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The Redlich-Kwong Equation and its Modifications

The equations of state most commonly used at the present time to represent gas behavior at moderate to high pressures are based on a simple modification of the van der Waals equation published by Redlich and Kwong in 1949  [Pg.403]

There is no really good theoretical justification for the two changes in the denominator of the a-term but the agreement with observed data is considerably improved. .. [Pg.403]

In the original RK equation, the parameters a and b were constants, independent of P and T. Since the RK equation first appeared in print, it too has undergone many modifications in an attempt to further improve its fit. Many of these modified Redlich-Kwong equations are summarized by Holloway (1977) and Kerrick and Jacobs (1981), and involve writing the a and b parameters as a function of T, P, or both T and P. The MRK equation of Kerrick and Jacobs fits most of the data for H2O and CO2 at elevated P and T to better than 1 % and is chosen for discussion here. [Pg.403]

The MRK equation of Kerrick and Jacobs keeps b constant but writes a as a function of both P and T  [Pg.404]

Here you can see that the repulsion term holds b constant but is more complicated (which gives it better flexibility). The a parameter in the attraction term is written as a simple polynomial function of 1 jV (hence of P) and of T. This is a MRK equation with 10 adjustable parameters, so naturally it fits real data considerably better than the original RK equation, which has only two parameters. [Pg.404]


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Equation modifications

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Redlich-Kwong

Redlich-Kwong equation

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