Find the average energy and the heat capacity at constant volume for a two-state system. Take the two energies of the system to be ± ε/2. (b) Show that the result for CV is proportional to 1/T2 for kT >>ε , and that it is of the form CV ≈ (constant/T2 e ^(−ε/kT) at low temperature, kT << ε
The partition function of the two state system is
This can also be written in terms of hyperbolic functions
where
the average energy is
Therefore
the heat capacity is
b) For high temperature
therefore
For low temperature
,
therefore
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