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Essentials of Computational Chemistry

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6.5 CASE STUDY: POLYMERIZATION OF 4-SUBSTITUTED AROMATIC ENYNES 199<br />

is the economical MIDI! basis set for which, as noted above, heteroatom d exponents<br />

were specifically optimized so that high-quality geometries and charge distributions (instead<br />

<strong>of</strong> minimal energies) are obtained from the HF wave function. Electrostatic potentials<br />

computed with MIDI! also give good agreement with correlated levels <strong>of</strong> electronic structure<br />

theory.<br />

A more complete discussion <strong>of</strong> charge distributions is deferred until Chapter 9. The performance<br />

<strong>of</strong> HF theory for other molecular properties is also presented in more detail there.<br />

6.5 Case Study: Polymerization <strong>of</strong> 4-Substituted<br />

Aromatic Enynes<br />

Synopsis <strong>of</strong> Ochiai, Tomita, and Endo (2001) ‘Investigation on Radical Polymerization Behavior<br />

<strong>of</strong> 4-Substituted Aromatic Enynes. Experimental, ESR, and <strong>Computational</strong> Studies’.<br />

One strategy for making highly functionalized polymers is first to carry out polymerization<br />

<strong>of</strong> a system bearing functionalizable appendages, and then after polymerization<br />

to react those appendages to introduce new functionality into the polymer. Such an<br />

approach can be advantageous in instances where the monomer that would in principle<br />

lead directly to the functionalized polymer fails itself to be useful as a polymerization<br />

substrate.<br />

Ochiai and co-workers developed an experimental protocol for the radical polymerization<br />

<strong>of</strong> one such reactive monomer, 4-phenylbut-1-en-3-yne. As illustrated in Figure 6.13, this<br />

polymerization creates a polyethylene chain functionalized with phenylethynyl substituents.<br />

A factor that affects the kinetics <strong>of</strong> the polymerization, and, more critically, the utility<br />

<strong>of</strong> the monomer in copolymerizations with other monomers, e.g., methyl methacrylate,<br />

is the stability <strong>of</strong> the radical formed from addition <strong>of</strong> the growing polymer chain to<br />

the vinyl terminus. In order to gauge the stabilizing effect <strong>of</strong> the phenylethynyl group,<br />

and the sensitivity <strong>of</strong> the stabilization to substitution at the para position <strong>of</strong> the aromatic<br />

ring, Ochiai and co-workers carried out calculations at the UHF/3-21G level to evaluate<br />

(i) the spin density in the 1-phenylprop-1-yn-3-yl radical and (ii) the reaction energy for the<br />

process<br />

ž ž<br />

RCH3 + CH3 → RCH2 + CH4<br />

(6.14)<br />

where R was varied over a number <strong>of</strong> different functional groups. This so-called isodesmic<br />

reaction (see Section 10.4.3) essentially computes the C–H bond energy for the substituted<br />

system relative to the C–H bond energy in methane, thereby reducing absolute errors that<br />

would be associated with a small HF calculation for an absolute bond energy.<br />

The spin density calculation, which analyzes the difference between each atom’s Mulliken<br />

population (see Section 9.1.3.2) <strong>of</strong> α and β electrons, indicated the unpaired electron to<br />

be highly delocalized, with populations on the ortho and para carbons <strong>of</strong> the phenyl<br />

ring nearly equal to that found on the formal radical position (these large positive spin<br />

densities were balanced by large negative spin densities on the intervening carbon atoms,<br />

which is a typically observed situation). HF theory tends to overpolarize spin, so the<br />

magnitude <strong>of</strong> the spin polarization is probably not trustworthy, but the large degree <strong>of</strong><br />

delocalization is probably qualitatively reasonable. The prediction that the ring para position<br />

carries substantial spin was found to be consistent with copolymerization reactivity

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