Elementary Boltzmann Statistics

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Homework Help Overview

The discussion revolves around elementary Boltzmann statistics, specifically focusing on the equilibrium state of a system of particles and the calculation of the partition function for both single and multiple particles.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants explore the definition and calculation of the partition function, questioning whether the provided equation for a single particle's partition function applies to the entire system. There is also discussion about the distinction between the partition function for indistinguishable and distinguishable particles.

Discussion Status

Some participants express confusion regarding the correct interpretation of the partition function for a single particle versus N particles. Guidance is offered regarding the nature of the partition function in classical mechanics, and references to external sources are made to clarify definitions.

Contextual Notes

Participants note that the particles are not indistinguishable, which may influence the calculation of the partition function. There is an ongoing exploration of definitions and assumptions related to the partition function in statistical mechanics.

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***SOLVED***

Homework Statement



A system of particles is at equilibrium. What is the proportion of particles in the ground state?

The Attempt at a Solution



[tex]P(\epsilon_{s})=\frac{exp(-0/\tau)}{1+exp(\frac{-\epsilon_{s}}{\tau})+exp(\frac{-2\epsilon_{s}}{\tau})}[/tex]

Is that right? This is a really basic problem but I haven't dealt with this in a while. Thanks!
 
Last edited:
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Seems right to me.
 
So what threw me for a little bit of a loop about this was that the denominator of the equation I posted is the partition function.
[tex] Z_{1}= 1+exp(\frac{-\epsilon_{s}}{\tau})+exp(\frac{-2\epsilon_{s}}{\tau})[/tex]

Then later I am asked what the partition function is. I guess the point is that Z above is the partition function for a single particle, not the whole system which would be

[tex]Z_{1}^{N}[/tex]

does that seem right? Edit: The particles are not indistinguishable.
 
I don't quite understand what you're saying. The partition function is exactly what you posted. You seem to think that there's another partition function for the whole system, which isn't the case.
 
Well then we are both confused :). I am asked

1. what is the partition function of a single particle?
2. what is the partition function for N particles?

Thanks for your time I really appreciate it.

Edit: Quoting Kittel & Kroemer, "If we have one atom in each of N distinct boxes (which is equivalent to N in one box, because they are non-interacting I assume), the partition function is the product of the separate one atom partion functions." Thanks for your help again.
 
Last edited:
So in other words for N particles we are talking about the grand canonical partition function.
 

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