Is it Valid to Treat a Solid as a Large Molecule in Calculating Specific Heat?

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SUMMARY

The discussion centers on the validity of treating a solid as a large molecule when calculating specific heat. It emphasizes that the Hamiltonian for a solid body, represented as \(\mathcal{H}_1=\mathcal{V}^{*}+\sum_{j=1}^{3n} \big(\frac{\widetilde{p}_s^2}{2m}+\frac{K_s}{2} \widetilde{u_s}^2\big)\), mirrors that of any system with N particles, not exclusively an N-atom molecule. This raises questions about the justification of this assumption in thermodynamic calculations. The discussion highlights the need for clarity in the application of molecular models to bulk materials.

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In the discussion of calculating specific heat for a solid, it is assumed that the whole solid body is a molecule with N atoms and the Hamiltonian of this solid is similar to that of a molecule with N atoms, i.e.
## \mathcal{H}_1=\mathcal{V}^{*}+\sum_{j=1}^{3n} \big(\frac{\widetilde{p}_s^2}{2m}+\frac{K_s}{2} \widetilde{u_s}^2\big) ##. How this assumption of taking solid as a huge molecule is justified?
 
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That's the Hamiltonian of *any* system of N particles, not just an N-atom molecule.
 
Thanks, modified the Hamiltonian in the question
.
 

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