H-theorem

In thermodynamics, the H-theorem describes the increase of entropy of an ideal gas in an irreversible process, solving the Boltzmann equation. The quantity H is defined as the integral over velocity space :
H \equiv \int { P ({ln P}) d^3 v} = \left\langle { ln P } \right\rangle
where P(r) is the probability. Using the Boltmann equation one can proved that H can only decrease. Therefore, the generalized entropy is defined as
S \equiv - { H \over k}
where S always increases. This theorem is based on Boltzmann's assumption of "molecular chaos" which breaks time reversal symmetry and therefore "begs the question". The final resolution of the time reversibility paradox - Loschmidt's paradox - is found in the Fluctuation Theorem.

 

<< PreviousWord BrowserNext >>
national archives
daniel franois malan
collapse
falkirk wheel
server side includes
martin ebbertz
johannes gerhardus strijdom
1820 in science
stardust memories
king's bench
karl korsch
new zealand music awards
battlement
free market environmentalism
kingbird
hms ibis (u99)
nexus magazine
general services administration
henry h. rogers
rudolph a. marcus
white tea
eddie irvine
night stalkers
accelerator physics
san francisco renaissance
carlton, leicestershire
john brinkley
bosworth
odaiba
bardu ali
deioces
metrical dindshenchas
east of scotland football league
linezolid
navy vieques protests
grammy award for best disco recording
ski mountaineering
hedwig elisabeth amelia de baviere pfalz neuburg
shivaji university
methicillin
muhurta
compressive stress
thomas johnson
thomas johnson (kansas)