Basic Statistical Mechanics question

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SUMMARY

The discussion centers on calculating the microstates of an isolated system with three distinguishable particles (A, B, C) and a total energy of U=3E. The possible distributions of energy among the particles are represented by the sets {2, 0, 0, 1}, {1, 1, 1, 0}, and {0, 3, 0, 0}. Each set corresponds to specific energy levels of the particles, confirming that these are the only configurations that yield the total energy of 3E. The analysis demonstrates the application of statistical mechanics principles to derive microstate configurations.

PREREQUISITES
  • Understanding of statistical mechanics concepts, specifically microstates and macrostates.
  • Familiarity with energy quantization in isolated systems.
  • Knowledge of distinguishable particle systems and their energy distributions.
  • Basic proficiency in combinatorial mathematics to analyze particle arrangements.
NEXT STEPS
  • Study the principles of statistical mechanics, focusing on microstate and macrostate definitions.
  • Explore energy distribution in quantum systems, particularly for distinguishable particles.
  • Learn about combinatorial methods for calculating possible configurations in statistical mechanics.
  • Investigate the implications of energy quantization on thermodynamic properties of systems.
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Students of physics, particularly those studying statistical mechanics, as well as educators and researchers looking to deepen their understanding of energy distributions in isolated systems.

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Homework Statement



An isolated system has N=3 distinguishable particles A, B, C with single particle states equally spaced at intervalsof E and a total energy U=3E.
ie the macrostate is defined by N=3, U=3E.

The system has single particle levels 0, E, 2E, 3E.



Homework Equations





The Attempt at a Solution



The beginning of the solution then begins with:

ni = {2, 0, 0, 1}
{1, 1, 1, 0}
{0, 3, 0, 0}

How were these sets of number obtained?

Thanks for any help!
 
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These are the possible microstates. For {2, 0, 0, 1} , you have two particles with energy ε=0 and one particle with ε=3E, so Ʃεi = 3E, as it should. For {1, 1, 1, 0}, one particle has ε=0, second has ε=E and third has ε=2E. For {0, 3, 0, 0} all particles have energy E. You should be able to convince yourself that these are the only possibilities to get total energy of 3E.
 

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