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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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464 Jacopo Tomasi, Benedetta Mennucci, Chiara Cappelli<br />

Figure 8.5. Example <strong>of</strong> the radial distribution function<br />

g(r) <strong>of</strong> a typical monoatomic liquid. Figure 8.6. Examples <strong>of</strong> h(r) and c(r) functions for a typical<br />

monoatomic liquid.<br />

a) the site-site correlation function g αβ(r αβ) proportional to the probability<br />

density that sites α and β on different molecules are separated by distance r,<br />

regardless <strong>of</strong> molecular orientations;<br />

b) the total correlation function h(r 12ω 1ω 2)= g(r 12ω 1ω 2)-1;<br />

c) the direct correlation function c(r 12ω 1ω 2).<br />

Simple examples <strong>of</strong> h and c functions are reported in Figure 8.6.<br />

In the list above, item (a) implies definite sites within molecules; these sites may be the<br />

nuclei themselves or sites at arbitrary locations within the molecules.<br />

In addition, the total correlation, h, between molecules 1 and 2 can be separated into<br />

two parts: (i) a direct effect <strong>of</strong> 1 on 2 which is short-ranged and is characterized by c, and (ii)<br />

and indirect effect in which 1 influences other molecules, 3, 4, etc., which in turn affect 2.<br />

The indirect effect is the sum <strong>of</strong> all contributions from other molecules averaged over their<br />

configurations. For an isotropic and homogeneous fluid formed by non-spherical molecules,<br />

we have<br />

( r ) ( r ) r ( r ) ( r )<br />

h 12ωω 1 2 = c 12ωω 1 2 + ρ∫ d 3 c 13ωω 1 3 h 32ω3ω2 [8.76]<br />

ω3<br />

which is the generalization <strong>of</strong> the Ornstein-Zernike (OZ) equation 50 to non-spherical molecules.<br />

The OZ equation is the starting point for many theories <strong>of</strong> the pair correlation function<br />

(PY, HNC, etc.); however, numerical solutions starting from [8.76] are complicated by<br />

the large number <strong>of</strong> variables involved. By expanding the direct and total correlation functions<br />

in spherical harmonics, one obtains a set <strong>of</strong> algebraically coupled equations relating<br />

the harmonic coefficients <strong>of</strong> h and c. These equations involve only one variable in the place<br />

<strong>of</strong> many in the original OZ equation. In addition, the theories we shall describe below truncate<br />

the infinite set <strong>of</strong> coupled equations into a finite set, thereby enabling a reasonably simple<br />

solution to be carried out.

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