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2.8 Conclusions 81<br />

strain. As A0 is an experimentally determined parameter based on a uniaxial orientation<br />

model whose value should represent the intensity of an absorption band<br />

exclusive of orientation effects, the anomalous increase of the structural absorbance<br />

during elongation-where the sample thickness actually decreases-points towards an<br />

invalidity of the uniaxial syinmetry. T~us, the geometries a and b of Figure 2-52 can<br />

be excluded on the basis that both would lead to a decrease of A" during elongation.<br />

The occurrence of the structural model c at the inversion point of the order<br />

parameter has first been proposed on the basis of small-angle X-ray measurements<br />

by Finkelinann and Kiipfer [117]. Thus, the appearance of four diffraction maxima<br />

have been explained in terms of a biaxial, planar orientation of the mesogens in the<br />

film plane (Figure 2-52c). Depending on the inclination angle of the mesogens with<br />

the stretching direction, such a transition state would lead to an order parameter<br />

close to zero and could also explain the anomalous behavior of the structural<br />

absorbance [36]. In conclusion, it could be shown that, during elongation of the<br />

anisotropic LSCE network, the network structure changes from a uniaxial symmetry<br />

perpendicular to the applied mechanical field (parallel to the orientation induced<br />

in the second crosslinking step) via a planar-biaxial model (inversion of the order<br />

parameter) to a system aligned in the stretching direction of the rheo-optical experiment<br />

[36]. Simultaneously, the originally transparent polymer becomes opaque<br />

at the inversion point of the order parameter and turns transparent again upon<br />

reorientation of the mesogens into the machine direction.<br />

2.8 Conclusions<br />

The aim of this contribution was to demonstrate the potential of FTIR/FTNIR<br />

polarization spectroscopy at variable temperatures for the characterization of segmental<br />

mobility in liquid crystals and liquid-crystalline polymers under the influence<br />

of external fields. Selected examples have been discussed, where either timeresolved<br />

measurements or static experiments have been utilized to monitor the<br />

effects of electric, electroniagnetic, or mechanical perturbations on the liquidcrystalline<br />

system under investigation. For the extremely fast, reversible switching<br />

processes of low-molecular weight liquid crystals and side-chain liquid-crystalline<br />

polymers in electric fields, the novel step-scan FTIR technique has been applied.<br />

The selective character of vibrational spectroscopy generally allowed us to separate<br />

the orientational effects in different functionalities of the liquid-crystalline compound.<br />

Thus, side-chain liquid-crystalline polymers, for example, have been characterized<br />

under the influence of different external fields in terms of the relative<br />

alignment of their main chain, spacer, and mesogenic groups, respectively. Although<br />

the presented data are necessarily limited to selected examples, the variety of<br />

information and its detailed quantitative Character demonstrate, that FTIR/FTNIR<br />

polarization spectroscopy has certainly become an extremely valuable tool lo elucidate<br />

the dynamics of segmental motion in liquid-crystalline systems.

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