Modern Polymer Spect..
Modern Polymer Spect..
Modern Polymer Spect..
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40 2 Segnwital Mobility of Liquid Crystuls aid Liquidcrystalline Polymevs<br />
6CPe<br />
0<br />
C H 3 - ( C H z ) e C - O D C = N<br />
5<br />
44.5°C 48.5OC<br />
K - N - I<br />
NLCP<br />
- 0<br />
2, H -&-O-(CHZ)~$$C O a C - N<br />
-.<br />
CH2<br />
-n 3S°C 130°C<br />
G - N - I<br />
Figure 2-6. Sti ucture aiid transition temperatures<br />
of the investigated low- aiid highmolecular<br />
weight LC systems I6CPB and<br />
NLCP).<br />
polymers and liquid-crystalline guest-host system) in switch-on/switch-off experiments,<br />
and on the other hand we will describe the structural consequences incurred<br />
by a ferroelectric side-chain polymer in a poled electric field.<br />
Nematic liquid-crystalline molecules, which consist of a rigid inesogenic unit with<br />
an attached flexible part (sequence of methylene units, for example) (Figure 2-6),<br />
are among the most characteristic thermotropic systems. FTIR spectroscopy has<br />
been applied to study the mechanisiii of orientation of the liquid crystals in an<br />
electric field; however, at present the experimental data are not always unequivocal,<br />
and conclusions obtained are not in complete agreement with each other. T~us,<br />
some authors did not detect any differences in orientational rates of the rigid and<br />
the flexible part of the LC molecule [16, 51-54], which is in accordance with the<br />
commonly accepted mechanism of the orientation of an LC as a cooperative<br />
motion of a molecular ensemble [l, 2, 381. Other authors reported, that the motion<br />
of the flexible part precedes that of the inesogen in both orientation and relaxation<br />
[29, 55-57], and some investigators suggested that the motion of the mesogen precedes<br />
the motion of the flexible part [58, 591. With respect to a more detailed exploitation<br />
of the spectroscopic data in terms of the synchronization of the segmental<br />
motions of different functionalities of the investigated liquid-crystalline systems,<br />
2D-correlation analysis [ 16, 30, 60, 611 has proved an extremely valuable tool. In<br />
view of the detailed discussion of this mathematical technique in Chapter 1 of this<br />
book; however, this topic will not be treated here, although several results extracted<br />
from the presented spectroscopic data are based on the application of the 2Dcorrelation<br />
formalism.<br />
2.5.1 Materials<br />
To study the addressed phenomena, a commercial sample of p-cyanophenyl p-nhexylbenzoate<br />
(hereafter abbreviated as 6CPB) (Figure 2-6) was obtained from<br />
Roche (Basel, Switzerland), and used without further purification [53, 541. The<br />
transition temperatures of this LC are also presented in Figure 2-6. It should be<br />
mentioned, that the nematic phase will be retained during cooling down to 7 "C<br />
below the crystal-nematic transition point. To demonstrate the reduction of