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-<br />

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-2950<br />

'<br />

E, Figure<br />

- ><br />

1-14. A synchronous 2D IR<br />

spectrum of a thin film of atactic<br />

polystyrene in the CH-stretching vibration<br />

region at room temperature.<br />

Regular one-dimensional spectra of<br />

the same system are provided at the<br />

top and left of the 2D spectrum for<br />

, I I l I I I I I 315" reference. Shaded areas represent<br />

I50 2950 2750<br />

Wavenumber. VI<br />

negative correlation intensity.<br />

1.5.1 Amorphous <strong>Polymer</strong>s<br />

A homogeneous one-phase system consisting of a single. noncrystallizing homopolymer,<br />

such as atactic polystyrene [3, 38-41 ] or poly(methy1 methacrylate) [42-<br />

441, provides one of the least complicated testing grounds for the applicability of<br />

the 2D IR technique for the study of local dynamics of polymers. By using 2D IR,<br />

surprisingly rich information can be extracted even from a simple polymeric system<br />

[25, 39-41 1. Figure 1-14 shows a contour-map representation of the synchronous<br />

2D IR correlation spectrum of an atactic polystyrene film in the CH-stretching<br />

region. A three-dimensional fish-net plot of the same 2D IR spectrum corresponding<br />

to Figure 1-14 has already been shown in Figure 1-1.<br />

DIRLD data used for the 2D correlation analysis was obtained by applying a<br />

23-Hz dynamic strain with an amplitude of 0.1% to a thin solution-cast film of atactic<br />

polystyrene (MI, 150,000) at room temperature 1391. The resulting dynamic dichroism<br />

spectra have already been shown in Figures 1-5 and 1-6. The time-dependent<br />

reorientations of transition dipoles associated with the molecular vibrations of<br />

backbone and side groups are all observable in the original dynamic dichroism<br />

spectra. However, much more detailed features are recognized in the 2D correlation<br />

spectrum.<br />

Autopeaks at the diagonal positions of Figure 1-14 represent transition dipoles<br />

that are susceptible to reorientational motions in the polystyrene sample. Peaks at<br />

2855 cm-I and 2925 cm-l are, respectively, assignable to the symmetric and antisymmetric<br />

CH2-stretching vibrations of the methylene groups in the backbone of<br />

the polystyrene chain; those peaks above 3000 cm-' arise from the phenyl ring CHstretching<br />

vibrations and indicate the reorientation of the side groups. The appearance<br />

of positive synchronous cross peaks at spectral coordinates corresponding to<br />

the two methylene bands indicates the transition dipoles associated with these two

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