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Modern Polymer Spect..

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148 3 ViLwntional <strong>Spect</strong>ra us N Probe of Striictural Order<br />

-<br />

5_1_<br />

L<br />

60-513 5<br />

- 5135-575<br />

575-565<br />

-<br />

-<br />

_v_ -<br />

--<br />

56 5-54<br />

54-526<br />

52 6-50 5<br />

505-49<br />

-49 - 47 1<br />

47.1 - 45.5<br />

43-41<br />

004.-<br />

-<br />

41-39<br />

a,<br />

C<br />

0<br />

__c.<br />

'?<br />

39-36<br />

2 002- 1<br />

n<br />

- ---36-33 1<br />

a<br />

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AT<br />

0.00 t<br />

Figure 3-26. (continued)<br />

dependent Raman and infrared spectra [I 141 it could be concluded that, in the K<br />

phase, most of the decamethylene segments are in the trans-planar conformation<br />

and that upon heating gnuclze rotamers are generated. The identification of what<br />

kind of conformational defects occur in the disordering process when the temperature<br />

increases can only be attempted by the study of the temperature-dependent<br />

spectrum in the traditional CH2 wagging range. We restrict here our analysis to<br />

the temperature-dependent spectra in the usual defect modes range from - 1400 to<br />

- 1300 cm-'. We aim at revealing the conformational evolution through phase<br />

transition of the segments consisting of 10 CH-, groups. Figure 3-27 illustrates the<br />

temperature-dependent infrared spectrum in the CH2 wagging range plotted in

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