Maxwell Relations (not equations)

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SUMMARY

The discussion centers on the derivation and understanding of Maxwell Relations in Thermodynamics, specifically using the equation of state TdS = dU + PdV. The four Maxwell Relations arise from selecting pairs of the thermodynamic variables: Temperature (T), Entropy (S), Pressure (P), and Volume (V). Despite having six possible pairs, only four Maxwell Relations exist due to the nature of thermodynamic conjugate pairs, which must be used together in the differential equations. The conversation also touches on the dimensional analysis of these equations and the implications of considering Massieu functions.

PREREQUISITES
  • Understanding of thermodynamic concepts, specifically Maxwell Relations
  • Familiarity with differential calculus and partial derivatives
  • Knowledge of thermodynamic differentials such as dU, dA, dH, and dG
  • Basic grasp of energy dimensions in thermodynamics
NEXT STEPS
  • Study the derivation of Maxwell Relations in detail using TdS = dU + PdV
  • Explore the implications of thermodynamic conjugate pairs in various equations
  • Learn about Massieu functions and their relationship to Maxwell Relations
  • Investigate the applications of Helmholtz and Gibbs free energy in thermodynamics
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Students and professionals in thermodynamics, physicists, and engineers who seek to deepen their understanding of thermodynamic relationships and their applications in energy systems.

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I just recently learned the Maxwell Relations in Thermodynamics. We aren't really doing anything with them, just went through the derivations.
In deriving them, we started with the equation of state:

TdS=dU+PdV

where T is temperature, S entropy, U internal energy, P pressure, V volume. We would than pick two of the four variables S,P,V,T, and with some math derive one of the maxwell relations. This was done using differentials, ie, if
df(x,y)=Adx+Bdy, than A=df/dx (partial derivative) and B=df/dy (p.d.), also, as long as the function isn't pathological, dA/dy=dB/dx (p.d.).

Here's my question, each of the four maxwell relations is found by chosing 2 of the four variables, and there are four maxwell relations. But there are 6 possible ways to chose 2 of the 4 variables, so how come there aren't 6 Maxwell Relations? Is there simply no way to manipulate the resulting equations to make it work for the other 2 pairs of variables, or is there some other reason for this? Thank you.
 
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You have to start with some differential relationship. Usually used are the thermodynamic differentials:
dU = T dS - P dV
dA = -S dT - P dV
dH = T dS + V dP
dG = -S dT - P dV

For the variables T, S, P, V, there are 6 possible choices for pairs: TS, TP, TV, SP, SV, PV. Notice the two that you can't get are TS and PV. It's because these pairs are thermodynamic conjugate pairs, and always appear together in these differentials.

If you consider the dimensional analysis of the above equations, the LHS is always an energy, and the right hand side is always products involving temperature and entropy, which is energy, and producst of pressure and volume, which is energy. In order to get T and S in different spots, ie. T dV + S dP, you have to have products on the RHS which are not energy, and don't make sense to be added together.
 
H is enthalpy.Okay.A must be Helmholtz potential.U've considered closed system (no change of # of particles)...
To conclude,the # of Maxwell relations is very large and it's even greater,if you consider the Massieu functions \Phi and \Psi.

Daniel.
 

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