2013
DOI: 10.1103/physreve.88.012505
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Oscillatory motion of sheared nanorods beyond the nematic phase

Abstract: We study the role of the control parameter triggering nematic order (temperature or concentration) on the dynamical behavior of a system of nanorods under shear. Our study is based on a set of mesoscopic equations of motion for the components of the tensorial orientational order parameter. We investigate these equations via a systematic bifurcation analysis based on a numerical continuation technique, focusing on spatially homogeneous states. Exploring a wide range of parameters we find, unexpectedly, that sta… Show more

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Cited by 12 publications
(53 citation statements)
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“…Finally, we notice the small "islands" of KT regions within the T state (A-species) or W-state (B-species). This indicates a bi-stability of the solutions which may be interpreted as a coexistence of in-shear-plane and out-of-shear plane oscillations (as already mentioned in [34]). At this point, it would be very interesting to extend the present analysis to spatially inhomogeneous systems: Indeed, as previously shown for a one-component system [37,71], bistability in the homogeneous system can translate to spatially separated dynamical coexistence of different states, when one allows for inhomogeneity.…”
Section: Numerical Resultssupporting
confidence: 62%
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“…Finally, we notice the small "islands" of KT regions within the T state (A-species) or W-state (B-species). This indicates a bi-stability of the solutions which may be interpreted as a coexistence of in-shear-plane and out-of-shear plane oscillations (as already mentioned in [34]). At this point, it would be very interesting to extend the present analysis to spatially inhomogeneous systems: Indeed, as previously shown for a one-component system [37,71], bistability in the homogeneous system can translate to spatially separated dynamical coexistence of different states, when one allows for inhomogeneity.…”
Section: Numerical Resultssupporting
confidence: 62%
“…The simplest one is a (supercritical) Hopf bifurcation occurring at the boundary between alignment (A) and wagging (W). In [34] we have presented a complete continuation analysis revealing the complexity of the dynamical behavior already in the one-component case (where one has already five dynamical variables). Performing such an analysis for the mixture would have been beyond the scope for the present paper.…”
Section: Numerical Resultsmentioning
confidence: 99%
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“…The Pyragas scheme has been applied to a broad variety of non-linear systems from various fields (see [30,31] for overviews) including semiconductor nanostructures, lasers, neural systems and general reaction-diffusion systems [32,33]. There are also recent applications to the flow of soft-matter systems, both from the experimental [34] and from the theoretical side [35], an example being the stabilization of steady shear-aligned states in sheared liquid crystals [36]. Within the present study, we focus on a non-diagonal control scheme which targets the average total stress or shear rate, respectively, yielding a Pyragas term involving only the viscoelastic stress.…”
Section: Introductionmentioning
confidence: 99%