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Modern Polymer Spect..

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11 Amorphous Crystalline ,...." I<br />

Figure 1-16. An asynchronous ZD IR<br />

spectrum for the main chain syminetric<br />

CH2-stretching vibration of linear<br />

low-density polyethylene [46].<br />

\ I...."<br />

I I , , 1 1 -2870<br />

2870 2855 2840<br />

Wavenumber, VI<br />

(ca. 3 mole'%,) of deuterium-substituted 1-octene comonomer units. The octene<br />

comonomer is incorporated into the polyethylene chain to produce short (sixcarbon)<br />

side branches. which reduce the melt temperature and crystallinity of the<br />

polymer. By selectively labeling the octene units with deuterium, one can unambiguously<br />

differentiate the dynamics of main chain and short side branches. The<br />

spectral region shown in Figure 1-16 represents IR signals arising exclusively from<br />

the polyethylene chain, with little contribution from the octene side branches.<br />

The presence of asynchronous peaks in the CHZ-stretching vibration of backbone<br />

methylene groups indicates there are two distinct bands in this region of the IR<br />

spectrum of the linear low density polyethylene sample. The band located near<br />

2855 cm-' can be assigned to the contribution from the crystalline phase of the<br />

sample. while the band near 2863 cm-' is due to the amorphous component of this<br />

semicrystalline polymer. The above assignment can be easily verified by heating the<br />

sample above its melt temperature to remove the IR spectral contribution from<br />

the crystalline component of the specimen. Because of the significant difference in<br />

the reorientational responses of polymer chains located in the crystalline and<br />

amorphous phase domains to a given dynamic deformation. 2D IR spectroscopy<br />

can easily differentiate IR bands associated with the two-phase domains, even<br />

though these bands are highly overlapped.<br />

Figure 1-17 shows an asynchronous 2D IR spectrum correlating the backbone of<br />

polyethylene segments located in either crystalline and amorphous domains and<br />

deuterium-substituted branches. Asynchronous cross peaks develop between the<br />

crystalline component of the symmetric CH2-stretching band of the polyethylene<br />

segments and bands for octene side branches. Such asynchronicity suggests short<br />

side branches can move independently of the polyethylene chain located in the<br />

crystalline phase of the sample. No noticeable asynchronicity. however, is observed

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