Van der Waals Equation
The van der Waals equation, (p + an²/V²)(V − nb) = nRT, is an equation of state proposed by Johannes Diderik van der Waals in 1873. The parameter a accounts for attractive forces between molecules, which reduce the pressure on the walls, and b for the volume excluded by the molecules themselves. It was the first equation of state to describe both gas and liquid and to predict a critical point, earning van der Waals the 1910 Nobel Prize in Physics.
Curious
The ideal gas law treats molecules as dimensionless points that ignore one another. That works at low density but cannot explain why gases condense into liquids. Van der Waals made two small corrections: subtract the volume the molecules themselves occupy, and reduce the pressure because neighbouring molecules attract and slow each other down before they hit the wall.
With just these two changes, a single equation describes gas, liquid and the transition between them, including the critical point, above which liquid and gas become indistinguishable. The weak attractions it introduced are now called van der Waals forces (see Johannes Diderik van der Waals).
Exploring
| Gas | a (Pa m6 mol−2) | b (10−5 m³/mol) |
|---|---|---|
| Helium | 0.00346 | 2.38 |
| Nitrogen | 0.137 | 3.87 |
| Carbon dioxide | 0.364 | 4.27 |
| Water | 0.554 | 3.05 |
Deep Dive
Corresponding states. Writing the equation in reduced variables pr = p/pc, Vr = V/Vc, Tr = T/Tc gives a universal form with no substance-specific parameters, (pr + 3/Vr²)(3Vr − 1) = 8Tr. Van der Waals's law of corresponding states (1880) holds approximately for many simple fluids and guided Kamerlingh Onnes in liquefying helium (see Heike Kamerlingh Onnes).
Critical behaviour. Near the critical point, van der Waals theory is a mean-field theory and predicts critical exponents such as β = 1/2 for the difference between liquid and gas densities. Experiments give β ≈ 0.326, the same as the three-dimensional Ising model, a universality explained by renormalisation-group theory (Wilson, Nobel Prize 1982). Modern engineering uses cubic equations of state such as Peng–Robinson, or reference equations fitted to extensive data.
Virial expansion. At low density the van der Waals equation gives a second virial coefficient B(T) = b − a/RT, which is negative at low temperature (attraction dominates) and positive at high temperature, crossing zero at the Boyle temperature TB = a/Rb (see Kinetic Theory of Gases).
Concept Relationship Map
Requires: ideal gas law, intermolecular forces
Enables: critical point, phase transitions, corresponding states
Commonly confused with: an accurate engineering equation of state
Sources
- van der Waals, J.D. (1873). Doctoral thesis, Leiden University.
- The Nobel Foundation (1910). The Nobel Prize in Physics 1910. nobelprize.org.
- Atkins, P., de Paula, J. (2014). Atkins' Physical Chemistry (10th ed.). Oxford University Press.