Maxwell Relation, Gibbs Free Energy, Thermal Expansion Coefficient

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SUMMARY

The discussion focuses 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. The relevant equations include the Gibbs free energy equation (G = U - TS + PV) and the definition of the thermal expansion coefficient (β = (1/V)(∂V/∂T) |_{N,P}). The participants conclude that the proof can be completed without relying on the ideal gas law, emphasizing the importance of the third law of thermodynamics in this context.

PREREQUISITES
  • Understanding of Gibbs free energy and its equations
  • Familiarity with Maxwell relations in thermodynamics
  • Knowledge of the third law of thermodynamics
  • Concept of thermal expansion coefficient (β)
NEXT STEPS
  • Study the derivation of Maxwell relations from thermodynamic potentials
  • Explore the implications of the third law of thermodynamics on physical systems
  • Investigate the behavior of thermal expansion coefficients in various states of matter
  • Review the relationship between Gibbs free energy and phase transitions
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Students and professionals in thermodynamics, physicists, and anyone studying the properties of materials at low temperatures.

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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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