334 Problems €4 Solutions on Thermodynamics d Statistical Mechanics
Keeping the first two terms, we have
N2
2v
= VN (1 + -. (-.I) ,
4ra3
In& = NlnV +In
where r = -.
Hence
3
r
2v
M NlnV - -N2 ,
so that
u==-lnz=-kT, a 3N
aP 2
and
J
C, = -Nk,
2
giving
pv=1+-. rN
NkT 2N
Thus
rN 27ra3
2 3
Ai(T) = - = -N.
2146
Consider a classical system of N point particles of mass m in a volume
V at temperature T. Let U be the total energy of the system, p the pressure.
The particles interact through a two-body central potential