1959
DOI: 10.1007/978-3-642-45912-2_4
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Thermodynamik der irreversiblen Prozesse

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Cited by 132 publications
(123 citation statements)
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“…More precisely, it is shown that knowledge of c p (ω) and α p (ω) at all frequencies allows one to calculate κ T (ω) except for an overall additive constant giving the high-frequency limit. This is equivalent to the above-mentioned result derived long ago [1,3,36], but now in a setting that is explicitly consistent with statistical mechanics.…”
Section: The General Stochastic Case: Two Independent Thermoviscoelassupporting
confidence: 82%
“…More precisely, it is shown that knowledge of c p (ω) and α p (ω) at all frequencies allows one to calculate κ T (ω) except for an overall additive constant giving the high-frequency limit. This is equivalent to the above-mentioned result derived long ago [1,3,36], but now in a setting that is explicitly consistent with statistical mechanics.…”
Section: The General Stochastic Case: Two Independent Thermoviscoelassupporting
confidence: 82%
“…These magnitudes determine (for a given metric gab) the family of curves in the infinitesimal first order neighbourhood of a point uniquely up to homogeneous Lorentz transformations, as follows from the relation (21) which is equivalent to (10). In addition to (9 we wish to explicitly introduce for later application the scalars ~ (i~ai~a) 1/2, ~0 --(Wacoa) 1/2 = (SrlWabW ab~l/~) , a = '2 ~o~(1-" .,,~b~l/2j .…”
Section: =3( 0 -mentioning
confidence: 99%
“…[13]), we side with Meixner's point of view [53,205] in that, differently to equilibrium, does not exists a unique and precisely defined concept of thermodynamic entropy out of equilibrium. The one of subsection IV.A, is the one peculiar to IST, and depending on the nonequilibrium thermodynamic state defined by Zubarev-Peletminskii selection law altogether with the use of Bogoliubov's principle of correlation weakening.…”
Section: Discussionmentioning
confidence: 99%