Calculate real gas properties accounting for molecular volume and intermolecular forces.
The Van der Waals equation is a modification of the ideal gas law that accounts for the finite size of gas molecules and the attractive forces between them. It provides a more accurate description of real gas behavior, especially at high pressures and low temperatures.
Key Insight: The Van der Waals equation introduces two correction factors: 'a' accounts for intermolecular attraction, and 'b' accounts for the finite volume occupied by gas molecules. These corrections become increasingly important as gas density increases.
Pressure Correction (a): The term a(n/V)² accounts for the reduction in pressure due to attractive forces between molecules. As molecules attract each other, they exert less force on the container walls, resulting in lower measured pressure.
Volume Correction (b): The term nb accounts for the volume occupied by the gas molecules themselves. In the ideal gas law, molecules are treated as point particles with no volume, but real molecules have finite size.
Van der Waals Constants: The constants a and b are specific to each gas and are determined experimentally. They depend on the strength of intermolecular forces and the size of the molecules.
| Gas | Formula | a (Pa·m⁶/mol²) | b (m³/mol) | Critical Temperature (K) |
|---|---|---|---|---|
| Hydrogen | H₂ | 0.0247 | 2.65×10⁻⁵ | 33.2 |
| Helium | He | 0.00346 | 2.38×10⁻⁵ | 5.2 |
| Nitrogen | N₂ | 0.1408 | 3.91×10⁻⁵ | 126.2 |
| Oxygen | O₂ | 0.1378 | 3.18×10⁻⁵ | 154.6 |
| Carbon Dioxide | CO₂ | 0.3640 | 4.27×10⁻⁵ | 304.2 |
| Methane | CH₄ | 0.2283 | 4.28×10⁻⁵ | 190.6 |
| Water Vapor | H₂O | 0.5536 | 3.05×10⁻⁵ | 647.1 |
The Van der Waals equation provides significantly better accuracy than the ideal gas law in several situations:
While more accurate than the ideal gas law, the Van der Waals equation has limitations:
Historical Context: The Van der Waals equation was proposed by Johannes Diderik van der Waals in 1873, for which he received the Nobel Prize in Physics in 1910. His work was groundbreaking because it provided a theoretical basis for understanding real gas behavior and the continuity between gases and liquids.