Chemical Potential: Physical Definition and Applications

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SUMMARY

The discussion centers on the concept of "Chemical Potential" in physics, defined as the energy required to introduce an additional particle into a system. Key points include its mathematical representation as the Fermi surface in the free electron theorem, its behavior in Bose-Einstein condensation where it approaches zero at absolute zero temperature, and its zero value for non-conserved quasi-particles like photons and phonons. The chemical potential serves as a conjugate thermodynamic variable to mass, analogous to pressure and volume, and is crucial in understanding systems in thermal equilibrium.

PREREQUISITES
  • Understanding of thermodynamic variables and their relationships
  • Familiarity with Fermi gas and Bose-Einstein condensation concepts
  • Knowledge of density-functional theory, particularly the work of Parr and Yang
  • Basic principles of statistical mechanics and particle conservation
NEXT STEPS
  • Study "Density-functional theory of atoms and molecules" by Parr and Yang for in-depth understanding
  • Research the original papers by Robert Mulliken on chemical potential
  • Explore the mathematical derivation of chemical potential in thermodynamic systems
  • Investigate the implications of chemical potential in various physical systems, including Fermi gases and Bose-Einstein condensates
USEFUL FOR

Physicists, graduate students in physical sciences, and researchers interested in thermodynamics and statistical mechanics, particularly those focusing on chemical potential and its applications in various physical systems.

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., \mu 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., \mu 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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