Titlebook: Extended Irreversible Thermodynamics; David Jou,José Casas-Vázquez,Georgy Lebon Book 19962nd edition Springer-Verlag Berlin Heidelberg 199

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Hyperbolic Heat Conductionst literature. One of them, of a theoretical nature, refers to the so-called “paradox” of propagation of thermal signals with infinite speed. The second one, more closely related to experimental observations, deals with second sound, ballistic phonon propagation and phonon hydrodynamics in solids at low temperatures.

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Relativistic Formulation and Cosmological Applicationsity and the viscosity of a gas of neutrinos play a role in phenomena like stellar collapse. In cosmology, bulk viscosity provides a source of dissipation which may have relevant effects on the dynamics of the Universe. These have fostered the research on relativistic non-equilibrium thermodynamic theories.

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Book 19962nd editiont be updated in order to incorporate memory, non-local, and non-linear effects. These effects have been studied by starting from microscopic models which are specific to particular systems and whose solution requires mathematical approximations and boundary conditions. The aim of extended irreversib

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Fluctuation Theorye shall present many illustrations of how these equations are useful in interpreting experimental data or dealing with situations which are beyond the scope of the classical theory. In this chapter, our interest is focused on the generalized Gibbs equation, which is the central thermodynamic result

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Non-equilibrium Statistical Mechanicster deals with more general methods of non-equilibrium statistical mechanics. First, we start from the Liouville equation and introduce the projection operator technique to relate the memory function to the time correlation function of the fluctuations of the fluxes, a key result in modem non-equili

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Rheological Materialsscosity, which may depend on the temperature and the pressure, but not on the velocity gradient. However, it has been observed that there exists a wide class of materials, such as polymers, soap solutions, some honeys, asphalts, and physiological fluids, that fail to obey the linear Newton law (7.1)