The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equilibrium and entropy. The problems associated with this are discussed and it is suggested that they can be resolved, to produce a version of statistical mechanics incorporating both approaches, by redefining equilibrium not as a binary property (being/not being in equilibrium) but as a continuous property (degrees of equilibrium) measured by the Boltzmann entropy and by introducing the idea of thermodynamic-like behaviour for the Boltzmann entropy. The Kac ring model is used as an example to test the proposals
Thermodynamics describes a large class of phenomena we observe in macroscopic systems. The aim of st...
Thermodynamics describes a large class of phenomena we observe in macroscopic systems. The aim of st...
The received wisdom in statistical mechanics is that isolated systems, when left to themselves, appr...
The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equil...
The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equil...
The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equil...
In a recent article, Werndl and Frigg discuss the relationship between the Boltzmannian and Gibbsian...
In a recent article, Werndl and Frigg discuss the relationship between the Boltzmannian and Gibbsian...
In a recent article, Werndl and Frigg discuss the relationship between the Boltzmannian and Gibbsian...
Systems prepared in a non-equilibrium state approach, and eventually reach, equilibrium. Why do they...
Systems prepared in a non-equilibrium state approach, and eventually reach, equilibrium. Why do they...
The Gibbs entropy of a macroscopic classical system is a function of a probability distribution over...
Why do systems prepared in a non-equilibrium state approach, and eventually reach, equilibrium? An i...
Boltzmann’s original scheme leading to the statistical interpretation of non-equilibrium entropy may...
The received wisdom in statistical mechanics is that isolated systems, when left to themselves, appr...
Thermodynamics describes a large class of phenomena we observe in macroscopic systems. The aim of st...
Thermodynamics describes a large class of phenomena we observe in macroscopic systems. The aim of st...
The received wisdom in statistical mechanics is that isolated systems, when left to themselves, appr...
The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equil...
The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equil...
The Boltzmann and Gibbs approaches to statistical mechanics have very different definitions of equil...
In a recent article, Werndl and Frigg discuss the relationship between the Boltzmannian and Gibbsian...
In a recent article, Werndl and Frigg discuss the relationship between the Boltzmannian and Gibbsian...
In a recent article, Werndl and Frigg discuss the relationship between the Boltzmannian and Gibbsian...
Systems prepared in a non-equilibrium state approach, and eventually reach, equilibrium. Why do they...
Systems prepared in a non-equilibrium state approach, and eventually reach, equilibrium. Why do they...
The Gibbs entropy of a macroscopic classical system is a function of a probability distribution over...
Why do systems prepared in a non-equilibrium state approach, and eventually reach, equilibrium? An i...
Boltzmann’s original scheme leading to the statistical interpretation of non-equilibrium entropy may...
The received wisdom in statistical mechanics is that isolated systems, when left to themselves, appr...
Thermodynamics describes a large class of phenomena we observe in macroscopic systems. The aim of st...
Thermodynamics describes a large class of phenomena we observe in macroscopic systems. The aim of st...
The received wisdom in statistical mechanics is that isolated systems, when left to themselves, appr...