Example 4.7
What is ( S/ V)Tfor a gas that follows a van der Waals equation of state?
Solution
The Maxwell relationship in equation 4.36 shows that ( S/ V)Tis equal to
( p/ T)V. Using the van der Waals equation,
p
V
n
RT
nb
a
V
n
2
2
Taking the derivative ofpwith respect to Tat constant volume gives
T
p
V
V
nR
nb
Therefore, by Maxwell’s relationships,
V
S
T
V
nR
nb
We do not need to measure the entropy changes experimentally. We can get
the isothermal change in entropy versus volume from the van der Waals pa-
rameters.
Example 4.8
In Chapter 1, we showed that
T
p
V
where is the expansion coefficient and is the isothermal compressibility.
For mercury,1.82 10 ^4 /K and 3.87 10 ^5 /atm at 20°C. Determine
how entropy changes with volume under isothermal conditions at this tem-
perature.
Solution
The derivative of interest is ( S/ V)T, which by equation 4.36 is equal to
( p/ T)V. Using the expansion coefficient and the isothermal compress-
ibility:
T
p
V
3
1
.8
.8
7
2
1
1
0
0
(^5) /
4
a
/
t
K
m
4.70
at
K
m
These do not seem to be appropriate units for entropy and volume. However,
if we note that
at
K
m
1
L
0
1
a
.3
tm
2J
101.32
J/
L
K
we can convert our answer into more identifiable units and find that
V
S
T
476
J/
L
K
102 CHAPTER 4 Free Energy and Chemical Potential