A. Romo-uribe, On the molecular orientation and viscoelastic behaviour of liquid crystalline polymers: the influence of macromolecular architecture, P ROY SOC A, 457(2005), 2001, pp. 207-229
Citations number
39
Categorie Soggetti
Multidisciplinary
Journal title
PROCEEDINGS OF THE ROYAL SOCIETY OF LONDON SERIES A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES
The influence of macromolecular architecture on the Aom-induced orientation
of main-chain thermotropic Liquid crystalline polymers (LCPs) is investiga
ted using in situ wide-angle X-ray scattering. In order to get more insight
into the interrelationship between microscopic and rheological behaviour,
the viscoelastic properties of the nematic melts were also studied. The LCP
s studied are wholly aromatics, composed only of mesogenic units, and semif
lexibles, which consist of mesogenic units separated by alkyl spacers. Rheo
-X-ray scattering evidenced the detrimental influence of the flexible space
rs on the orientation process. The wholly aromatic LCPs readily orient alon
g the how direction, even under modest shear flows (<(<gamma>) over dot> =
0.1 S-1). The semiflexible LCPs, however, display lower levels of orientati
on than the wholly aromatics, and the quality of the orientation worsens as
the length of the flexible spacer increases. The rheological characterizat
ion shows that, like conventional flexible-chain polymers, the thermotropic
LCPs exhibit a linear viscoelastic (LVE) regime. Moreover, dynamic measure
ments, within the LVE regime, suggest a level of elasticity in the nematic
melts. As the length of the alkyl spacer increases, the rheological behavio
ur is more akin to that displayed by common flexible molecular chains. The
poor shear orientation exhibited by the semiflexible LCPs is then associate
d with a molecular network formed by the less-than-rigid molecular chains.
Furthermore, the steady shear viscosity is always smaller than the dynamic
viscosity, i.e. the Cox-Merz rule does not hold. This is due to the fact th
at steady shear induces molecular orientation, whereas oscillatory shear do
es not. The relaxation of orientation after steady shear showed that the mo
lecular orientation relaxes after hundreds of seconds. The sheer stress, ho
wever, relaxes within only a few seconds. Strikingly, the rate of molecular
orientation relaxation was slower for the semiflexible than for the wholly
aromatic LCPs.