a point on a phase diagram corresponding to the critical state. The critical point of two-phase liquid-vapor equilibrium is the end point on the equilibrium curve and is characterized by the critical values of the temperature Tc, pressure Pc, and volume Vc (see Table 1).
| Table 1. Parameters of the liquid-vapor critical point of some substances | |||
|---|---|---|---|
| Tc (oK)> | pc (atm)* | Vc × 106 (m3 /mole) | |
| * 1 atm = 1.01 × 106 N/m2 | |||
| Helium........... | 5.3 | 2.26 | 57.8 |
| Hydrogen........... | 33.0 | 12.8 | 61.8 |
| Oxygen................. | 154.8 | 50.1 | 74.4 |
| Nitrogen........... | 126.2 | 33.5 | 90.1 |
| Carbon dioxide......... | 304.2 | 72.9 | 94.0 |
| Propane............ | 369.9 | 42.0 | 200 |
| Alcohol (ethyl)............ | 516.3 | 63.0 | 167 |
| Bromine.............. | 584 | 102 | 144 |
| Water........... | 647 | 218.3 | 56 |
| Iodine........... | 785 | 116 | – |
| Sulfur........... | 1313 | 116 | – |
| Mercury........... | 1750 | 1,500 | 44 |
| Cesium........... | 2030 | 115 | 332 |
The critical point is a particular case of the phase transition point and is characterized by the loss of thermodynamic stability with respect to the density or composition of the substance. On one side of the critical point the substance is homogeneous (usually when T > Tc); on the other it separates into phases. For mixtures or solutions a distinction should be made between the critical point of liquid-vapor equilibrium and the critical point of equilibrium of phases of different composition that are in the same state of aggregation (liquid-liquid or gas-gas). In this connection the critical point of mixtures (or solutions) is also characterized by the critical concentration xc. As a result of the increased number of parameters determining the system’s state, mixtures have not a critical point but rather a critical curve, whose points differ in the values of Tc, pc, Vc, and xc. Critical phenomena are observed in the region of the critical point.