Thermodynamical potentials: some hand-waving please

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SUMMARY

This discussion centers on the understanding of thermodynamical potentials in the context of statistical physics. Participants emphasize the importance of grasping the physical significance of these potentials, specifically internal energy (U), enthalpy (H), and Gibbs free energy (G). The equations presented, such as dU = μ dN and dU = μ dN + P dV - T ds, illustrate the relationships between energy, particle number, pressure, and entropy. A deeper "feeling" for these concepts is deemed essential for both theoretical comprehension and practical application in thermodynamics.

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  • Understanding of statistical physics principles
  • Familiarity with thermodynamic laws
  • Knowledge of key thermodynamic potentials: internal energy, enthalpy, and Gibbs free energy
  • Basic grasp of differential calculus in physical contexts
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Students of physics, particularly those studying statistical mechanics and thermodynamics, as well as educators seeking to enhance their teaching of thermodynamical concepts.

jonas_nilsson
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Hello!

I am right now occupied with statistical physics, and of course the connections to thermodynamics are always there. We are especially verifying the old-school thermodynamical results. This leads to a lot of talking about thermodynamical potentials, but I feel that I and most of the students lack a "feeling" for them.

I would appreciate if some people could do some hand-waving and tell me what "feeling" they have developed for the thermodynamical potentials. What do they really describe? I'm sure it would help us out also with the theoretical stuff.


Jonas
 
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Suppose you wanted to conjure a rabbit in your hat. For one thing, you would have to assemble the molecules:

[tex]dU=\mu dN[/tex]

But you would also have to do the work to make room for the rabbit:

[tex]dU = \mu dN + P dV[/tex] (Enthalpy)

And you can extract some energy from the surrounding air to help you:

[tex]dU = \mu dN + P dV - T ds[/tex] (Gibbs free energy)
 

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