Maxwell Relation, Gibbs Free Energy, Thermal Expansion Coefficient

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The discussion centers on proving that the thermal expansion coefficient β equals zero at absolute zero temperature (T = 0) using a Maxwell relation derived from Gibbs free energy and the third law of thermodynamics. The original poster encountered difficulties in their calculations, suggesting that their results indicated an ideal gas is incompatible with the third law. However, it is advised that the proof can be completed without relying on the ideal gas law. The conversation emphasizes the importance of correctly applying thermodynamic principles to reach the conclusion about β at T = 0. Understanding these relationships is crucial for grasping fundamental thermodynamic concepts.
Tian En

Homework Statement


By means of a Maxwell relation derived from the Gibbs free energy and making use of the third law of thermodynamics, prove that the thermal expansion coefficient β must be zero at T = 0. I tried but I got something funny.

Homework Equations


$$G=U-TS+PV$$
$$dG=\mu dN-SdT+VdP$$
$$S=Nk_B[\ln(\frac{V}{N}(\frac{4\pi mU}{3Nh^2})^{3/2})+\frac{5}{2}]$$
$$PV=Nk_B T$$
$$\beta = \frac{1}{V}\frac{\partial V}{\partial T} \Bigg| _{N,P}$$

The Attempt at a Solution


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I believe you have essentially shown that an ideal gas is not compatible with the third law.

I think you should be able to finish the proof using your result
upload_2017-10-26_11-51-36.png
without assuming the ideal gas law.
 

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Last edited:

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