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Titlebook: Extended Thermodynamics; Ingo Müller,Tommaso Ruggeri Book 19931st edition Springer-Verlag New York, Inc. 1993 Boltzmann equation.kinetic t

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Bernard Dacorogna,Paolo Marcellinisses in fluids. This was before there was any non-equilibrium thermodynamics. It was much later—essentially when Eckart’s papers [1], [2], [3] appeared—that these laws became incorporated into thermodynamics of irreversible processes. That theory, while not entirely systematic, is simple and has gre
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Charakterisierung von Unternehmensanleihen,eat them thermodynamically. The first successful attempt in that direction was Boltzmann’s derivation of what we now call the Stefan-Boltzmann law. That law relates the energy density of cavity radiation in equilibrium with the wall to the temperature of the wall.
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Werner Glasmacher,Dietmar Sommer this wave and confirmed that its temperature variations are uncoupled from the pressure variations: therefore the second sound is often referred to as a temperature wave. This phenomenon is now well understood. We described it in Chapter 3 following the work of Dreyer [81], who showed that the bifl
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https://doi.org/10.1007/978-3-476-05727-3tage of this method is that it works in equilibrium; in fact, it makes use of the density fluctuations in equilibrium. By Onsager’s hypothesis the auto-correlation function of such a fluctuation is related to the solution of the macroscopic field equations.
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https://doi.org/10.1007/978-3-658-26109-2 expression for the phase speeds and attenuations. If the theory contains unknown parameters, a comparison of the empirical data with the theoretical prediction delivers values for these parameters; but, if a theory is specific—as is the case with molecular extended thermodynamics—the experiments pr
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978-1-4684-0449-4Springer-Verlag New York, Inc. 1993
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