5. GrΓΌneisen constant. (a) Show that the free energy of a phonon mode of frequency 𝜔 is 𝑘𝐵&#1198

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5. GrΓΌneisen constant. (a) Show that the free energy of a phonon mode of frequency 𝜔 is 𝑘𝐵&#1198

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5. GrΓΌneisen constant. (a) Show that the free energy of a phonon
mode of frequency πœ” is
π‘˜π΅π‘‡ 𝐼𝑛 [2 𝑠𝑖𝑛h (β„πœ”/2π‘˜π΅π‘‡)]. It is necessary to retain the zero-point
energy 1/2(β„πœ”) to obtain
this result. (b) If A is the fractional volume change, then the
free energy of the crystal may be
written as 𝐹(Ξ”, T) = (1/2) 𝐡Δ^2 + π‘˜π΅π‘‡ βˆ‘π‘™π‘› [2 𝑠𝑖𝑛h (β„πœ”πΎ/2π‘˜π΅π‘‡)] where
B is the bulk modulus. Assume that the volume dependence of πœ”π‘˜ is
π›Ώπœ”/πœ” = βˆ’π›ΎΞ”, where 𝛾 is known as the GrΓΌneisen constant. If 𝛾 is
taken as independent of the mode K, show that F is a minimum
with respect to A when 𝐡Δ = π›Ύβˆ‘ ( 1/2 β„πœ”) coth ( β„πœ”/2π‘˜π΅π‘‡ ), and show
that this may be written in terms of the thermal energy density as
Ξ” = π›Ύπ‘ˆ(𝑇)/𝐡 (c) Show that on the Debye model 𝛾 = βˆ’ πœ•lnπœƒ/πœ•ln𝑉 .
Note: Many approximations are involved in this theory: the result
(a) is valid only if πœ” is independent of temperature; 𝛾 may be
quite for different Inodes.
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