According to the definition of entropy, we can write
Using the definition of the heat capacity at constant volume for the first differential and the appropriate Maxwell relation for the second we have:
Expressing CV in terms of ĉV as developed in the above section, differentiating the ideal gas equation of state, and integrating yields:
Using (3) we get:
where all constants have been incorporated into the logarithm as f(N) which is some function of the particle number N having the same dimensions as VTĉV in order that the argument of the logarithm be dimensionless.
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