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78 2 Segnientril Mobility of Lipid Crystals uizd Licliri~-Cr)istulliiie Polvrwrs<br />

0.07 -<br />

0.06 ..<br />

-<br />

N 005 .*<br />

Figure 2-47. Stress-strain diagram of<br />

0 10 20 30 40 an elongation-recovery cycle of' the<br />

STRAIN I"/]<br />

reference elastomer at 27 "C.<br />

0. 60<br />

S<br />

0. 40<br />

0. 20<br />

Figure 2-48. Order parameter/<br />

strain-plot for the v(C-N)<br />

I .<br />

I I I I I I 1 I absorption corresponding to the<br />

10 20 30 10 ' 40 30 20 10 elongation-recovery cycle shown<br />

STRAIN [Yo] in Figure 2-47.<br />

decrease in sample thickness based on the assumption of a constant sample volume<br />

during elongation [30, 361. A more complex behavior is observed during the elongatioii-recovery<br />

cycle of the LSCE system to a maximum strain of 45% at 27°C.<br />

The corresponding stress-strain curve is shown in Figure 2-49 and has been subdivided<br />

into different strain intervals. The order parameter of the v(C-N) absorption<br />

derived from the spectra acquired during this mechanical treatment is presented<br />

in Figure 2-50. Here too, the analogous strain intervals are indicated to assist<br />

the correlation and interpretation of the mechanical and spectroscopic changes.<br />

Due to the anisotropy of the starting material and the reorientation of the mesogens<br />

during the mechanical treatment, specific assumptions in terms of the reference<br />

direction were necessary. Thus, for the derivation of the order parameter during<br />

elongation between 0 and 32% strain (intervals I and I1 in Figure 2-50), the deformation<br />

direction during the second crosslinking step (which is perpendicular to the<br />

applied deformation in the rheo-optical experiment) has been chosen as polarization<br />

reference direction. Beyond the inversion point of S = 0, the machine direction of<br />

the rheo-optical experiment is applied as polarization reference (interval 111). During<br />

recovery this procedure is reversed. Therefore, the order parameter always has<br />

a positive value throughout the whole experiment. From Figure 2-50 the following<br />

picture can be derived for the orientational changes taking place during the<br />

elongatioii-recovery cycle:

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