Van der Waals equation of state: Difference between revisions
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* <math> T </math> is the absolute [[temperature]], | * <math> T </math> is the absolute [[temperature]], | ||
* <math> R </math> is the [[molar gas constant]]; <math> R = N_A k_B </math>, with <math> N_A </math> being the [[Avogadro constant]] and <math>k_B</math> being the [[Boltzmann constant]]. | * <math> R </math> is the [[molar gas constant]]; <math> R = N_A k_B </math>, with <math> N_A </math> being the [[Avogadro constant]] and <math>k_B</math> being the [[Boltzmann constant]]. | ||
==Critical point== | |||
At the [[Critical points |critical point]] one has <math>\left.\frac{\partial p}{\partial v}\right|_{T=T_c}=0 </math>, and <math>\left.\frac{\partial^2 p}{\partial v^2}\right|_{T=T_c}=0 </math>, leading to | |||
:<math> | :<math>T_c= \frac{8a}{27bR}</math> | ||
:<math>p_c=\frac{a}{27b^2}</math> | :<math>p_c=\frac{a}{27b^2}</math> | ||
:<math>\left.V_c\right.=3b</math>. | :<math>\left.V_c\right.=3b</math>. | ||
and | |||
:<math>\frac{p_cV_c}{T_c}= \frac{3R}{8}</math> | |||
which then leads to | |||
:<math>a= \frac{27}{64}\frac{R^2T_c^2}{P_c}</math> | |||
:<math>b= \frac{RT_c}{8P_c}</math> | |||
==Dimensionless formulation== | ==Dimensionless formulation== | ||
If one takes the following reduced quantities | If one takes the following reduced quantities |
Revision as of 13:00, 20 October 2009
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 introduces somehow the repulsive behavior between pairs of molecules at short distances, it represents the minimum molar volume of the system, whereas 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
- .
where:
- is the pressure,
- is the volume,
- is the number of moles,
- is the absolute temperature,
- is the molar gas constant; , with being the Avogadro constant and being the Boltzmann constant.
Critical point
At the critical point one has , and , leading to
- .
and
which then leads to
Dimensionless formulation
If one takes the following reduced quantities
one arrives at
The following image is a plot of the isotherms = 0.85, 0.90, 0.95, 1.0 and 1.05 (from bottom to top) for the van der Waals equation of state:
Maxwell's equal area construction
Interesting reading
- Johannes Diderik van der Waals "The Equation of State for Gases and Liquids", Nobel Lecture, December 12, 1910
- 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)
References
- J. D. van der Waals "Over de Continuiteit van den Gas- en Vloeistoftoestand", doctoral thesis, Leiden, A,W, Sijthoff (1873).
English translation: