Debye internal energy for heat capacity

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SUMMARY

The discussion centers on deriving the normal definition of heat capacity using Feynman's definition of internal energy within the Debye theory. The user presents the equation for internal energy, U, and expresses confusion regarding the volume term, V, which they calculate as V = 3N/(4π). They seek clarification on this volume value and its necessity for obtaining the standard Debye heat capacity equation, C_V = 9Nk_B(T/Θ_D)^3∫(0 to Θ_D/T)(x^4e^x)/(e^x - 1)^2 dx. The integration of this equation is also a point of inquiry.

PREREQUISITES
  • Understanding of Debye theory and its application to heat capacity
  • Familiarity with thermodynamic concepts, particularly internal energy and heat capacity
  • Knowledge of integral calculus, specifically techniques for evaluating definite integrals
  • Basic grasp of statistical mechanics and the role of Boltzmann's constant, k_B
NEXT STEPS
  • Study the derivation of the Debye model for heat capacity in solid-state physics
  • Learn about the significance of Debye temperature (Θ_D) in thermal properties of materials
  • Explore advanced integration techniques relevant to statistical mechanics
  • Investigate the relationship between internal energy and heat capacity in thermodynamic systems
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Physicists, materials scientists, and students studying thermodynamics and statistical mechanics, particularly those interested in the Debye model and heat capacity calculations.

cristata
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I'm working from Feynman's definition of internal energy for the Debye theory of heat capacity. I'm trying to use that to derive the normal definition of heat capacity that I've seen. But I'm running into a problem. Note, in the following V_0 is frequency, whereas V is volume (that's how Feynman writes it).

<br /> <br /> U=\frac{3Vk_{B}^{4}T^{4}}{2\pi^{2}\hbar^{3}V_{0}^{3}}\int_{0}^{\Theta_{D}/T}\frac{x^{3}e^{x}}{\left (e^x - 1\right )} dx<br /> <br />

<br /> = \frac{12\pi V k_{B}T^{4}}{\Theta_{D}^{3}}\int_{0}^{\Theta_{D}/T}\frac{x^{3}e^{x}}{\left (e^x - 1\right )} dx<br /> <br />

<br /> <br /> = \frac{4\pi V}{3}\frac{9k_{B}T^{4}}{\Theta_{D}^{3}}\int_{0}^{\Theta_{D}/T}\frac{x^{3}e^{x}}{\left (e^x - 1\right )} dx<br /> <br />

I get V = \frac{3N}{4 \pi}, in order to obtain

<br /> <br /> C_{V} =9Nk_{B}\left (\frac{T}{\Theta_{D}} \right)^{3}\int_{0}^{\Theta_{D}/T}\frac{x^{4}e^{x}}{\left (e^x - 1\right )^{2}} dx<br /> <br />

Why would V be this amount? I don't understand why this must be the case, unless I'm making a mistake somewhere, but I can't see where. The only way I can get the normal definition of Debye heat capacity is if I set V equal to this.

http://books.google.com/books?id=Ou...e+debye+temperature"&cd=1#v=onepage&q&f=false
 
Last edited:
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how can i solve the integration in this equation?
 

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