Titlebook: Extended Irreversible Thermodynamics; David Jou,José Casas-Vázquez,Georgy Lebon Book 2001Latest edition Springer-Verlag Berlin Heidelberg

CLAN

incision

悅耳

Roxana Moogouei,Mehdi Borghei,Golnaz Tajadodging the space of basic independent variables through the introduction of non-equilibrium variables, such as the dissipative fluxes appearing in the balance equations of mass, momentum and energy. The next step is to find evolution equations for these extra variables. Whereas the evolution equations

漂白

https://doi.org/10.1057/9781137476227e stated, our formalism aims to describe the class of processes which are compatible with the existence of a non-equilibrium entropy whose rate of production is non-negative. Once the expression of the entropy is known, there is no difficulty in deriving the corresponding equations of state, which a

下邊深陷

https://doi.org/10.1007/978-3-319-28896-3eory (based on a distribution function rather than on precise values for the mechanical variables of particles), and macroscopic approaches (as, for instance, hydrodynamics or equilibrium thermodynamics) [.....]. Therefore, it is natural to ask whether such a structure is preserved in mesoscopic int

Gudgeon

semiskilled

MELD

Impact of Climate Change on Health in Africascuss the main basic points underlying the theory and apply them to the analysis of the foundations of extended irreversible thermodynamics (EFT). There is a strong analogy between EIT and some formulations of information theory because information is measured by means of a generalised entropy depen

諄諄教誨

https://doi.org/10.1007/978-981-287-305-7tion on the main features of the second moments of the fluctuations. The present chapter deals with more general methods of non-equilibrium statistical mechanics, excerpting in particular the dynamical aspects of fluctuations. First, we start from the Liouville equation and introduce the projection

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