Justify the identification of the statistical entropy with the thermodynamic entropy.
The main term on which the definition of statistical entropy is based is probability of number of atoms or the number of equivalent microstates.
Boltzman defined entropy as: S= Kln
,
where K is a proportionality constant and
is the number of equivalent microstates. Replacing k by the number
of moles (i.e N/Na=n; where Na is avogadros number) and rate
constant (R) the equation becomes
S= nRln
If we take change in entropy (
S)
and replace the number of microstates (
)
by change in volume (V2-V1) the equation becomes
S= nRln(V2/V1).
Now the main term that defines THERMODYNAMIC ENTROPY is change in heat in a reversible system.
q(rev) = nRT ln(V2/V1)
Dividing the whole equation by T, we get
q(rev) /T = nR ln(V2/V1)
(i. e) S = nR ln (V2/V1)
Justify the identification of the statistical entropy with the thermodynamic entropy.
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