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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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748 Roland Schmid<br />

Packing density η<br />

minimum maximum<br />

≈ 0 0.4 - 0.6 0.74<br />

perfect gas liquids cubic close packed<br />

These considerations ultimately<br />

<strong>of</strong>fer the basis <strong>of</strong> a genuinely<br />

molecular theory <strong>of</strong> solvent effects,<br />

as compared to a mean-field theory.<br />

Thus, packing and repacking effects<br />

accompanying chemical reactions<br />

have to be taken into account for any<br />

realistic view <strong>of</strong> the solvent’s role<br />

played in chemical reactions to be attained.<br />

The well-known cavity formation<br />

energy is the work done<br />

against intermolecular repulsions.<br />

At present, this energy is calculated<br />

for spherical cavities by the Boublik-Mansoori-Carnahan-Starling-Leland (BMCSL) mixed<br />

HS equation <strong>of</strong> state 45,46<br />

Table 13.1.2. Packing densities in some liquids<br />

Liquid η free volume, %<br />

H2O n-C6 0.41<br />

0.50<br />

59<br />

50<br />

Benzene 0.51 49<br />

MeOH 0.41 59<br />

Et2O 0.47 53<br />

n-C16 0.62 38<br />

( )<br />

3<br />

2<br />

2<br />

ΔGrep<br />

ηd<br />

ηd<br />

ηd<br />

− d + d + 1<br />

3 2<br />

= 2 + 3 + 3<br />

+ ( − 2d + 3d − 1)<br />

ln( 1− η ) [13.1.10]<br />

3<br />

2<br />

RT ( 1−η)<br />

( 1−η)<br />

( 1−<br />

η)<br />

where d = σ σ<br />

0 / is the relative solute size (σ 0 is the solute HS diameter, and σ is the solvent<br />

diameter). Quite recently, a modification <strong>of</strong> this equation has been suggested for high liquid<br />

densities and large solute sizes. 47 Notice that under isochoric conditions the free energy <strong>of</strong><br />

cavity formation is a totally entropic quantity. Ravi et al 48 have carried out an analysis <strong>of</strong> a<br />

model dissociation reaction (Br 2 → 2Br) dissolved in a Lennard-Jones solvent (Ne, Ar, and<br />

Xe). That and the previous work 49 demonstrated that solvent structure contributes significantly<br />

to both chemical reaction volumes (which are defined as the pressure derivatives <strong>of</strong><br />

reaction free energies) and free energies, even in systems containing no electrostatic or dispersion<br />

long-ranged solvent-solute interactions.<br />

Let us now turn to the more difficult case <strong>of</strong> intermolecular attractive forces. These<br />

may be subdivided into:<br />

Long-ranged or unspecific<br />

• dispersion<br />

• induction<br />

• dipole-dipole<br />

• higher multipole<br />

Short-ranged or specific<br />

• electron overlap (charge transfer)<br />

• H-bonding<br />

For the first three ones (dispersion, induction, dipole-dipole forces) adequate calculations<br />

are just around the corner. Let us give some definitions.

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