Every liquid in a closed container establishes an equilibrium with its vapour; the pressure exerted by the vapour at this point is the vapour pressure. When a solute is added, the behaviour of the solution's vapour pressure is governed by Raoult's law.
For a solution of two volatile liquids A and B, Raoult's law states that the partial vapour pressure of each component equals its vapour pressure in the pure state multiplied by its mole fraction in solution:
- $p_A=p_A^0\,x_A$ and $p_B=p_B^0\,x_B$,
- so the total vapour pressure is $p_{total}=p_A^0 x_A+p_B^0 x_B$.
Because $x_B=1-x_A$, this can be written $p_{total}=p_B^0+(p_A^0-p_B^0)x_A$ — a straight line when plotted against $x_A$. The composition of the vapour is richer in the more volatile component than the liquid is.
For a non-volatile solute dissolved in a volatile solvent, only the solvent contributes to the vapour pressure: $p_{solution}=p_{solvent}^0\,x_{solvent}$. Since $x_{solvent}<1$, the vapour pressure is always lowered — this leads directly to the colligative properties.
An ideal solution obeys Raoult's law over the entire composition range. In an ideal solution the A–B interactions are essentially identical to the A–A and B–B interactions, so $\Delta_{mix}H=0$ and $\Delta_{mix}V=0$ (e.g. benzene + toluene, n-hexane + n-heptane).
Non-ideal solutions deviate from Raoult's law:
- Positive deviation: A–B forces are weaker than A–A/B–B forces, so molecules escape more easily — the observed vapour pressure is higher than predicted. Here $\Delta_{mix}H>0$ and $\Delta_{mix}V>0$ (e.g. ethanol + water, acetone + carbon disulphide).
- Negative deviation: A–B forces are stronger (often hydrogen bonding), molecules escape less easily — the vapour pressure is lower than predicted, with $\Delta_{mix}H<0$ and $\Delta_{mix}V<0$ (e.g. acetone + chloroform, $\text{HNO}_3$ + water).
Solutions showing large deviations form azeotropes — constant-boiling mixtures that distil unchanged in composition. Minimum-boiling azeotropes arise from large positive deviation (ethanol–water at 95%), and maximum-boiling azeotropes from large negative deviation ($\text{HNO}_3$–water). Azeotropes cannot be separated into pure components by simple fractional distillation.