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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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

Thermodynamical properties<br />

Paying attention again to calculations for acetone and chlor<strong>of</strong>orm, we would like to mention<br />

two papers by the Regensburg group 113,114 exploiting molecular Ornstein-Zernike (MOZ)<br />

theory and site-site Ornstein-Zernike (SSOZ) theory for the calculation <strong>of</strong> excess internal<br />

energies. In the MOZ framework, the internal excess energy per molecule is computed by a<br />

configurational average <strong>of</strong> the pair potential V acting between molecules:<br />

ex ρ<br />

E = ∫ ∫ ∫V(<br />

R ) g( R ) dR d d<br />

2 2 12, Ω1, Ω2 12, Ω1, Ω2 12 Ω1 Ω2<br />

[8.134]<br />

Ω<br />

with ρ the density <strong>of</strong> molecules.<br />

Using instead SSOZ, E ex can be directly calculated from the site-site distribution function,<br />

g αβ, as:<br />

∞ k k<br />

πρ∫ ∑ ∑ αβ<br />

0 α=<br />

1 β=<br />

1<br />

() ()<br />

ex<br />

2<br />

E = 2 g r V r r dr<br />

αβ<br />

[8.135]<br />

where k is the number <strong>of</strong> sites per molecule.<br />

In both cases the calculated values are in good agreement with experimental data and<br />

with calculations done exploiting the Monte Carlo computer simulation. In this case, E ex can<br />

be obtained as:<br />

E<br />

ex<br />

N N k k<br />

1 ε zzer<br />

rf −1<br />

0<br />

= ∑ ∑∑∑Vαβ(<br />

rαβ,<br />

ij ) +<br />

3<br />

N<br />

2ε + 1 4πε<br />

r<br />

i = 1 j > 1 α = 1 β=<br />

1<br />

rf<br />

2 2<br />

α β αβ,<br />

ij<br />

0 cut<strong>of</strong>f<br />

[8.136]<br />

where k is the number <strong>of</strong> sites per molecule, rαβ,ij is the distance between site α <strong>of</strong> molecule i<br />

and site β<strong>of</strong> molecule j. Only pairs i,j <strong>of</strong> molecules for which rij

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