Every real gas has a characteristic critical temperature (Tc) above which it is physically impossible to
liquefy the gas by applying pressure alone, no matter how great that pressure is. Below its critical temperature,
sufficient pressure will condense a gas into a liquid; above it, the gas simply becomes more compressed without
ever separating into two distinct phases. This means cooling a gas below its critical temperature is a necessary
prerequisite before liquefaction by compression can succeed — pressure by itself is never sufficient if the gas
starts out above Tc.
Two related quantities complete the description: the critical pressure (Pc) is the minimum pressure needed
to liquefy the gas when it is held exactly at its critical temperature, and the critical volume (Vc) is the
molar volume of the gas under these critical conditions. Together, (Tc,Pc,Vc) define the critical point,
the unique condition at which the distinction between the liquid and gaseous states of a substance disappears
entirely — the densities of the liquid and vapour phases become identical.
Critical temperature values vary enormously between gases and directly determine how readily each can be
liquefied under ordinary laboratory or industrial conditions. Carbon dioxide, with Tc=31.1∘C —
only slightly above normal room temperature — can be liquefied simply by compressing it at or below room
temperature, exactly how CO2 fire extinguishers and carbonated-beverage cylinders store liquid
CO2 under moderate pressure. Ammonia, with Tc=132.4∘C, liquefies even more readily at …