A What frequencies allow for the long wavelength limit in solid state physics?

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The discussion focuses on the long wavelength limit in solid state physics as described in C. Kittel's "Introduction to Solid State Physics." It highlights the expansion of the cosine function for small values of Ka, leading to a simplified dispersion relation. The participants question the specific frequencies that allow this limit to be valid, noting that it likely varies based on application. The Taylor approximation is discussed, emphasizing the significance of higher-order terms and their relevance depending on the desired accuracy. The conversation underscores the need to consider the context of the application when determining the applicability of the approximation.
Yu-Ting
In the "Introduction to Solid State Physics" by C. Kittel, there is a long wavelength limit in chapter 4 -Phonons I.

When Ka << 1 we can expand cos Ka ≡ 1 - ½ (Ka)2

the dispersion relation will become ω2 = (C/M) K2 a2

Does anyone know what frequencies can allow this long wavelength limit to hold?
 
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I am not sure that there is a standard, since it likely depends on your application.
This is simply the Taylor approximation of the cosine function:
## \cos x = 1 - \frac12 x^2 + \frac{1}{24}x^4 - \frac{1}{720}x^6 ...##
Therefore, you can cut off the higher order terms whenever you feel they are small enough to be insignificant.
For example, when x = .1, your third term is less than .00001. Maybe this is small enough to disregard for your application. Maybe you need your error to be less than 10^-12. Then you should only apply the approximation when x is on the order of 10^-3.
 

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