Applied to the Condensed States
As we saw in Section 9.3, the kinetic molecular theory of gases has five postulates: (1) the volume occupied by a gas is largely empty space; by comparison, the real volume of the gas molecules is negligible; (2) there are no attractive forces between the molecules of a gas; (3) the gaseous molecules are in constant, random, rapid, straight-line motion; (4) the molecules collide frequently with one another and with the walls of the container, but no energy is lost by these collisions; and (5) the average kinetic energy of the molecules is proportional to the temperature of the sample.
These postulates do not hold completely for liquids and solids. We have already seen that, when the average kinetic energy of a gas sample decreases, the sample eventually reaches a temperature at which this kinetic energy is no longer great enough to overcome the attractive forces between the molecules, and they start to interact with one another. These forces become more effective as the temperature lowers, and the sample becomes first a liquid and then, at a lower temperature, a solid. In these states, the sample has the properties described in Section 9.1. For condensed states, the kinetic molecular theory must be modified. The properties of molecules in these states can be described as follows: