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| | Citebase - Second Law of Thermodynamics and Macroscopic Observables within Boltzmann's principle, an attempt (Site not responding. Last check: 2007-10-05) |
 | | Boltzmann's principleS=k*ln W is generalized to non-equilibrium Hamiltonian systems with possibly fractal distributions in phase space by the box-counting volume. |
 | | A geometric foundation thermo-statistics is presented with the only axiomatic assumption of Boltzmann's principle S(E,N,V)=k\ln W. This relates the entropy to the geometric area e^{S(E,N,V)/k} of the manifold of constant energy in the finite-N-body phase space. |
 | | Boltzmann's principle S(E,N,V)=k\ln W relates the entropy to the geometric area e^{S(E,N,V)} of the manifold of constant energy in the N-body phase space. |
| citebase.eprints.org /cgi-bin/citations?id=oai%3AarXiv%2Eorg%3Acond%2Dmat%2F0011130 (896 words) |
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