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Re: Second law in the microscopic scale



For dimensional reasons, [xi] has to be something like the
correlation length over the particle (or lattice) spacing. The point I
intended, however, is that (barring phase transitions, which I don't know
how to envision for few-particle systems) is that when N is Avagodro's
number, fluctations are ignorable.


On Sat, 27 Dec 2003, David Bowman wrote:

Regarding Jack U's comment:

Essentially yes. If N is the number of particles in the system,
then the random-fluctuation probability is like 1/sqrt(N) - See
Landau and Lifshitz introduction.
Jack
=20
If we include the effects of correlations between the particles I
believe the relative fluctuations go more like sqrt([xi]^d / N) where
[xi] is the correlation length and d is the spatial dimensionality
of the system (assuming the interactions between the particles are
finite-ranged).

David Bowman


--
"Don't push the river, it flows by itself"
Frederick Perls