Van der Waals equation of state

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The van der Waals equation of state, developed by Johannes Diderik van der Waals, takes into account two features that are absent in the ideal gas equation of state; the parameter b introduces somehow the repulsive behavior between pairs of molecules at short distances, it represents the minimum molar volume of the system, whereas a measures the attractive interactions between the molecules. The van der Waals equation of state leads to a liquid-vapor equilibrium at low temperatures, with the corresponding critical point.

Equation of state

The van der Waals equation of state can be written as

p=nRTV−nb−a(nV)2.

where:

Critical point

At the critical point one has ∂p∂v|T=Tc=0, and ∂2p∂v2|T=Tc=0, leading to

Tc=8a27bR


pc=a27b2


Vc=3b.


and


pcVcTc=3R8


which then leads to


a=2764R2Tc2Pc


b=RTc8Pc

Dimensionless formulation

If one takes the following reduced quantities

p~=ppc;V~=VVc;t~=TTc;

one arrives at

p~=8t~3V~−1−3V~2

The following image is a plot of the isotherms T/Tc = 0.85, 0.90, 0.95, 1.0 and 1.05 (from bottom to top) for the van der Waals equation of state:

Plot of the isotherms T/T_c = 0.85, 0.90, 0.95, 1.0 and 1.05 for the van der Waals equation of state
Plot of the isotherms T/T_c = 0.85, 0.90, 0.95, 1.0 and 1.05 for the van der Waals equation of state

Maxwell's equal area construction

Interesting reading

References

  • J. D. van der Waals "Over de Continuiteit van den Gas- en Vloeistoftoestand", doctoral thesis, Leiden, A,W, Sijthoff (1873).

English translation: