Abstract

An ensemble of classical subsystems interacting with surrounding particles has been considered. In general case, a phase volume of the subsystems ensemble was shown to be a function of time. The evolutional equations of the ensemble are obtained as well as the simplest solution of these equations representing the quasi-local distribution with the temperature pattern being assigned. Unlike the Gibbs's distribution, the energy of interaction with surrounding particles appears in the distribution function, which make possible both evolution in the equilibrium case and fluctuations in the non-equilibrium one. The expression for local entropy is obtained. The derivation of hydrodynamic equations from Boltzmann equation has been analyzed. The hydrodynamic equations obtained from Boltzmann equation were shown to be equations for ideal liquid. Reasons for stochastic description in deterministic Hamilton's systems, conditions of applicability of Poincare's recurrence theorem as well as the problem of irreversibility have been considered.

Highlights

  •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

  • RQH FDQ ZULWHQ H[SUHVVLRQ WKH SUHVHQFH RI WKH WKLUG DQG IRXUWK WHUPV LV YHU\ HVVHQWLDO ZKLFK FRQWDLQ SDUWLDO GHULYDWLYHV.

  • ZLWK UHVSHFW WR T DQG S L H ZLWK UHVSHFW WR FRRUGLQDWHV DQG PRPHQWD RI VXUURXQGLQJ SDUWLFOHV :KHQ.

Read more

Summary

RI WKH SKDVH SRLQW DW PRPHQWV W DQG W

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

RQH FDQ ZULWH
GW GW
WLPH VKRXOG EH ZULWWHQ LQ WKH IRUP
6XEVWLWXWLQJ LQWR ZH REWDLQ
LV HTXDO WR
RI WKH IRUP
GHSHQG RQ WKH WLPH W DQG UHSUHVHQW LW LQ WKH IRUP
7KH ODVW HTXDWLRQ LV REWDLQHG LQ WHUPV RI
1RZ ZH
WKH ULJKW KDQG VLGH RI WKH WUDQVIHU HTXDWLRQ ZKLFK WDNHV WKH
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call