Relationship between Debye Temperature and Speed of Sound in Metals

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SUMMARY

The relationship between Debye temperature and speed of sound in metals is established through the equation \(\Theta_D = \hbar \omega_D / k_b\), where \(\omega_D\) is derived from the speed of sound \(c\) and the Debye wave vector \(k_D\). For Silicon and Lead, with speeds of sound of 9150 m/s and 1320 m/s respectively, the Debye temperature can be estimated by first determining the cutoff frequency using the linear dispersion relation. The long wavelength limit indicates that \(k = \pi/a\), where \(a\) is the unit cell dimension. This relationship is crucial for understanding thermal properties in solid-state physics.

PREREQUISITES
  • Understanding of Debye temperature and its significance in solid-state physics
  • Familiarity with the linear dispersion relation in wave mechanics
  • Knowledge of the concepts of wave vectors and unit cell dimensions
  • Proficiency in using fundamental constants such as \(\hbar\) (reduced Planck's constant) and \(k_b\) (Boltzmann constant)
NEXT STEPS
  • Research the calculation of Debye temperature for various materials
  • Study the linear dispersion relation and its applications in solid-state physics
  • Explore the significance of the Debye model in understanding specific heat capacity
  • Learn about the relationship between crystal structure and sound velocity in solids
USEFUL FOR

Students and researchers in solid-state physics, materials scientists, and anyone interested in the thermal properties of metals and their relationship to sound propagation.

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Homework Statement



I'm struggling to understand the relationship between the Debye temperature and the speed of sound in a substance. An example problem given is:

Estimate the Debye Temperature of Silicon and Lead, given that their respective speeds of sound are 9150 m/s and 1320 m/s. (not sure if its relevant to this part of the question but also given graph of C_v vs T for Argon from which you can read a Debye temp of about ~80K).


Homework Equations



\Theta_D = \hbar \omega_D / k_b
where \omega_D = c k_D
and k_D is the radius of the "Debye Sphere"

The Attempt at a Solution



Not sure how to attempt this to be honest, there seems like there are too many unknowns. Presumably there is some simplifying assumption, but I'm not sure where to begin...
 
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you first need to find the cut off frequency wd by using the linear dispersion relation. For the Debye model w is proportional to k. At the long wavelength limit k=pi/a where a is the dimension of the unit cell. Having found w you can then substitute it back into your first equation for temperature.
 
captainjack2000 said:
you first need to find the cut off frequency wd by using the linear dispersion relation. For the Debye model w is proportional to k. At the long wavelength limit k=pi/a where a is the dimension of the unit cell. Having found w you can then substitute it back into your first equation for temperature.

Thanks yes this makes sense. I had funnily enough just worked it out 5 mins ago, I forgot that k could be found fairly easily by estimating a.
 

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