Callen H.B - Thermodynamics And An Introduction To Thermostatistics · Problem 17.3-4

QUANTUM FLUIDS

Physics — Statistical Mechanics · adsorption-vibrational-grand-canonical

Problem

Suppose the adsorption model to be augmented by assuming that two adsorbed molecules on the same site interact in a vibrational mode of frequency ω\omega. Thus the energy of an empty site is zero, the energy of a singly occupied site is ε1\varepsilon_1, and the energy of a doubly occupied site can take any of the values ε2+n′ℏω\varepsilon_2 + n'\hbar\omega, with n′=0,1,2,…n' = 0, 1, 2, \ldots Calculate aa) The grand canonical partition sum bb) The grand canonical potential cc) The mean occupation number, as computed directly from (a) dd) The mean occupation number, as computed directly from (b) ee) The probability that the system is in the state with n=2n = 2 and n′=3n' = 3 Answer: Denoting εj−μ\varepsilon_j - \mu by εj′\varepsilon_j', (b)Ψ=N~kBTln⁡(1+e−βε1′+e−βε2′1−e−βℏω)(b) \quad \Psi = \tilde{N}k_BT\ln\left(1 + e^{-\beta\varepsilon_1'} + \frac{e^{-\beta\varepsilon_2'}}{1 - e^{-\beta\hbar\omega}}\right) (c,d)nˉ=(1−e−βℏω)e−βε1′+2e−βε2′(1−e−βℏω)(1+e−βε1′)+e−βε2′(c,d) \quad \bar{n} = \frac{(1 - e^{-\beta\hbar\omega})e^{-\beta\varepsilon_1'} + 2e^{-\beta\varepsilon_2'}}{(1-e^{-\beta\hbar\omega})(1 + e^{-\beta\varepsilon_1'}) + e^{-\beta\varepsilon_2'}} (e)f2,3=e−β(ε2′+2ℏω)/g(e) \quad f_{2,3} = e^{-\beta(\varepsilon_2' + 2\hbar\omega)}/g

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