Derivation of Maxwell's relations

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Discussion Overview

The discussion revolves around the derivation of one of Maxwell's relations in thermodynamics, specifically the relationship between entropy, volume, pressure, and temperature. Participants explore different approaches to derive this relation and the appropriate thermodynamic potentials to use.

Discussion Character

  • Technical explanation, Debate/contested

Main Points Raised

  • One participant presents a derivation attempt using the internal energy differential and arrives at a form of the Maxwell relation.
  • Another participant suggests that the derivation should not be based on the internal energy differential and recommends using enthalpy, Gibbs free energy, or Helmholtz free energy instead.
  • A later reply emphasizes that the form of the relation implies temperature and volume are the parameters of the system, supporting the use of Helmholtz free energy.
  • Concerns are raised about the correctness of multiplying by the partial derivative of entropy with respect to temperature in the derivation process.

Areas of Agreement / Disagreement

Participants express disagreement regarding the appropriateness of using the internal energy differential for the derivation. Multiple competing views on the correct approach to derive the Maxwell relation remain unresolved.

Contextual Notes

Participants highlight potential limitations in the derivation process, including the choice of thermodynamic potentials and the implications of the parameters involved.

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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