Second Law in Classical Non-Extensive Systems

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dc.creatorGross, D. H. E.
dc.date2002-09-19
dc.date.accessioned2026-07-07T02:47:20Z
dc.date.available2026-07-07T02:47:20Z
dc.descriptionEquilibrium statistics of Hamiltonian systems is correctly described by the microcanonical ensemble, whereas canonical ones fail in the most interesting, mostly inhomogeneous, situations like phase separations or away from the thermodynamic ``limit'' (e.g. self-gravitating systems and small quantum systems). A new derivation of the Second Law is presented that respects these fundamental complications. Our ``geometric foundation of Thermo-Statistics'' opens the fundamental (axiomatic) application of Thermo-Statistics to non-diluted systems or to ``non-simple'' systems which are not similar to (homogeneous) fluids. Supprisingly, but also understandably, a so far open problem c.f. Uffink: cond-mat/0005327, page 50 and page 72.
dc.descriptionLatex, 6 pages, 1 figure, presented at the First International Conference on Quantum Limits to the Second Law, San Diego 2002
dc.identifierhttps://arxiv.org/abs/cond-mat/0209467
dc.identifierhttp://arxiv.org/abs/cond-mat/0209467
dc.identifierAIP Conf.Proc. 643 (2003) 131-136
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/19974
dc.subjectStatistical Mechanics
dc.subjectNuclear Theory
dc.subjectClassical Physics
dc.titleSecond Law in Classical Non-Extensive Systems
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