2018
DOI: 10.1007/s00205-018-1321-6
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Twisted Solutions to a Simplified Ericksen–Leslie Equation

Abstract: In this article we construct global solutions to a simplified Ericksen-Leslie system on R 3 . The constructed solutions are twisted and periodic along the x3-axis with period d " 2π L µ. Here µ ą 0 is the twist rate. d is the distance between two planes which are parallel to the x1x2 -plane. Liquid crystal material is placed in the region enclosed by these two planes. Given a well-prepared initial data, our solutions exist classically for all t P r0, 8q. However these solutions become singular at all points on… Show more

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Cited by 3 publications
(2 citation statements)
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“…Based on the finite time singularities of the 2D heat flow of harmonic maps [6], solutions of (1.1)-(1.4) with finite time singularities have been recently constructed in [18], where the spatial domain is a bounded open set in R 3 . The long time behavior of solutions of (1.1)-(1.4) is concerned in [9,10]. The behavior of defects is also an important subject in the study of liquid crystals.…”
Section: Introductionmentioning
confidence: 99%
“…Based on the finite time singularities of the 2D heat flow of harmonic maps [6], solutions of (1.1)-(1.4) with finite time singularities have been recently constructed in [18], where the spatial domain is a bounded open set in R 3 . The long time behavior of solutions of (1.1)-(1.4) is concerned in [9,10]. The behavior of defects is also an important subject in the study of liquid crystals.…”
Section: Introductionmentioning
confidence: 99%
“…Nevertheless, it should be pointed out that important progresses have been achieved for the original Ericksen-Leslie model (as well as its simplified versions), in which the penalisation energy density W (d) is removed and instead, a Lagrangian multiplier corresponding to the unitary constraint |d(t, x)| = 1 has to be introduced in the director equation. For instance, we refer the interested readers to [7,23,24,27,29,33,39,44,49] for the simplified liquid crystal system involving the transported heat flow of harmonic map, to [21,26,32,45] for the general Ericksen-Leslie system as well as its non-isothermal extension [12], and to [2,28] for the case with inertial term in the director equation (i.e., the so-called hyperbolic Ericksen-Leslie system).…”
Section: Introductionmentioning
confidence: 99%