compound H 2 O. One of the noteworthy points is that there are actually several
types of solid H 2 O, that is, ice. Note the pressure and temperature scales, how-
ever. We are not likely to experience these forms of ice outside the laboratory.
Figure 6.7 shows a phase diagram of helium. Because helium is a gas at
temperatures down to 4.2 K, the temperature axis on this diagram does not
have a large temperature range. At the other extreme, Figure 6.8 shows a phase
diagram of carbon. Notice the regions where diamond is the stable phase.
Although pressure and temperature are the common variables for phase
diagrams in chemistry, volume can also be plotted on an axis in a phase dia-
gram, as shown in Figure 6.9. There are also three-dimensional phase dia-
grams that plot pressure, volume, and temperature; Figure 6.10 shows an ex-
ample of that.
Phase diagrams are very useful in helping to understand how single-
component systems act under a change in condition: simply plot the change on
6.6 Phase Diagrams and the Phase Rule 157
40
0
0.0001
Temperature (K)
100
Pressure (bar)
Superfluid
B phase
0.001 0.01 0.1 1 10
30
20
10
Solid
Gas
Superfluid
A phase
Normal liquid
Figure 6.7 The phase diagram of helium, He, does not need a large temperature
range. Notice that solid He does not exist unless pressures are large.
103
10 –^2
0
Temperature ( 103 K)
6
Pressure (kbar)
54321
102
10
1
10 –^1
Gas
Diamond
Graphite
Liquid
T
Volume
V 1
Temperature
V 2
Gas
P
Liquid
Volume
Pressure
1-phase
2-phase region
region
Temperature
Figure 6.10 A three-dimensional phase diagram
can plot the phases present in a system for given sets
of pressures, temperatures, and volumes.
Figure 6.8 A phase diagram of carbon, showing where
the graphite allotrope is stable and where the diamond
allotrope is stable.
Figure 6.9 An example of a temperature-volume phase diagram. At a certain pres-
sure P, the phase diagram specifies what phase must be present except between V 1 and
V 2 (for the given pressure). Under these conditions, a varying amount of liquid phase
(shaded area) may be present and still satisfy the given conditions ofTand P. In part
because of this ambiguity, temperature-volume phase diagrams aren’t as common as
pressure-temperature phase diagrams.