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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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

The decomposition <strong>of</strong> the interaction energy through a variational<br />

approach: a summary<br />

We have so far given a description <strong>of</strong> the elements in which ΔEAB(R) may be decomposed<br />

using variational approaches. We report here the final expression:<br />

ΔE AB = ES + PL + EX + CT + COUP + DIS<br />

[8.22]<br />

At the HF level, all terms (but one: DIS) can be obtained with almost zero computational<br />

cost with respect to the numerical determination <strong>of</strong> ΔE AB; in the HF decomposition <strong>of</strong><br />

the interaction energy there is a small additional term (called COUP) describing further couplings<br />

between the other components, which is <strong>of</strong>ten left as it is obtained (i.e., as the difference<br />

between the original ΔE AB value and the sum <strong>of</strong> the other four components) or<br />

subjected to further decompositions.<br />

8 The last term, DIS, may be<br />

calculated at this level using<br />

specialistic time-dependent formulations<br />

<strong>of</strong> the HF procedure.<br />

Going beyond the HF level, the<br />

decomposition can be obtained at<br />

the MP2 level essentially using<br />

the same techniques (DIS may be<br />

appreciated by separating some <strong>of</strong><br />

the MP2 contributions that are<br />

strictly additive).<br />

The variational approaches<br />

we have considered are able to describe,<br />

and to decompose, the interaction<br />

energy at the level <strong>of</strong><br />

Figure 8.3. Decomposition <strong>of</strong> the interaction energy ΔE in<br />

H 2O�HOH.<br />

accuracy one wishes, once the<br />

necessary computational resources<br />

are available. In fact, as<br />

we shall see later, there is no need<br />

<strong>of</strong> reaching extreme precision in the preliminary calculations to model interaction potentials<br />

for liquids, because other approximations must be introduced that will drastically reduce the<br />

accuracy <strong>of</strong> the description.<br />

We report in Figure 8.3 as an example the decomposition <strong>of</strong> the interaction energy <strong>of</strong><br />

the water dimer, in the same orientation Ω used in Figure 8.1.<br />

At large distances the interaction is dominated by ES; this contribution also gives a<br />

reasonable approximation to ΔE at the equilibrium distance. The IND decays with the distance<br />

more rapidly than ES; this contribution is particularly sensitive to the quality <strong>of</strong> the<br />

expansion basis set {χ}. Old calculations <strong>of</strong> IND using restricted basis sets are not reliable.<br />

EX is a short ranged term: its contribution is however essential to fix the position <strong>of</strong> the minimum<br />

(and to describe portion III <strong>of</strong> the PES). CT and DIS terms have both a short-range<br />

character.<br />

This schematic analysis is valid for almost all the dimeric interactions where at least<br />

one partner has a dipolar character. The presence <strong>of</strong> a hydrogen bond (as is the case for the

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