3.8 The Einstein Model

For ω = ω0 we find for the inner energy

U = 3 ∫ dωD(ω) ℏω exp ⁡ (ℏω kT ) - 1 = ℏω0 exp ⁡ (ℏω0 kT ) - 13N.

(3.43)

and:

CV = dU dT = 3Nℏω (eℏω kT - 1) 2 eℏω kT ℏω kT .

(3.44)

For high temperatures we again get:

CV = 3Nk.

(3.45)