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Modern Polymer Spect..

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2.3 Theory<br />

Throughout this chapter the general form of the order parameter S will be used<br />

[3, 3 1 j to describe the long-range orientational order of the investigated liquidcrystalline<br />

materials. In contrast to the theory of Maiei- and Saupe 132, 331, which<br />

considers the uniaxial distribution of the mesogens in a nematic phase relative to the<br />

macroscopic preferential direction (director), this formalism also allows negative<br />

values. The relation of S to the inclination angle 0 of the inesogenic/structural-unit<br />

axis and the reference direction (if not otherwise stated, the external field direction)<br />

is outlined for the case of an SCLCP in Figure 2-3. Also shown are the values of<br />

S for parallel and perpendicular orientation of the mesogens and their isotropic<br />

distribution. The derivation of S, which corresponds to the orientation factor f in<br />

general polynier orientation terminology [14, 17-20], is given in Figure 2-3, where<br />

R is the dichroic ratio determined from the experimental absorbance values measured<br />

with light polarized parallel and perpendicular, respectively, to the chosen<br />

reference direction. Ro is the theoretical dichroic ratio for perfect aligiiinent of the<br />

mesogen, and p is the angle between the transition moment of the absorbing group<br />

and the local chain axis (in the present case the long axis of the mesogenic group)<br />

[14j. The structural absorbance Ao has been chosen as parameter which represents<br />

the intensity of an absorption band exclusive of contributions from the orientation<br />

of the investigated polymer. It is given by [14]:<br />

Both, order parameter S and structural absorbance A0 are based on the assumption<br />

of a uniaxial orientation syniinetry [14, 18-20].<br />

external field<br />

(referencc direction)<br />

s= I<br />

(e =or)<br />

parallel orientation<br />

a<br />

1<br />

S=-- (0=900)<br />

2<br />

perpendicular orientation<br />

s=o<br />

isotropic distribution<br />

Figure 2-3. Geometrical considerations for the<br />

derivation of the order parameter S of a side-chain<br />

liquid-crystalline polymer under the influence of an<br />

exterilal field (ff = inclination angle of the inesogen<br />

with the reference axis, v, = angle between the<br />

transition moment of the absorbing group and the<br />

local chain axis, Rn = theoretical dichroic ratio for<br />

a perfectly aligned structural unit).

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