Kirkwood-Buff theory of solutions

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Kirkwood-Buff integrals [1] \[G_{\alpha \beta} = \int_0^\infty \left[{\mathrm g}_{\alpha \beta}^{(2)}({\mathbf r})-1\right] 4\pi r^2 ~d{\mathbf r}\] where \({\mathrm g}_{\alpha \beta}({\mathbf r})\) is the pair distribution function.

[edit] References

  1. John G. Kirkwood and Frank P. Buff "The Statistical Mechanical Theory of Solutions. I", Journal of Chemical Physics 19 pp. 774-777 (1951)

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