Derivation of Maxwell's relations

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SUMMARY

The discussion centers on the derivation of Maxwell's relations in thermodynamics, specifically the relation \(\left( \frac{\partial S}{\partial V} \right)_T = \left( \frac{\partial P}{\partial T} \right)_V\). The user attempts to derive this relation using the internal energy differential \(dU = TdS - PdV\) but encounters difficulties. It is concluded that the derivation cannot be achieved through internal energy and that alternative approaches using enthalpy, Gibbs free energy, or Helmholtz free energy should be considered, with a specific emphasis on Helmholtz free energy.

PREREQUISITES
  • Understanding of thermodynamic concepts such as entropy (S), pressure (P), and temperature (T).
  • Familiarity with the internal energy differential \(dU = TdS - PdV\).
  • Knowledge of Maxwell's relations and their significance in thermodynamics.
  • Basic grasp of thermodynamic potentials including enthalpy, Gibbs free energy, and Helmholtz free energy.
NEXT STEPS
  • Study the derivation of Maxwell's relations using Helmholtz free energy.
  • Explore the implications of Gibbs free energy in thermodynamic systems.
  • Learn about the perfect differential and its role in thermodynamics.
  • Review the relationship between state functions and their derivatives in thermodynamic contexts.
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Students and professionals in physics and engineering, particularly those specializing in thermodynamics, who seek to deepen their understanding of Maxwell's relations and their derivations.

komodekork
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In thermodynamics one of the maxwell relations is:
<br /> \left( \frac{\partial S}{\partial V} \right)_T = \left( \frac{\partial P}{\partial T} \right)_V<br />

When I try to derive it from dU = TdS - PdV i get:
<br /> T = \left( \frac{\partial U}{\partial S} \right)_V<br />
<br /> P = -\left( \frac{\partial U}{\partial V} \right)_S<br />
<br /> \left( \frac{\partial T}{\partial V} \right)_S = \frac{\partial}{\partial V}\left( \frac{\partial U}{\partial S} \right)_V = \frac{\partial}{\partial S}\left( \frac{\partial U}{\partial V}\right)_S = -\left( \frac{\partial P}{\partial S} \right)_V<br />
I then multiply with \frac{\partial S}{\partial T},
<br /> \frac{\partial S}{\partial T} \left( \frac{\partial T}{\partial V} \right)_S = \frac{\partial S}{\partial T} \left( -\frac{\partial P}{\partial S} \right)_V<br />
<br /> \left( \frac{\partial S}{\partial V} \right)_S = -\left( \frac{\partial P}{\partial T} \right)_V<br />
So, what am I doing wrong?
 
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I don't think you can derive that Maxwell relation from the internal energy differential. Try enthalpy, Gibbs free energy, or Helmholtz free energy instead.
 
komodekork said:
In thermodynamics one of the maxwell relations is:
<br /> \left( \frac{\partial S}{\partial V} \right)_T = \left( \frac{\partial P}{\partial T} \right)_V<br />

So, what am I doing wrong?

Muphrid said:
I don't think you can derive that Maxwell relation from the internal energy differential. Try enthalpy, Gibbs free energy, or Helmholtz free energy instead.
Helmholtz free energy specifically. The form he is trying to derive implies T & V are the parameters of the system.
 

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