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Numerous experimental studies of liquid crystal polymers(LCP)
undergoing shear flow have revealed that they generally adopt a
texture of randomly oriented nematic microdomains separated by
singular structures, known as disclinations in the orientation
field. As a consequence their rheological and optical properties
are largely those of an ordinary isotropic polymer. As was found
by Larson and Mead, under shear, the microstructural and
rheological behavior of LCPs can be very rich with multiple
transitions in texture.
This is quite different from the situation found in small
nematics. When subject to shear flow, small nematics generally
adopt a fixed orientation near the flow direction, and
disclinations are much less common. Their material properties are
generally that of a nematic phase.
A complete understanding of the dynamics of texture evolution and
its interaction with flow is still missing. Several attempts to
analyze these experimental observations have been made via
numerical calculations using the Leslie-Ericksen(LE) theory.
However, the LE theory is accurate only for small shear rates, and
in principle cannot handle disclinations. The Doi theory uses a
much richer order parameter, the orientational distribution
functions. It takes into account the effects of flow, Brownian
dynamics and intermolecular interaction. However, it does not
include the so-called distortional elasticity which is the elastic
penalty for spatial distortions. Therefore the Doi theory is only
valid for spatially homogeneous systems. Indeed the work of Nayak
shows that even though the Doi model leads readily to disclination
and microstructure formation, the simulations eventually break
down since spatial interaction is not properly accounted for.
Marrucci and Greco proposed the incorporation of long-range
distortional elasticity into the Doi model via a generalization of
the Maier-Saupe mean-field potential. Their model was recently
extended into a new constitutive theory for LCP flows. This theory
is a mixture of the macroscopic order parameter description and
the description using orientational distribution function. It is
therefore still desirable to develop a theory that is based solely
on the Doi approach using orientational distribution function.
In our work, we account for the distortional elasticity by
properly taking into account the spatial interactions between the
rod. This allow us to study the long time dynamics of liquid
crystal polymer flow, including domain formation, dynamics of
disclinations between domains, and transition between different
dynamic regimes such as flow aligning, wagging and tumbling.
we also propose a new method to deal with anchoring condition for
Fokker-Planck equation.
1+1 Case
- First "1": dimention of macroscopical flow.
- Second "1": DOF of microcosmic molecular orientation.
Pattern of order parameter $S$ ($C=1, \gamma=5/9, T=400s$)
The disclination first generated in $y\approxeq
0.16, 0.84$, and then propagate to the both sides,
become weaker and weaker, 50s later it meets with
another disclination and get the strongest at
$y\approxeq 0.45, 0,55$
2+1 Case
Under the flow, the orientations of the rods in the whole region
present a polydomain structure. The texture is produced where the
directors abruptly change
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