Pt. Mather et al., Morphological and rheological responses to shear start-up and flow reversal of thermotropic liquid-crystalline polymers, MACROMOLEC, 33(20), 2000, pp. 7594-7608
Novel rheo-optical methods have been used to directly observe morphology ev
olution, during shear start-up and reversal flow, in semiflexible main-chai
n thermotropic liquid-crystalline polymers (TLCPs). Using a specially desig
ned microrheometer allowing for simultaneous transient optical and mechanic
al observations, we observed band formation upon reversal of flow direction
. It was seen that this band formation causes asymmetric light diffraction
in H-V small-angle light scattering mode, indicating a tilted arrangement o
f the regularly spaced bands. Also conducted were shear start-up and flow r
eversal experiments using a cone-and-plate rheometer under the same thermal
and deformation histories as those in rheo-optical experiments for polymer
s of differing spacer lengths at equal temperature difference below the nem
atic-to-isotropic transition temperature (T-NI) It was observed that, durin
g both shear startup and flow reversal, the first normal stress difference
N-1(+)(gamma, t) exhibits a large overshoot followed by an oscillatory deca
y, while shear stress o(+)(gamma, t) exhibits a large overshoot followed by
a monotonic decay. It was found that the higher the applied shear rate, th
e larger the overshoot of N-1(+)(gamma, t) and sigma(+)(gamma, t), and the
longer the persistence of oscillations in N-1(+)(gamma, t). Similarity was
found between the ratio N-1(+)(gamma, t)/ sigma(+)(gamma, t) and flow biref
ringence Delta n(+)(gamma, t) during shear start-up and flow reversal of th
e TLCPs investigated in this study. Further, we found that the ratio sigma(
+)(t, gamma)/sigma scales with gamma t but the ratio N-1(+)(gamma, t) /N-1
does not, where sigma denotes shear stress at steady state and N-1 denotes
first normal stress difference at steady state.