Statistical Mechanics - Physics at Oregon State University
Statistical Mechanics - Physics at Oregon State University
Statistical Mechanics - Physics at Oregon State University
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40 CHAPTER 2. THE CANONICAL ENSEMBLE<br />
A system has only two quantum st<strong>at</strong>es available. St<strong>at</strong>e number one has<br />
energy zero and st<strong>at</strong>e number two has energy ɛ > 0.<br />
(a) Calcul<strong>at</strong>e the partition function for this system.<br />
(b) Calcul<strong>at</strong>e U(T) and S(T).<br />
(c) Calcul<strong>at</strong>e the he<strong>at</strong> capacity as a function of temper<strong>at</strong>ure.<br />
The he<strong>at</strong> capacity as a function of temper<strong>at</strong>ure peaks <strong>at</strong> a certain value of<br />
the temper<strong>at</strong>ure. This peak is called a Schottky anomaly.<br />
(d) Is this peak associ<strong>at</strong>ed with a phase transition? Give an argument justifying<br />
your answer.<br />
Problem 4.<br />
(From Reif) A sample of mineral oil is placed in an external magnetic field<br />
H. Each proton has spin 1<br />
2 and a magnetic moment µ; it can, therefore, have two<br />
possible energies ɛ = ∓µH, corresponding to the two possible orient<strong>at</strong>ions of<br />
its spin. An applied radio frequency field can induce transitions between these<br />
two energy levels if its frequency ν s<strong>at</strong>isfies the Bohr condition hν = 2µH. The<br />
power absorbed from this radi<strong>at</strong>ion field is then proportional to the difference<br />
in the number of nuclei in these two energy levels. Assume th<strong>at</strong> the protons in<br />
the mineral oil are in thermal equilibrium <strong>at</strong> a temper<strong>at</strong>ure T which is so high<br />
th<strong>at</strong> µH ≪ kT . How does the absorbed power depend on the temper<strong>at</strong>ure T of<br />
the sample?<br />
Problem 5.<br />
(From Reif) A system consists of N weakly interacting particles, each of<br />
which can be in either of two st<strong>at</strong>es with respective energies ɛ1 and ɛ2, where<br />
ɛ1 < ɛ2.<br />
(a) Without explicit calcul<strong>at</strong>ion, make a qualit<strong>at</strong>ive plot of the mean energy<br />
Ē of the system as a function of its temper<strong>at</strong>ure T. Wh<strong>at</strong> is Ē in the limit of<br />
very low and very high temper<strong>at</strong>ures? Roughly near wh<strong>at</strong> temper<strong>at</strong>ure does Ē<br />
change from its low to its high temper<strong>at</strong>ure limiting values?<br />
(b) Using the result of (a), make a qualit<strong>at</strong>ive plot of the he<strong>at</strong> capacity CV<br />
(<strong>at</strong> constant volume) as a function of the temper<strong>at</strong>ure T.<br />
(c) Calcul<strong>at</strong>e explicitly the mean energy Ē(T ) and he<strong>at</strong> capacity CV (T )<br />
of this system. Verify th<strong>at</strong> your expressions exhibit the qualit<strong>at</strong>ive fe<strong>at</strong>ures<br />
discussed in (a) and (b).<br />
Problem 6.