(McQuarrie 6-44) In this problem, we'll calculate the fraction of diatomic molecules in a particular rotational level at a temperature T using the rigid rotor approximation. This fraction is governed by the Boltzmann distribution, which says that the number of molecules with energy EJ is proportional to e-Eл/kBT, where kB is the Boltzmann constant and T is the temperature in Kelvin. Because the J-th rotational level has degeneracy (2J + 1), we write, where we have used EJ. = NJ = c(2J+1)e-BJ(J+1)/kBT BJ(J+1). Plot NJ/No versus J for H35 Cl (B = 10.60 cm-1) and 127135 Cl (B = 0.114 cm-1) at 300 K. At approximately what rotational state J is the population ratio NJ/No a maximum in each case? Explain how this distribution of rotational state populations leads to the spectroscopic band structure of the sort seen in McQuarrie Figure 6.4 or in lecture.
(McQuarrie 6-44) In this problem, we'll calculate the fraction of diatomic molecules in a particular rotational level at a temperature T using the rigid rotor approximation. This fraction is governed by the Boltzmann distribution, which says that the number of molecules with energy EJ is proportional to e-Eл/kBT, where kB is the Boltzmann constant and T is the temperature in Kelvin. Because the J-th rotational level has degeneracy (2J + 1), we write, where we have used EJ. = NJ = c(2J+1)e-BJ(J+1)/kBT BJ(J+1). Plot NJ/No versus J for H35 Cl (B = 10.60 cm-1) and 127135 Cl (B = 0.114 cm-1) at 300 K. At approximately what rotational state J is the population ratio NJ/No a maximum in each case? Explain how this distribution of rotational state populations leads to the spectroscopic band structure of the sort seen in McQuarrie Figure 6.4 or in lecture.
Chemistry
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ISBN:9781305957404
Author:Steven S. Zumdahl, Susan A. Zumdahl, Donald J. DeCoste
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Chapter1: Chemical Foundations
Section: Chapter Questions
Problem 1RQ: Define and explain the differences between the following terms. a. law and theory b. theory and...
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Transcribed Image Text:(McQuarrie 6-44) In this problem, we'll calculate the fraction of diatomic molecules in a
particular rotational level at a temperature T using the rigid rotor approximation. This
fraction is governed by the Boltzmann distribution, which says that the number of molecules
with energy EJ is proportional to e-Eл/kBT, where kB is the Boltzmann constant and T is
the temperature in Kelvin. Because the J-th rotational level has degeneracy (2J + 1), we
write,
where we have used EJ. =
NJ = c(2J+1)e-BJ(J+1)/kBT
BJ(J+1). Plot NJ/No versus J for H35 Cl (B = 10.60 cm-1) and
127135 Cl (B = 0.114 cm-1) at 300 K.
At approximately what rotational state J is the population ratio NJ/No a maximum in each
case? Explain how this distribution of rotational state populations leads to the spectroscopic
band structure of the sort seen in McQuarrie Figure 6.4 or in lecture.
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