à phonons is approximately Gak.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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Show that 22.12 imples 22.14

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Exercise 22.3. Debye theory of the lattice heat capacity of solids.
At low temperatures, the heat capacity of dielectric solids is known to be pro-
portional to T³, just as the heat capacity of the radiation field as derived from
(22.10) is proportional to T8. We call a quantized elastic wave a phonon, in
analogy to a photon as a quantized electromagnetic wave. The dispersion
relation for long-wavelength phonons is approximately
w = C,k,
where c, is the velocity of sound. (a) If c, is taken as constant for all three
longitudinal and transverse modes of vibration, show that the heat capacity
per unit volume
(22.12)
с, 3D (12тЧkN /5)(T/Ө),
where the Debye temperature O is given by
(22.13)
kO = hc,(6m*N)½,
N being the number of atoms per unit volume. It is instructive to rewrite
(22.12) for a cube of side L
au
272
(22.14)
C.
5
hc,L
Transcribed Image Text:Exercise 22.3. Debye theory of the lattice heat capacity of solids. At low temperatures, the heat capacity of dielectric solids is known to be pro- portional to T³, just as the heat capacity of the radiation field as derived from (22.10) is proportional to T8. We call a quantized elastic wave a phonon, in analogy to a photon as a quantized electromagnetic wave. The dispersion relation for long-wavelength phonons is approximately w = C,k, where c, is the velocity of sound. (a) If c, is taken as constant for all three longitudinal and transverse modes of vibration, show that the heat capacity per unit volume (22.12) с, 3D (12тЧkN /5)(T/Ө), where the Debye temperature O is given by (22.13) kO = hc,(6m*N)½, N being the number of atoms per unit volume. It is instructive to rewrite (22.12) for a cube of side L au 272 (22.14) C. 5 hc,L
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