emergence of a nonconstant entropy for a fast-slow Hamiltonian system in its second-order asymptotic expansion
Matthias Klar ; Karsten Matthies ; Johannes Zimmer ;
Date 21 Oct 2020
AbstractA system of ordinary differential equations describing the interaction of a fast and a slow particle is studied, where the interaction potential $U_epsilon$ depends on a small parameter $epsilon$. The parameter $epsilon$ can be interpreted as the mass ratio of the two particles. For positive $epsilon$, the equations of motion are Hamiltonian. It is known (Bornemann, Springer Lecture Notes in Mathematics 1687) that the homogenised limit $epsilon o0$ results again in a Hamiltonian system with homogenised potential $U_{hom}$. In this article, we are interested in the situation where $epsilon$ is small but positive. In the first part of this work, we rigorously derive the second-order correction to the homogenised degrees of freedom, notably for the slow particle $y_epsilon = y_0 +epsilon^2 (ar{y}_2 +[y_2]^epsilon)$. In the second part, we give the resulting asymptotic expansion of the energy associated with the fast particle $E_epsilon^perp = E_0^perp + epsilon [E_1^perp]^epsilon+ epsilon^2 (ar{E}_2^perp+[E_2^perp]^epsilon)$, a thermodynamic interpretation. In particular, we note that to leading-order $epsilon o0$, the dynamics of the fast particle can be identified as an emph{adiabatic} process with emph{constant entropy}, $dS_0 =0$. This limit $epsilon o0$ is characterised by an energy relation that describes equilibrium thermodynamic processes, $d E_0^perp = F_0 d y_0 + T_0 dS_0 = F_0 d y_0$, where $T_0$ an $F_0$ are the leading-order temperature and external force terms respectively. In contrast, we find that to second-order $epsilon^2$, a emph{non-constant entropy} emerges, $d ar{S}_2 eq 0$, effectively describing a non-adiabatic process. Remarkably, this process satisfies on average (in the weak$^ast$ limit) a similar thermodynamic energy relation, i.e., $d ar{E}^perp_2 = F_0 d ar{y}_2 + T_0 d ar{ar{S}}_2$.
Source arXiv, 2010.10971
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