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

FELON

Springer Tracts in Natural Philosophyhttp://image.papertrans.cn/e/image/319826.jpg

災難

https://doi.org/10.1007/978-1-4684-0447-0Boltzmann equation; kinetic theory; thermodynamics

騷動

https://doi.org/10.1007/978-3-658-20862-2to identical results. This was first shown by Dreyer [95]. To be sure, the methods are different in the two fields and, in particular, the role of entropy is different: In extended thermodynamics the entropy inequality is exploited, while in the molecular theory we maximize the kinetic expression for the entropy.

excursion

地牢

palliate

0081-3877 tions of irreversible thermodynamics - those of Navier-Stokes and Fourier - are parabolic. This incompatibility between the expectation of physicists and the classical laws of thermodynamics has prompted the formulation of extended thermodynamics. After describing the motifs and early evolution of t

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Bernard Dacorogna,Paolo Marcellinid—that these laws became incorporated into thermodynamics of irreversible processes. That theory, while not entirely systematic, is simple and has great suggestive value. We start out with a brief description of how thermodynamics of irreversible processes arrives at the laws of Fourier and Navier-Stokes.

Ligneous

Theoretische Grundlagen der Arbeit, Müller [5] formulated the theory relativistically, but this work was not properly published until Israel [33] presented a very similar theory. These theories had all the shortcomings of extended TIP that were discussed in Chapter 1.

Obstacle

Werner Glasmacher,Dietmar Sommers 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 bifluid theory of Tisza and Landau is a special case of the thermodynamic theory of binary mixtures in general.

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