Connecting the microcanonical with the (grand) canonical ensemble

Click For Summary
SUMMARY

This discussion focuses on the relationship between the microcanonical ensemble and the canonical/grand canonical ensembles, particularly in the context of Helium gas. The microcanonical ensemble is used to derive the Bose-Einstein (BE) distribution and the Gibbs distribution under specific conditions, such as low occupancy limits. The temperature and chemical potential are derived using Lagrange multipliers, which are essential for maintaining constant energy and particle numbers. The conversation highlights the limitations of applying the microcanonical ensemble to systems with strong interactions, quantum degeneracy, and entanglement, advocating for a Gibbsian approach for more complex systems.

PREREQUISITES
  • Understanding of microcanonical and canonical ensembles in statistical mechanics
  • Familiarity with Bose-Einstein distribution and Gibbs distribution
  • Knowledge of Lagrange multipliers and their application in thermodynamics
  • Concepts of quantum degeneracy and entanglement in quantum gases
NEXT STEPS
  • Study the Gibbsian picture of statistical thermodynamics for complex systems
  • Explore the Sackur-Tetrode equation for ideal gases and its implications
  • Learn about the Gross-Pitaevskii equation for weakly interacting Bose gases
  • Investigate the quantum microcanonical ensemble as discussed in Landau and Lifshitz
USEFUL FOR

Physicists, particularly those specializing in statistical mechanics, quantum gases, and thermodynamics, as well as researchers exploring the connections between different statistical ensembles.

  • #31
Philip Koeck said:
Also answering vanHees!

Maybe one could start with chapter 3 in Reif and the loop back to the first 2 chapters in case that's necessary.
How do we do this? Just start a thread and hope for interest?
Which Reif? The Berkeley physics course one or the more advanced standalone textbook? I'm fine with both.
 
Science news on Phys.org
  • #32
Philip Koeck said:
I certainly use Stirling's formula a lot, so all my results can only be valid for large N. I agree completely.

One big problem occurs in section 6 when I try to specify what the chemical potential and the density of states actually is for an ideal gas. That's where I switch to an integral with an infinite upper limit although the total energy is finite. I guess that's related to what you point out.
I really only use an infinite upper limit so that I can evaluate the integrals for total energy and particle number.
Until section 6 I only consider a finite set of discrete energy levels, which ought to mean that I can keep the highest energy level below the total energy simply by definition.
I simply shouldn't try to apply the theory to anything real! :)
That's one of the subtler points of stat. mech. The "thermodynamic limit" is not as simple as it looks!
 
  • #33
vanhees71 said:
Which Reif? The Berkeley physics course one or the more advanced standalone textbook? I'm fine with both.
I would say the Berkeley one.
 
  • #34
That's a good choice. The other book is very detailed and sometimes you can get lost in these details, though it's a very good source if you want to study the issues in more depth from different points of view.
 
  • #35
vanhees71 said:
That's a good choice. The other book is very detailed and sometimes you can get lost in these details, though it's a very good source if you want to study the issues in more depth from different points of view.
How do we do this? Should I just start a thread called "Reading Reif together" or something like that, or should this come from an advisor?
 
  • Like
Likes   Reactions: vanhees71
  • #36
I don't know. I'd say, just post such an "intro posting" and see what happens.
 
  • Like
Likes   Reactions: Twigg and Philip Koeck
  • #37
vanhees71 said:
I don't know. I'd say, just post such an "intro posting" and see what happens.
It's started.
 
  • Like
Likes   Reactions: vanhees71
  • #38
Philip Koeck said:
Then I'll go a step further and decide that the system should consist of a single atom.
It doesn't matter whether the number of particles is ##N=1## or ##N=10^{23}##. One has to distinguish the number of particles in the system (which doesn't need to be large), from the number of systems in the ensemble (which must be large). In the Gibbs theory of ensembles, an ensemble is a fictitious ensemble; it's a thing we imagine to conceptualize the notion of probability. For example, you can say that the probability of a single coin to be in the heads state is 1/2, but to conceptualize this you can imagine that you flipped this single coin a 1000 times.

That being said, once you said that ##N## is fixed (##N=1## in your case), you can talk about a canonical ensemble, but not about a grand-canonical ensemble.
 
  • Like
Likes   Reactions: Philip Koeck and vanhees71

Similar threads

  • · Replies 15 ·
Replies
15
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 1 ·
Replies
1
Views
37K