Why are only five out of eight possible thermodynamic potentials important?

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The discussion centers on the significance of five out of eight thermodynamic potentials: entropy, Helmholtz free energy, enthalpy, Gibbs free energy, and grand potential. The less common potentials are less relevant because they pertain to systems with constant entropy or chemical potential, which are not typically encountered in standard thermodynamic contexts. Despite their rarity, these potentials are still defined and applicable to more exotic systems. Additionally, one potential is noted to be identically zero, further diminishing its relevance. For a deeper understanding, the reference to Graben and Ray's work is suggested.
ati
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Starting from the equation

dE=tdS-PdV+\mu dN

It is straightforward to derive all 8 possible thermodynamic potentials. My question is the following: Why are the only important potentials

Entropy
Helmholtz free energy
Enthalpy
Gibbs free energy
Grand potential ?

Why aren't the other three as relevant as these?

Thanks for your help
-Ati
 
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Hi ati, welcome to PF. Systems with constant entropy or constant chemical potential are somewhat less familiar to us than systems with constant temperature or constant particle number. Potentials are still defined and used for the more exotic systems even though they aren't mentioned in most thermodynamics texts. Also, note that one of the potentials (E-TS+PV-\muN) is identically zero!

You may be interested in reading Graben and Ray's "Eight physical systems of thermodynamics, statistical mechanics, and computer simulations" Molecular Physics 80(5) (1993).
 
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