Colligative properties of solutions and Raoult's laws

Analysis of colligative properties of dilute solutions: vapor pressure lowering, boiling and freezing point changes, osmotic pressure. Formulations of Raoult's and van 't Hoff's laws, isotonic coefficient, everyday examples.

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Concept of colligative properties of solutions

Colligative properties are properties of dilute solutions that depend only on the number of particles of a non-volatile solute and do not depend on its chemical nature. The decisive role is played by the number of particles in the solution, rather than their individual characteristics. Colligative properties include the lowering of the saturated vapor pressure of the solvent over the solution, elevation of the boiling point, depression of the freezing point, and osmotic pressure.

The theoretical basis of all quantitative relationships is Le Chatelier's principle: when a solute is added, the equilibrium between the liquid and gaseous phases of the solvent shifts, which leads to a change in the physical constants of the solution.

Raoult's first law

The vapor pressure of a solvent over a solution of a non-volatile substance is always lower than over the pure solvent at the same temperature. The explanation is based on the dynamic equilibrium of evaporation ⇌ condensation. When a non-volatile substance is added to the solvent, part of the solvent molecules is bound by the solvation process and leaves the equilibrium. According to Le Chatelier's principle, the equilibrium shifts toward the liquid phase—condensation predominates, so the vapor pressure decreases.

Quantitatively, the vapor pressure lowering is proportional to the mole fraction of the solute. It is the mole fraction that is used in the first formulation of Raoult's law.

Raoult's second law: boiling and freezing

The second law describes the change in phase transition temperatures:

Here m is the molal concentration (moles of solute per 1 kg of solvent). Molality is used because, unlike molarity which changes due to thermal expansion of the solution, it is temperature-independent.

E is the ebullioscopic constant, K is the cryoscopic constant. These are tabulated characteristics of the solvent: for water, cyclohexane, naphthalene, and benzene they are known and depend only on the nature of the solvent.

Van 't Hoff's isotonic coefficient

The isotonic coefficient i accounts for the dissociation of the solute and effectively shows into how many particles a formula unit breaks down in solution.

The larger i is, the more pronounced the colligative effects are at the same molality.

Third law: osmotic pressure (van 't Hoff's law)

When two solutions of different concentrations are separated by a semipermeable membrane, the solvent spontaneously passes into the more concentrated solution. The pressure that must be applied to stop this transition is called osmotic pressure.

Van 't Hoff's equation: π = i · C · R · T, where C is the molar concentration (this is the only colligative law using molarity), R is the universal gas constant, and T is the absolute temperature in kelvins. Osmosis forms the basis of plant cell turgor, renal function, and infusion therapy.

Practical examples

Key points

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