Optimal boundary control of a simplified Ericksen--Leslie system for nematic liquid crystal flows in
arXiv:1609.03861 · doi:10.1007/s00205-017-1095-2
Abstract
In this paper, we investigate an optimal boundary control problem for a two dimensional simplified Ericksen--Leslie system modelling the incompressible nematic liquid crystal flows. The hydrodynamic system consists of the Navier--Stokes equations for the fluid velocity coupled with a convective Ginzburg--Landau type equation for the averaged molecular orientation. The fluid velocity is assumed to satisfy a no-slip boundary condition, while the molecular orientation is subject to a time-dependent Dirichlet boundary condition that corresponds to the strong anchoring condition for liquid crystals. We first establish the existence of optimal boundary controls. Then we show that the control-to-state operator is Fréchet differentiable between appropriate Banach spaces and derive first-order necessary optimality conditions in terms of a variational inequality involving the adjoint state variables.
References in corpus (8)
- Regularity and existence of global solutions to the Ericksen-Leslie system in
- Energy Dissipation and Regularity for a Coupled Navier-Stokes and Q-Tensor System
- On the General Ericksen-Leslie System: Parodi's Relation, Well-posedness and Stability
- Well-posedness of the Ericksen-Leslie system
- Global strong solutions of the full Navier-Stokes and -tensor system for nematic liquid crystal flows in : existence and long-time behavior
- On a 3D isothermal model for nematic liquid crystals accounting for stretching terms
- Optimal distributed control of a nonlocal Cahn-Hilliard/Navier-Stokes system in 2D
- Regularity of Solutions to the Liquid Crystals Systems in and