I can't figure out how to show that the Clausius entropy(adsbygoogle = window.adsbygoogle || []).push({});

[tex] \Delta S= \int_{T_1}^{T_2} \frac{dQ}{T}[/tex]

is equivalent to the Boltzmann entropy

[tex] S=kln \Omega [/tex]

at thermal equilibrium.

Does anyone know how to do this?

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# Equivalence of Boltzmann and Clausius entropy

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