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Essentials of Computational Chemistry

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294 8 DENSITY FUNCTIONAL THEORY<br />

concluded that the B3LYP functional is particularly robust for predicting geometries in<br />

this area. This is consistent with the good behavior <strong>of</strong> this functional when applied to<br />

minimum-energy structures composed only <strong>of</strong> first-row atoms as already noted above. Cramer<br />

and Barrows (1998) have emphasized, however, that overdelocalization problems can arise<br />

in ionic examples <strong>of</strong> such electrocyclic reactions, and caution may be warranted in these<br />

instances.<br />

8.6.3 Charge Distributions<br />

Over the 108 molecules in Test Set B <strong>of</strong> Table 8.5, Scheiner, Baker, and Andzelm computed<br />

the mean unsigned errors in predicted dipole moments to be 0.23, 0.20, 0.23, 0.19, and<br />

0.16 D at the HF, MP2, SVWN, BPW91, and B3PW91 levels <strong>of</strong> theory, respectively, using<br />

the 6-31G(d,p) basis set. These results were improved somewhat for the DFT levels <strong>of</strong> theory<br />

when more complete basis sets were employed.<br />

Cohen and Tantirungrotechai (1999) compared HF, MP2, BLYP, and B3LYP to one another<br />

with respect to predicting the dipole moments <strong>of</strong> some very small molecules using a very<br />

large basis set, and their results are summarized in Table 8.6. In general the performances <strong>of</strong><br />

MP2, the pure BLYP functional, and the hybrid B3LYP functional are about equal, although<br />

both DFT functionals do very slightly better than MP2 for several cases. HF theory shows<br />

its typical roughly 10–15 percent overestimation <strong>of</strong> dipole moments, and its historically<br />

well-known reversal <strong>of</strong> moment for carbon monoxide.<br />

In addition to the moments <strong>of</strong> the charge distribution, molecular polarizabilities have also<br />

seen a fair degree <strong>of</strong> study comparing DFT to conventional MO methods. While data on<br />

molecular polarizabilities are less widely available, the consensus appears to be that for this<br />

property DFT methods, pure or hybrid, fail to do as well as the MP2 level <strong>of</strong> theory, with<br />

conventional functionals typically showing errors only slightly smaller than those predicted<br />

by HF (usually about 1 a.u.), while the MP2 level has errors only 25 percent as large. In<br />

certain instances, ACM functionals have been more competitive with MP2, but still not quite<br />

as good.<br />

Table 8.6 Dipole moments (D) for eight small molecules at four levels <strong>of</strong><br />

theory using the very large POL basis set a<br />

Molecule HF MP2 BLYP B3LYP Experiment<br />

NH3 1.62 1.52 1.48 1.52 1.47<br />

H2O 1.98 1.85 1.80 1.86 1.85<br />

HF 1.92 1.80 1.75 1.80 1.83<br />

PH3 0.71 0.62 0.59 0.62 0.57<br />

H2S 1.11 1.03 0.97 1.01 0.97<br />

HCl 1.21 1.14 1.08 1.12 1.11<br />

CO −0.25 0.31 0.19 0.10 0.11<br />

SO2 1.99 1.54 1.57 1.67 1.63<br />

a From Cohen and Tantirungrotechai 1999.

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