Partition Function for system with 3 energy levels

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SUMMARY

The discussion focuses on calculating the partition function for a system with three indistinguishable particles (A, B, and C) across three energy levels. The user identifies discrepancies in their method for determining partition functions for distinguishable and indistinguishable particles. Key points include the necessity of treating indistinguishable particles uniformly and the implications of energy level restrictions on particle occupancy. The correct partition functions were derived, but the user seeks clarification on the methodology and the treatment of energy states.

PREREQUISITES
  • Understanding of statistical mechanics and partition functions
  • Familiarity with the concepts of distinguishable vs. indistinguishable particles
  • Knowledge of energy level configurations in quantum systems
  • Basic principles of combinatorics as applied to particle arrangements
NEXT STEPS
  • Study the derivation of partition functions for indistinguishable particles in quantum mechanics
  • Explore the implications of energy level restrictions on particle distributions
  • Learn about the Gibbs paradox and its relevance to indistinguishable particles
  • Investigate advanced combinatorial techniques for counting states in statistical mechanics
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Students and researchers in physics, particularly those focusing on statistical mechanics, quantum mechanics, and thermodynamics, will benefit from this discussion.

MigMRF
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Homework Statement
A system contains 3 particles A, B and C. A can have the energies (0, Delta) while B and C can have the energies (0,Delta,6 Delta). Determine the partition function if the particles and distinguisable. Then determine the partition function if the particles are indistinguishable
Relevant Equations
Z=sum(e^(-beta*E))
I determined the partition function of the particle A, B and C.
1652369926116.png

1652369953371.png

C should be the same as B.
I then considered the situation, where all particles are in the system at the same time, and drew a diagram of all possible arrangements:
1652370142390.png

The grey boxes are the different partitions, given that we can't tell the difference on the particles. The number at the bottom of the table is the sum of all the energies.
From this table i created the two partition functions as shown below:
Distinguishable:
1652370259304.png

Indistinguishable:
1652370313306.png

The correct answer is the following partition functions:
1652370488128.png

1652370510644.png

So my question is. Why does my method not work?

Kind Regards
 
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I agree with your answer for part (a). It looks like the given solution does not include any states where particle A is in the state with energy ##\Delta##.

For part (b), I'm not sure. When the particles are indistinguishable, we can no longer pick out "particle A" and restrict it to the first two energy levels, while allowing the other two particles to be in any of the three levels. This would be treating one of the particles differently than the other two, which doesn't make sense if the particles are indistinguishable. But, maybe they intend for us to interpret the restriction for part (b) as saying that the level with energy ##6 \Delta## is only allowed to hold at most two particles. So, we disallow the state where all three particles occupy this energy level. This appears to be how you interpreted it. If this is what they want, then I agree with your answer for part (b). It looks like their answer leaves out states where there are no particles in the lowest energy level.
 

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