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Statistical Mechanics - Physics at Oregon State University

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4.7. PROBLEMS FOR CHAPTER 4 87<br />

4.7 Problems for chapter 4<br />

Problem 1.<br />

Imagineons have weird st<strong>at</strong>istics. The number of particles in a given orbital<br />

can be 0,1, or2.<br />

( A.) Calcul<strong>at</strong>e the Imagineon distribution function fI(ɛ).<br />

( B.) Sketch the shape of this function with ɛ in units of kBT .<br />

Fermions with spin 1<br />

2 can also have two particles in one orbital (in the traditional<br />

sense the word orbital does not include a spin quantum number, like the 1s<br />

orbital in an <strong>at</strong>om).<br />

( C.) Calcul<strong>at</strong>e the distribution function for the number of particles in each<br />

orbital.<br />

( D.) Why is this result the same/different from the result of B?<br />

Problem 2.<br />

Assume th<strong>at</strong> for a system of N fermions the Fermi level coincides with the<br />

energy level of M orbitals.<br />

(A.) Calcul<strong>at</strong>e the entropy <strong>at</strong> T = 0.<br />

(B.) In the thermodynamic limit N → ∞ this entropy is non-zero. Wh<strong>at</strong> do<br />

you know about M in this case?<br />

Problem 3.<br />

Starting with Ω(T, µ, V ) = −kBT <br />

orb log Zorb(T, µ, V ) for a system of independent,<br />

identical bosons, show th<strong>at</strong> the entropy is given by<br />

<br />

S = −kB (fBE(ɛo) log(fBE(ɛo)) − (1 + fBE(ɛo)) log(1 + fBE(ɛo))) (4.88)<br />

Problem 4.<br />

orb<br />

The Maxwell distribution function fM is given by fM (ɛ; T, µ) = e 1<br />

k B T (µ−ɛ) .<br />

Show th<strong>at</strong>

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