RMS displacement of a diatomic atom

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SUMMARY

The discussion centers on calculating the root mean square (RMS) displacement of a diatomic atom with an effective spring constant of k = 4.0×10−3 N/m. The RMS displacement is given as x = 5.0×10−10 m, leading to the conclusion that the temperature required to achieve this displacement is 72 K. The relevant equations utilized include = 7kT/2 and U = 7nRT/2, indicating a classical harmonic oscillator model for the diatomic atom.

PREREQUISITES
  • Understanding of classical mechanics, specifically harmonic oscillators
  • Familiarity with thermodynamic principles, including the ideal gas law
  • Knowledge of statistical mechanics, particularly the equipartition theorem
  • Basic proficiency in manipulating equations involving temperature and energy
NEXT STEPS
  • Study the principles of harmonic oscillators in classical mechanics
  • Explore the equipartition theorem in statistical mechanics
  • Learn about the relationship between temperature and RMS displacement in oscillatory systems
  • Investigate the implications of non-rigid rotators in molecular physics
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Students and professionals in physics, particularly those focusing on molecular dynamics, thermodynamics, and statistical mechanics, will benefit from this discussion.

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Homework Statement


A hypothetical atom is diatomic containing two identical atoms separated by an equilibrium distance. About this distance the atoms vibrate with the electric forces providing an effective spring constant of k = 4.0×10^−3 N/m. As the temperature of the sample is increased the amplitude of the vibration increases. At what temperature will the rms displacement of the atoms be x= 5.0×10−10m? (Answer: 72 K)


Homework Equations


<E> = 7kT/2

U = 7nRT/2


The Attempt at a Solution



I assumed that because of spring like nature of the atoms, this atom was a diatomic non rigid rotator, which is how I have those relevant equations. I am unsure if this initial assumption is even correct. Even if it was, I still don't have an idea of how to proceed from there.
 
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It seems that you need to be modelling the bond as a harmonic oscillator. I imagine also that this should be considered as a classical oscillator, and not quantum mechanical. Then, you need to take out your classical mechanics textbook and figure out the relation between the energy of the oscillator and the amplitude of the oscillation, which will be related to the rms displacement ##\sqrt{\langle x^2 \rangle}##.
 
Got it, thanks.
 

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