Fraction of Hydrogen Atoms in First Excited State

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Homework Help Overview

The problem involves determining the fraction of hydrogen atoms in the first excited state at a temperature of 8000 K. It references the energy difference between the ground state and the first excited state of hydrogen, requiring an understanding of statistical mechanics and the Boltzmann distribution.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of the Boltzmann factor to find the fraction of hydrogen atoms in the excited state. There is an initial attempt to relate energy to temperature and the Boltzmann constant, followed by questions about the proper application of the Boltzmann factor.

Discussion Status

Some participants have provided guidance on using the Boltzmann factor, and there appears to be a growing understanding of how to apply it to the problem. Clarifications are being sought, indicating an active exploration of the concepts involved.

Contextual Notes

There may be assumptions regarding the ideal behavior of hydrogen atoms and the applicability of the Boltzmann distribution at the given temperature. The original poster expresses uncertainty about the approach, indicating a need for further clarification on the method.

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Homework Statement


1. Homework Statement
The temperature of the surface of a certain star is 8000 K. Most hydrogen atoms at the surface of the star are in the electronic ground state. What is the approximate fraction of the hydrogen atoms that are in the first excited state (and therefore could emit a photon)? The energy of the first excited state above the ground state is (-13.6/22 eV) - (-13.6 eV) = 10.2 eV = 1.632e-18 J.

Homework Equations


Kb = 1.38e-23 J/K
1/T = E/Kb

The Attempt at a Solution


I don't really know how to do this problem. My guess was to divide the energy in joules by the temperature and then divide by the Boltzmann constant to make it unitless.

(1.632e-18/8000)/(1.38e-23)=14.8
 
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Hmm... You are right so far, but you might want to use the Boltzmann factor for this problem as well.
 
What do you mean? Could you clarify?
 
Wait I think I understand. Are you saying take e raised to this value?
 
Yeah I got it. Thanks
 
Yes, using the Boltzmann factor you get:

\frac{P(E_1)}{P(E_0)} = e^{-\frac{E_1-E_0}{kT}}

where P(E) is the probability the electron is in the state with energy E.

Since a vast majority of the electrons are in the ground state, you can say P(E_0)\approx 1.
 

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