An impurity atom sitting at a fixed site in a crystal has three non-degenerate states

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Statistical foundations and the equilibrium ensembles · Statistical foundations and the equilibrium ensembles

Thermal Physics, Ch The Boltzmann factor, the canonical ensemble and the partition function

Problem

An impurity atom sitting at a fixed site in a crystal has three non-degenerate states, of energies 00, ε\varepsilon and 3ε3\varepsilon, with ε=6.00×10−21 J\varepsilon = 6.00\times10^{-21}\,\mathrm{J}. The crystal acts as a reservoir at T=300 KT = 300\,\mathrm{K}, and the coupling is weak, so the atom's energy levels are those listed. Take kB=1.381×10−23 J K−1k_B = 1.381\times10^{-23}\,\mathrm{J\,K^{-1}} and give numerical answers to three significant figures. ((a)) Evaluate the partition function ZZ of one impurity atom. ((b)) Find the probability of each of the three states. ((c)) Find the mean energy UU of one impurity atom, in joules. ((d)) A sample contains N=5.0×1020N = 5.0\times10^{20} such impurity atoms, each at its own fixed site and independent of all the others. Find the total mean energy of the impurities, in joules.

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