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Statistical Mechanics - Physics at Oregon State University

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A.3. SOLUTIONS FOR CHAPTER 3 245<br />

(A) Calcul<strong>at</strong>e the partition function Z1(T, V ) for N=1.<br />

(B) Calcul<strong>at</strong>e Z(T, V, N).<br />

(C) Calcul<strong>at</strong>e p(T, V, N), S(T, V, N), and µ(T, V, N).<br />

Ignore spin<br />

Transform to integral<br />

Z1(T, V ) = <br />

Z1(T, V ) =<br />

nx,ny,nz<br />

√ cπ − k e B T L n2 x +n2 y +n2z x = cπ<br />

kBT L (nx, ny, nz)<br />

<br />

cπ<br />

−3 <br />

1<br />

kBT L 8<br />

d 3 xe −x<br />

where we extended the range of integr<strong>at</strong>ion to all values of x,and not only one<br />

octant.<br />

3 ∞<br />

kBT L<br />

Z1(T, V ) =<br />

4πx<br />

c2π 0<br />

2 dxe −x<br />

3 3 kBT L<br />

kBT<br />

Z1(T, V ) =<br />

8π = V 8π<br />

c2π<br />

c2π<br />

This is allowed <strong>at</strong> low density, when the points in x-space are close together<br />

Z(T, V, N) = 1<br />

3N N kBT<br />

V (8π)<br />

N! c2π<br />

N<br />

F = −kBT log(Z) = −NkBT log(8π V<br />

3 kBT<br />

) − NkBT<br />

N c2π<br />

Where we used Stirling<br />

Check:<br />

<br />

∂F<br />

p = −<br />

=<br />

∂V T,N<br />

NkBT<br />

V<br />

<br />

∂F<br />

S = −<br />

= NkB log(8π<br />

∂T V,N<br />

V<br />

N<br />

µ =<br />

∂F<br />

∂N<br />

<br />

T,V<br />

3 kBT<br />

) + 4NkB<br />

c2π<br />

= −kBT log(8π V<br />

3 kBT<br />

)<br />

N c2π

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