The number of oscillations in the frequency range υ and υ + dυ is given as dn. Using quantum mechanical principle dn is evaluated as
dn = 4π²v . ʋ² dʋ ....................(1)
c³
V - volume of the crystal, c - velocity of light and υ - frequency of oscillator.
There are two kinds of waves with in elastic materials. They are transverse waves with velocity c₁ with two directions of polarization for any given direction of propagation and longitudinal waves with velocity c₁. The total number of modes of vibration between ʋ and ʋ + dʋ will be
dn = ( 2 + 1 ) 4π²V. ʋ² dʋ ............(2)
ct² cl³
One mole of crystal contains N number of atoms or ions or molecules which will have (3N-6) vibrational degrees of freedom. As N is large ; it's approximated to 3N. Hence the upper limit for the allowed vibrational frequency ʋD is equal to 3N.
∫ dn = ∫₀ᵛᴰ 4π² V. v² (2 + 1 ) ʋ² dʋ = 3N
ct³ cl³
4π²V ( 2 + 1 ) ʋ³D = 3N
ct³ cl³ 3
( 2 + 1 ) = 9N ..........(3)
ct³ cl³ 4π² V ʋ³D
Substitute equation (3) into equation (2)
dn = 9N . 4π²V. ʋ² dʋ =
4π² V ʋ³D
9Nʋ²dʋ ...................(4)
ʋ³D
The average energy of oscillator, vibrational modes in a crystal is assumed to be same as the average energy of oscillator in a black body as given by Planck.
E = E.
eE/kT-1
∴ Energy of dn vibrational modes = dn. E
= ( 9Nʋ²dʋ ) ( E )
ʋ³D eE/kT− 1
= ( 9Nʋ²dʋ ) ( hʋ )
ʋ³D ehʋ/kT − 1
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