Chemical potential different for different systems?

Click For Summary
SUMMARY

The discussion focuses on the differences in chemical potential between the canonical ensemble and the grand canonical ensemble in statistical mechanics. In the canonical ensemble, the chemical potential is defined as μ(T,V,N), while in the grand canonical ensemble, it is defined as μ(T,V,⟨N⟩). As the number of particles approaches infinity, both chemical potentials converge, indicating that they become equivalent in the thermodynamic limit. This equivalence allows for the modeling of open systems as closed systems by appropriately setting the chemical potential.

PREREQUISITES
  • Understanding of statistical mechanics concepts, particularly ensembles.
  • Familiarity with the canonical ensemble and grand canonical ensemble.
  • Knowledge of chemical potential and its mathematical representation.
  • Basic grasp of thermodynamic limits and their implications.
NEXT STEPS
  • Study the mathematical derivation of chemical potential in the canonical ensemble.
  • Explore the implications of the grand canonical ensemble on particle number fluctuations.
  • Investigate the concept of thermodynamic limits in statistical mechanics.
  • Learn about applications of chemical potential in real-world systems, such as gases and liquids.
USEFUL FOR

Students and researchers in physics, particularly those focusing on statistical mechanics, thermodynamics, and chemical thermodynamics.

pivoxa15
Messages
2,250
Reaction score
1

Homework Statement


For a given phenomena of macroscopic particles.

If we model it using the canonical ensemble then we get a certain chemical potential u.

But if we model it using the Grand Canonical system, we get a varying chemcial potential that depends on the average number of particles in the system.

So two different chemical potentials for the two systems. But in the thermodynamic limit of n-> infinity, both u equals each other.

That sounds right doesn't it?
 
Physics news on Phys.org
Yeah, you're basically right.

In any of the systems in the canonical ensemble, the chemical potential is given by

[tex]\mu(T,V,N)[/tex]

whereas in any of the systems in the grandcanonical ensemble, it's given by

[tex]\mu(T,V,\langle N \rangle)[/tex]

Now, in the "thermodynamic limit" as you have called it, the number of particles in any of the grandcanonical systems is *MUCH* more likely to be equal to [itex]\langle N \rangle[/itex] than to any other number. So it's equivalent to having a closed system with a fixed number of particles [itex]\langle N \rangle[/itex].

If I have an open system and I want it to be equivalent to a closed system with a particular number of particles [itex]N_0 [/tex], I'd have to somehow <b>pick </b> or <b>set</b> the value of [itex]\mu [/tex] such that [itex]\langle N \rangle = N_0[/itex] for that system.[/itex][/itex]
 
Last edited:

Similar threads

Replies
1
Views
3K
Replies
4
Views
1K
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 37 ·
2
Replies
37
Views
6K
  • · Replies 2 ·
Replies
2
Views
3K
Replies
1
Views
2K