Boltzmann Distribution: Calculate Probability of Particle in 4 States

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Homework Help Overview

The discussion revolves around the Boltzmann distribution and its application to calculate the probabilities of a particle being in various energy states. The particle interacts with a reservoir at a temperature of 500 K and can occupy four states, with specified energies for the ground and excited states.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the correct application of the Boltzmann distribution formula, questioning the signs in the exponent and the inclusion of degeneracy in the calculations. There is also discussion regarding the assignment of energy values to the ground and excited states, with some participants suggesting potential corrections to these assignments.

Discussion Status

The discussion is active, with participants providing feedback on the original poster's calculations and questioning the assumptions made regarding energy levels. Some guidance has been offered regarding the correct formulation of the Boltzmann factor and the importance of defining energy levels appropriately.

Contextual Notes

There is confusion regarding the energy values assigned to the ground and excited states, as well as the notation used for temperature and the Boltzmann constant. The original poster's calculations appear to be based on potentially incorrect assumptions about these values.

shayan825
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A certain particle is interacting with a reservoir at 500 k and can be in any four possible states. The ground state has energy 3.1 eV and three excited states all have the same energy. what is the probability that the particle is in ground state? what is the probability that the particle is in a particular excited state? what is the probability that it is in a state of energy -3.0 eV? using Boltzmann distribution

I use the formula (e^E/kT)/sum of e^E/kT but get a wrong answer.
 
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There is a factor of -1 missing from the exponent. Are you also including the degeneracy in the sum?
 
tman12321 said:
There is a factor of -1 missing from the exponent. Are you also including the degeneracy in the sum?

yes, for the first question(the probability that the particle is in the ground state) I get 0.032. e^(-3.1/500k) / e^(-3.1/500k) + 3e^(-3.0/500k). The answer should be 0.7725
 
Why would 3.1 eV be the energy of the ground state, and -3.0 eV be the energy of the excited state? Is it supposed to be the other way around?
 
tman12321 said:
Why would 3.1 eV be the energy of the ground state, and -3.0 eV be the energy of the excited state? Is it supposed to be the other way around?[/QUOTwell,

that's what the book says..ya
 
There seem to be a couple of problems here:
(1) The energy of the ground state should not be greater than the energy of an excited state. The ground state should have the lowest energy. I guess you meant that the ground state is -3.1 eV and the excited state is -3.0 eV, i.e. a 0.1 eV difference. (You were missing this minus sign before).
(2) The Boltzmann factor is Exp[-ΔE/kT], not Exp[ΔE/kT], where ΔE > 0.
(3) You seem to be mixing the usage of k and K. K denotes a temperature in Kelvin and is a unit, and k is the Boltzmann constant, a number. You say that the reservoir is at 500 k, when I think you meant 500 K. You then divide the energies in eV by 500k, but it is unclear whether you think this means 500*k or 500 K. (500*k would be right assuming you're using the value of k in eV/K).

It will be easiest, from a computational standpoint, if you redefine -3.1 eV to be the zero of the energy . Then the ground state has energy 0 eV, and the excited states have energy 0.1 eV.
 

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