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010   $a3-319-41153-5
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035   $a(DE-He213)978-3-319-41153-8
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035   $a(PPN)194517209
035   $a(EXLCZ)993710000000751198
100   $a20160713d2016      u|         0
101 0 $aeng
135   $aurnn|008mamaa
181   $ctxt$2rdacontent
182   $cc$2rdamedia
183   $acr$2rdacarrier
200 10$aKinetic Theory of Nonequilibrium Ensembles, Irreversible Thermodynamics, and Generalized Hydrodynamics $eVolume 2. Relativistic Theories /$fby Byung Chan Eu
205   $a1st ed. 2016.
210  1$aCham :$cSpringer International Publishing :$cImprint: Springer,$d2016.
215   $a1 online resource (IX, 201 p. 1 illus. in color.) 
311   $a3-319-41152-7 
320   $aIncludes bibliographical references at the end of each chapters and index.
327   $aRelativistic Kinetic Theory for Matter -- Relativistic Kinetic Theory of Matter and Radiation -- Radiative Transport Coefficients and Their Mutual Relations.
330   $aThis book presents the fundamentals of irreversible thermodynamics for nonlinear transport processes in gases and liquids, as well as for generalized hydrodynamics extending the classical hydrodynamics of Navier, Stokes, Fourier, and Fick. Together with its companion volume on nonrelativistic contexts, it provides a comprehensive picture of the relativistic covariant kinetic theory of gases and relativistic hydrodynamics of gases.Relativistic theories of macroscopic irreversible processes must strictly conform to the thermodynamic laws at every step and in all approximations that enter their derivation from the mechanical principles. Upholding this as the inviolable tenet, the author develops theories of irreversible transport processes in fluids (gases or liquids). They apply regardless of whether the processes are near to or far removed from equilibrium, or whether they are linear or nonlinear with respect to macroscopic fluxes or thermodynamic forces. The irreversible covariant Boltzmann as well as the covariant form of the Boltzmann-Nordheim-Uehling-Uhlenbeck equation is used for deriving theories of irreversible transport equations and generalized hydrodynamic equations for either classical gases or quantum gases. They all conform rigorously to the tenet. All macroscopic observables described by the so-formulated theories therefore are likewise expected to strictly obey the tenet.
606   $aThermodynamics
606   $aStatistical physics
606   $aDynamics
606   $aPhysics
606   $aThermodynamics$3https://scigraph.springernature.com/ontologies/product-market-codes/P21050
606   $aComplex Systems$3https://scigraph.springernature.com/ontologies/product-market-codes/P33000
606   $aMathematical Methods in Physics$3https://scigraph.springernature.com/ontologies/product-market-codes/P19013
606   $aStatistical Physics and Dynamical Systems$3https://scigraph.springernature.com/ontologies/product-market-codes/P19090
615  0$aThermodynamics.
615  0$aStatistical physics.
615  0$aDynamics.
615  0$aPhysics.
615 14$aThermodynamics.
615 24$aComplex Systems.
615 24$aMathematical Methods in Physics.
615 24$aStatistical Physics and Dynamical Systems.
676   $a536.7
700   $aEu$b Byung Chan$4aut$4http://id.loc.gov/vocabulary/relators/aut$0786809
906   $aBOOK
912   $a9910254622403321
996   $aKinetic Theory of Nonequilibrium Ensembles, Irreversible Thermodynamics, and Generalized Hydrodynamics$91807461
997   $aUNINA