Kirkwood-Buff theory of solutions
|
This article is a 'stub' page, it has no, or next to no, content. It is here at the moment to help form part of the structure of SklogWiki. If you add sufficient material to this article then please remove the {{Stub-general}} template from this page. |
Kirkwood-Buff integrals [1]
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle G_{\alpha \beta} = \int_0^\infty \left[{\mathrm g}_{\alpha \beta}^{(2)}({\mathbf r})-1\right] 4\pi r^2 ~d{\mathbf r}}
where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle {\mathrm g}_{\alpha \beta}({\mathbf r})} is the pair distribution function.
References
Related reading
- A. Ben-Naim "Inversion of the Kirkwood–Buff theory of solutions: Application to the water–ethanol system", Journal of Chemical Physics 67 pp. 4884-4890 (1977)
- Arieh Ben-Naim "The Kirkwood–Buff integrals for one-component liquids" Journal of Chemical Physics 128 234501 (2008)
- Elizabeth A. Ploetz, Nikolaos Bentenitis, and Paul E. Smith "Kirkwood–Buff integrals for ideal solutions", Journal of Chemical Physics 132, 164501 (2010)