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Statistical Mechanics - Physics at Oregon State University

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66 CHAPTER 3. VARIABLE NUMBER OF PARTICLES<br />

A system can be in one of four st<strong>at</strong>es. These are<br />

(1) No particles, zero energy<br />

(2) One particle, energy ɛ1<br />

(3) One particle, energy ɛ2<br />

(4) Two particles, energy ɛ1 + ɛ2 + I<br />

where ɛ2 > ɛ1 > 0 and I < 0. This sign of I is unusual. The temper<strong>at</strong>ure<br />

is T and the chemical potential is µ. This is a very simple model, and in order<br />

to make this realistic we should really consider many of these systems together.<br />

Th<strong>at</strong> is not asked in this question, though.<br />

(A) Calcul<strong>at</strong>e the grand partition function<br />

(B) Calcul<strong>at</strong>e N(T, µ)<br />

(C) Calcul<strong>at</strong>e <br />

∂N<br />

∂T µ and show th<strong>at</strong> this can be neg<strong>at</strong>ive. Wh<strong>at</strong> does th<strong>at</strong><br />

mean?

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