Combining rules: Difference between revisions
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Carl McBride (talk | contribs) m (→Admur and Mason: Corrected Ref. number.) |
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(Ref. 3) | (Ref. 3) | ||
====Admur and Mason==== | ====Admur and Mason==== | ||
For the [[second virial coefficient]] of a mixture (Ref. | For the [[second virial coefficient]] of a mixture (Ref. 4) | ||
:<math>B_{ij} = \frac{\left(B_{ii}^{1/3}+B_{jj}^{1/3}\right)^3}{8}</math> | :<math>B_{ij} = \frac{\left(B_{ii}^{1/3}+B_{jj}^{1/3}\right)^3}{8}</math> | ||
==References== | ==References== | ||
#[http://dx.doi.org/10.1080/00268970010020041 Jérôme Delhommelle; Philippe Millié "Inadequacy of the Lorentz-Berthelot combining rules for accurate predictions of equilibrium properties by molecular simulation", Molecular Physics '''99''' pp. 619-625 (2001)] | #[http://dx.doi.org/10.1080/00268970010020041 Jérôme Delhommelle; Philippe Millié "Inadequacy of the Lorentz-Berthelot combining rules for accurate predictions of equilibrium properties by molecular simulation", Molecular Physics '''99''' pp. 619-625 (2001)] |
Revision as of 15:56, 29 January 2008
The combining rules (also known as mixing rules) for binary mixtures are variously given by
Berthelot rule
Lorentz rule
See also Lennard-Jones model
Kong rules
(Ref. 2)
Waldman-Hagler rules
(Ref. 3)
Admur and Mason
For the second virial coefficient of a mixture (Ref. 4)
References
- Jérôme Delhommelle; Philippe Millié "Inadequacy of the Lorentz-Berthelot combining rules for accurate predictions of equilibrium properties by molecular simulation", Molecular Physics 99 pp. 619-625 (2001)
- Chang Lyoul Kong "Combining rules for intermolecular potential parameters. II. Rules for the Lennard-Jones (12–6) potential and the Morse potential", Journal of Chemical Physics 59 pp. 2464-2467 (1973)
- M. Waldman and A. T. Hagler "New combining rules for rare-gas Van der-Waals parameters", Journal of Computational Chemistry 14 pp. 1077-1084 (1993)
- I. Amdur and E. A. Mason "Properties of Gases at Very High Temperatures", Physics of Fluids 1 pp. 370-383 (1958)