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Modern Polymer Spect..

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I I D W l<br />

0 : 2n 4n<br />

+ p H- Phase Angle<br />

0 2n 4n<br />

Figure 1-4. A small-amplitude sinusoidal<br />

strain applied to a sample and resulting<br />

dynamic IR dichroism I DIRLDI response<br />

induced by the strain. The two siiiusoidal<br />

signals are not always in phase with each<br />

other.<br />

-<br />

c<br />

n<br />

L<br />

m<br />

58msec<br />

Figure 1-5. A time-resolved<br />

dynamic IR dichroism<br />

(DIRLD I spectrum of an<br />

atactic polystyrene film under<br />

a small-amplitude (ca. 0. I'X))<br />

sinusoidal (23-Hzl dynamic<br />

strain at room temperature.<br />

the rate-dependent nature of the reorientation processes of various submolecular<br />

constituents.<br />

The advantage of using IR spectroscopy in dynamic studies of polymers is that<br />

such a measurement can be used to examine individual submolecular constituents<br />

or chemical functional groups by simply changing the wavelength of the IR probe.<br />

The variation of IR dichroism, depicted as a simple sinusoidal signal in Figure 1-4.<br />

can actually be measured as a function of not only time but also IR wavenumber.<br />

In other words, dynamic IR dichroism is obtained as a time-resolved spectrum<br />

representing the molecular level response of polymers, as shown in Figure 1-5.<br />

For a given sinusoidal dynamic strain i(t) with a small amplitude i and fre-

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