Thermodynamics ★★ Intermediate

🧪 Van der Waals Gas

Real gases differ from ideal ones: molecules attract each other at moderate distances and repel at close range. Van der Waals corrected the ideal gas law with two parameters — a (intermolecular attraction) and b (excluded volume) — producing P-V isotherms that capture gas, liquid-vapour coexistence, and the critical point.

Tc = K Pc = bar Vc = L/mol T/Tc = Zc = 3/8 = 0.375
(P + a/Vm²)(Vm − b) = RT  |  Tc = 8a/(27Rb)  |  Pc = a/(27b²)  |  Vc = 3b

Van der Waals Equation of State (1873)

Johannes Diderik van der Waals proposed two corrections to the ideal gas law PV = nRT:

  • Pressure correction (+a/Vm²) — molecules attract each other, reducing the pressure that would be exerted on the walls.
  • Volume correction (−b) — molecules have a finite size, so the free volume available is less than the total volume.

Below the critical temperature Tc, the isotherm develops an S-shaped loop (the van der Waals loop). The physical equilibrium line — the horizontal coexistence plateau — is determined by Maxwell's equal-area rule: the areas above and below the horizontal tie-line are equal.

At the critical point, the three roots of the cubic in V merge: Tc = 8a/(27Rb), Pc = a/(27b²), Vc = 3b, giving a universal compressibility factor Zc = PcVc/(RTc) = 3/8.