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Statistical and Classical Entropy

Contrary to what happens for mechanical systems, chemical systems do not reach equilibrium by minimizing their internal energy. The essential difference is that in [Pg.13]

Further manipulations give the Boltzmann equilibrium distribution and the total entropy of an ideal gas  [Pg.14]

The partition function (2 has a translational, rotational and vibrational part, and so does entropy. The first two contributions can be calculated in a straightforward way, but the vibrational contribution to entropy requires a knowledge of the normal vibrational frequencies of the molecule or of the crystal. [Pg.14]

The classical definition of entropy goes through the Clausius inequality  [Pg.14]


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