Theorems of Liouville and Poincare & their relation to entropy

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Liouville's theorem applies to systems where the phase space volume is conserved, but it does not guarantee that Poincaré's recurrence theorem will hold in all cases. Poincaré's recurrence theorem requires that the system's energy and space remain constant, indicating that it is applicable primarily to microcanonical ensembles. In canonical ensembles, where energy is not conserved, Poincaré's theorem does not hold. Therefore, the relationship between Liouville's theorem and Poincaré's theorem is conditional on the conservation of energy. Understanding these distinctions is crucial for analyzing the behavior of dynamical systems over time.
Heirot
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If we have a system for which the Liouville's tm holds, can we automaticly say the Poincare's recurrence tm also holds? Presumably this is true in microcanonical ansable, but how about canonical, where the energy isn't constant?
 
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Heirot said:
If we have a system for which the Liouville's tm holds, can we automaticly say the Poincare's recurrence tm also holds? Presumably this is true in microcanonical ansable, but how about canonical, where the energy isn't constant?
Poincaré's recurrence theorem holds for any statistical system in which system's energy and the system's space do not change. It says, essentially, that such a system will return to a microstate that is to within an arbitrarily close approximation of its original microstate, if it is given enough time. So if energy is not conserved in the system, Poincaré's recurrence theorem does not hold.

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