Statistical mechanics - N distinguishable particles

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SUMMARY

The discussion focuses on calculating the number of microstates for a system of N distinguishable particles, each occupying one of two quantum energy levels, E0 = 0 and E1 = ε, with a total energy of Mε. Participants emphasize the use of binomial coefficients to derive the general equation for this scenario. Specifically, the number of microstates can be determined using the formula nCr(N, M), where N is the number of boxes and M is the number of particles in the excited state. The analogy of tossing coins is also presented to illustrate the counting method for energy distributions.

PREREQUISITES
  • Understanding of quantum mechanics, specifically energy levels and microstates.
  • Familiarity with combinatorial mathematics, particularly binomial coefficients.
  • Knowledge of Bose-Einstein statistics for systems with indistinguishable particles.
  • Basic grasp of statistical mechanics concepts.
NEXT STEPS
  • Research the application of binomial coefficients in statistical mechanics.
  • Study the differences between classical and quantum statistics, focusing on Bose-Einstein and Fermi-Dirac distributions.
  • Explore examples of microstate calculations in quantum systems with varying energy levels.
  • Learn about the implications of distinguishable versus indistinguishable particles in statistical mechanics.
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Students and professionals in physics, particularly those studying statistical mechanics, quantum mechanics, and combinatorial mathematics, will benefit from this discussion.

fuselage
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Homework Statement


"A model system consists of N identical ”boxes” (e.g. quantum wells, atoms), each box with only two quantum levels, energies E0 = 0 and E1 = ε What is the number of microstates corresponding to the macrostate with total energy Mε?"

The Attempt at a Solution


I've done questions like this in the past with a small number of quantum wells, but then I've simply counted the number of possible arrangements. For example, if you have 3 quantum wells with one particle in each, and each well has 4 energy levels (including E0=0), there are 10 different microstates if the macrostate energy is 3ε. But I can't find a general equation.

Does anyone know the general equation(s) that are used to solve a question like this?
 
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Well aware of the binomial coefficients, but I still can't figure it out.
 
You're trying to figure out how to put M units of energy into N boxes.
 
But that doesn't work.

Take the case I described in my attempt at a solution: If you simply count by hand, you will find 10 ways to get 3 units of energy out of a system of three particles each in its own quantum well with four energy levels (Ranging from E0=0 to E3=3). But nCr(3,3) ≠ 10, nor does nCr(4,3).
 
fuselage said:

Homework Statement


"A model system consists of N identical ”boxes” (e.g. quantum wells, atoms), each box with only two quantum levels, energies E0 = 0 and E1 = ε What is the number of microstates corresponding to the macrostate with total energy Mε?"

The Attempt at a Solution


I've done questions like this in the past with a small number of quantum wells, but then I've simply counted the number of possible arrangements. For example, if you have 3 quantum wells with one particle in each, and each well has 4 energy levels (including E0=0), there are 10 different microstates if the macrostate energy is 3ε. But I can't find a general equation.

Does anyone know the general equation(s) that are used to solve a question like this?

Think of tossing a coin N times On each toss, 'heads' ↔ energy level ε, 'tails' ↔ energy level 0. You want to know how many sequences of tosses have M heads and (N-M) tails.

Note: that is essentially "classical" counting. If, instead, your N have integer spins you need to use the so-called "Bose-Einstein" statistics, which gives a radically different result.
 
fuselage said:
But that doesn't work.

Take the case I described in my attempt at a solution: If you simply count by hand, you will find 10 ways to get 3 units of energy out of a system of three particles each in its own quantum well with four energy levels (Ranging from E0=0 to E3=3). But nCr(3,3) ≠ 10, nor does nCr(4,3).
But that's not the case you have here. Each box can be in one of two states, which makes it much easier, and you can use nCr.

For the case where each system can be in more than one state, see http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/disbol.html
 

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