Chemical Potential: Physical Definition and Applications

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Discussion Overview

The discussion focuses on the concept of "Chemical Potential," exploring its physical definition, implications, and applications in various contexts such as thermodynamics and quantum mechanics. Participants examine its role in systems like Fermi gases and Bose-Einstein condensates, as well as its mathematical representations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses uncertainty about the definition of chemical potential as an energy, suggesting it should have a clearer physical meaning beyond mathematical formulations.
  • Another participant references a source that discusses the rigorous derivation of chemical potential, indicating that there is substantial literature on the topic.
  • It is proposed that chemical potential represents the energy cost of introducing an additional particle into a system.
  • Some participants describe chemical potential as a conjugate thermodynamic variable related to mass, drawing parallels with pressure and volume.
  • A participant mentions the Fermi level in the context of a fermion gas, contrasting it with the energy dynamics in a Bose-Einstein condensate.
  • There is a suggestion that chemical potential can be viewed as a force or pressure rather than strictly as energy, depending on the context of its application.

Areas of Agreement / Disagreement

Participants express differing views on the nature and interpretation of chemical potential, with no consensus reached on a singular definition or understanding. Various perspectives on its role in different physical systems are presented, indicating ongoing debate.

Contextual Notes

Some claims rely on specific mathematical frameworks or theoretical contexts that may not be universally applicable. The discussion includes references to various physical systems, each with unique characteristics that influence the interpretation of chemical potential.

TheDestroyer
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Hello Guys,

I'm searching for the best physical definition for the "Chemical Potential" as an energy, what I know is that it's a constant set through Lagrange multiplicands which is set to sustain the number of particles. Actually I'm still not convinced with that, it's an energy, and should have some physical meaning.

What I also happen to know is:

1- For free electron theorem chemical potential is Fermi surface, mathematically.
2- In Bosé-Einstein condensation chemical potential for bosons falls to zero when T tends to zero, also mathematically.
3- For photons, phonons, magnons and so have zero chemical potential, because the number of quasi-particles isn't conserved, and so also mathematically!

So guys, any "physics" about this?

Thanks :)
 
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Hey guys, is the question that complicated?
 
I don't have it in front of me right now, but as I recall, "Density-functional theory of atoms and molecules" by Parr and Yang has a whole chapter devoted to the rigorous derivation and investigation of the chemical potential. Or you could go look at the papers by Mulliken, who I think was the one who did the original pioneering work.
 
The chemical potential is the amount of energy it costs to introduce another particle into the system.
 
Equivalently, it's the conjugate thermodynamic variable to mass; i.e., [itex]\mu[/itex] is to mass what -P is to V, T is to S, etc.
 
In the context I use it all the time,

it's the Fermi-Level of a large, equilibrium fermion gas.

That explains, to me at least, why at temperature T, why there's still lots of energy in a Fermi gas, whereas no energy in Einstein-Bose condensate.
 
Mapes said:
Equivalently, it's the conjugate thermodynamic variable to mass; i.e., [itex]\mu[/itex] is to mass what -P is to V, T is to S, etc.

If you want to think about chemical potential in terms of being a conjugate thermodynamic variable, then it doesn't act as an energy, but as a force or pressure.

U = T*S - P*V + mu*N + other terms

T P and mu are conjugates that act of S V and N.

From a practical perspective... I imagine the system being in contact with a reservoir of particles and mu being the energy for a particle to pass from the reservoir into the system.
 

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