Kierlik and Rosinberg's weighted density approximation: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) m (Changed page to Cite format) | m (Added a sub-section headding) | ||
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| so as to reproduce the [[Exact solution of the Percus Yevick integral equation for hard spheres | Percus-Yevick]]   | so as to reproduce the [[Exact solution of the Percus Yevick integral equation for hard spheres | Percus-Yevick]]   | ||
| [[Direct correlation function |direct pair correlation function]] for the uniform [[hard sphere model]]. | [[Direct correlation function |direct pair correlation function]] for the uniform [[hard sphere model]]. | ||
| ==Aplication to polyatomic fluids== | |||
| ==See also== | ==See also== | ||
| *[[Tarazona's weighted density approximation]] | *[[Tarazona's weighted density approximation]] | ||
Latest revision as of 12:43, 28 September 2010
In the Kierlik and Rosinberg's weighted density approximation [1] [2] four weighting functions are used so as to reproduce the Percus-Yevick direct pair correlation function for the uniform hard sphere model.
Aplication to polyatomic fluids[edit]
See also[edit]
References[edit]
- ↑ E. Kierlik and M. L. Rosinberg "Free-energy density functional for the inhomogeneous hard-sphere fluid: Application to interfacial adsorption", Physical Review A 42 pp. 3382-3387 (1990)
- ↑ E. Kierlik and M. L. Rosinberg "Density-functional theory for inhomogeneous fluids: Adsorption of binary mixtures", Physical Review A 44 pp. 5025-5037 (1991)
