Van der Waals equation of state: Difference between revisions

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The '''van der Waals equation of state''' is
The '''van der Waals equation of state''', developed by [[ Johannes Diderik van der Waals]], can be written as


:<math> \left. p = \frac{ n R T}{V - n b } - a \left( \frac{ n}{V} \right)^2  \right. </math>.
:<math> \left. p = \frac{ n R T}{V - n b } - a \left( \frac{ n}{V} \right)^2  \right. </math>.

Revision as of 11:21, 22 May 2007

The van der Waals equation of state, developed by Johannes Diderik van der Waals, can be written as

p=nRTV−nb−a(nV)2.

where:

  • p is the pressure
  • V is the volume
  • n is the number of moles
  • T is the absolute temperature

The van der Waals equation of state 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.

Critical point

The critical point for the van der Waals equation of state can be found at

Tc=8a27bR,
pc=a27b2

and at

vc=3b.

References

  1. J. D. van der Waals "On the Continuity of the Gaseous and Liquid States", Dover Publications ISBN: 0486495930
  2. Luis Gonzalez MacDowell and Peter Virnau "El integrante lazo de Van der Waals", Anales de la Real Sociedad Española de Química 101 #1 pp. 19-30 (2005)