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1.5 Appliccitioiis 23<br />

Methylene<br />

Figure 1-20. IR spectra of normal atactic polystyrene and<br />

backbone-deuterated polystyrene films.<br />

I I I I<br />

I 475 14: 5<br />

Wavenumber<br />

hydrogen bonding, is often involved in such blends to overcome the tendency<br />

to phase segregate. In those cases, 2D IR spectroscopy is especially suited for the<br />

investigation of the molecular origin of such specific interactions. One of the wellknown<br />

miscible systems, a blend of atactic polystyrene and poly(viny1 methyl ether)<br />

1191. was investigated using 2D IR to elucidate the molecular origin of the miscibility<br />

of these polymers [52. 531.<br />

Interestingly. polystyrene and poly(viny1 methyl ether) are very different polymers.<br />

Polystyrene is a hard hydrophobic plastic resin. while polyivinyl methyl ether)<br />

is a soft water-soluble polymer. It is quite surprising that such a pair of polymers<br />

could produce a molecularly mixed homogeneous one-phase system. The specific<br />

origin of the miscibility of this polymer pair is not well understood, although some<br />

level of interaction is speculated between the methoxyl groups of poly(viny1 methyl<br />

ether) and the phenyl groups of polystyrene [54].<br />

To simplify the spectral assignment, polystyrene which had been selectively<br />

deuterium substituted to eliminate the backbone contribution (Figure 1-21) was<br />

blended with poly(viny1 methyl ether). Special attention was paid to the symmetric<br />

CHZ-stretching peak of the methoxyl group of the poly(viny1 methyl ether) component<br />

near 2820 cm-'. Figure 1-22 shows the asynchronous 2D IR spectrum of<br />

poly(viny1 methyl ether) in this region. The presence of a pair of asynchronous cross<br />

peaks at the spectral coordinates at 2825 and 2813 cm-' indicates there are two<br />

distinct populations of methoxyl groups belonging to the poly(viny1 methyl ether)<br />

component of this blend, each having a different IR absorption band.<br />

Figure 1-23 shows that the methoxyl band of poly(viny1 methyl ether) at<br />

28 13 cm-' is synchronously correlated with the IR bands located at 3055 cm-' and<br />

3024 cm-' (assigned to the phenyl side groups of the polystyrene component of this<br />

blend). The presence of such synchronous correlation cross peaks strongly suggests<br />

the existence of a specific interaction synchronizing the local motions of the<br />

methoxyl groups of polyivinyl methyl ether) with the polystyrene phenyl groups.

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