[PoM] Average rotational energy

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SUMMARY

The discussion focuses on calculating the average rotational energy per molecule of a rarefied gas of HF at a temperature of 50 K, using the wave number of rotational absorption for the transition L = 2 → 3, which is 121.5 cm-1. The calculated average rotational energy is established as Erot = 5.493 x 10-22 J. The classical limit formula for average rotational energy is applied, and the relationship between rotational frequency and moment of inertia is explored. The challenge presented is determining how to limit the number of energy levels considered in the calculation.

PREREQUISITES
  • Understanding of rotational energy calculations in molecular physics
  • Familiarity with the concepts of moment of inertia and angular frequency
  • Knowledge of quantum mechanics principles, specifically energy quantization
  • Basic proficiency in thermodynamics, particularly the relationship between temperature and energy
NEXT STEPS
  • Study the derivation of the moment of inertia for diatomic molecules
  • Learn about the implications of limiting energy levels in quantum mechanical systems
  • Explore the application of the Boltzmann distribution in rotational energy calculations
  • Investigate the significance of wave numbers in molecular spectroscopy
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This discussion is beneficial for physics students, molecular chemists, and researchers involved in thermodynamics and quantum mechanics, particularly those focusing on rotational dynamics of gases.

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Homework Statement


Determines the average energy of rotation (per molecule) of a rarefied gas of HF at T = 50 K, knowing that the wave number of rotational absorption for the transition L = 2 → 3 worth 121.5 cm-1. [Hint: it performs the calculation by limiting the number of levels taken into account, making sure to get the numerical result by 5%.]

Solution:##E_{rot}=5.493*10^{-22} [J]##

The Attempt at a Solution


In the classical limit, the average rotational energy per molecule is:

##\frac{E_{rot}}{N}=\frac{1}{2}I\omega^2##

For transition L = 2 → 3, I have:

##\nu=\frac{E_{rot}}{h}=\frac{\hbar^2l(l+1)}{2hI} \Rightarrow I=\frac{\hbar^2l(l+1)}{\nu 2h}##

then,

##\omega^2=(2\pi \nu)^2=\frac{2k_BT}{I}=3.3318*10^{17} [rad/s]##

so:

##E_{rot}=\frac{1}{2}I\omega^2=k_BT=6.903*10^{-22} [J]###

But, in what way I have to limit the number of levels taken into account?
 
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