2015
DOI: 10.1016/j.na.2014.09.011
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Weak solutions for an initial–boundary Q-tensor problem related to liquid crystals

Abstract: The coupled Navier-Stokes and Q-Tensor system is considered in a bounded three-dimensional domain under homogeneous Dirichlet boundary conditions for the velocity u and either nonhomogeneous Dirichlet or homogeneous Neumann boundary conditions for the tensor Q.The corresponding initial-value problem in the whole space R 3 was analyzed in [Paicu & Zarnescu, 2012].In this paper, three main results concerning weak solutions will be proved; the existence of global in time weak solutions (bounded up to infinite tim… Show more

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Cited by 37 publications
(64 citation statements)
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“…Asymptotic behavior of the Cauchy problem in R 3 with ξ = 0 is recently discussed in [10]. Besides, initial boundary value problems subject to various boundary conditions for d = 2, 3 have been investigated by several authors in [2,16,17] under the assumption ξ = 0. In these works, they proved the existence of global weak solutions, the existence and uniqueness of local strong solutions, as well as some regularity criteria, etc.…”
Section: T) = U(x T) Q(x + E I T) = Q(x T) For (X T) ∈mentioning
confidence: 99%
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“…Asymptotic behavior of the Cauchy problem in R 3 with ξ = 0 is recently discussed in [10]. Besides, initial boundary value problems subject to various boundary conditions for d = 2, 3 have been investigated by several authors in [2,16,17] under the assumption ξ = 0. In these works, they proved the existence of global weak solutions, the existence and uniqueness of local strong solutions, as well as some regularity criteria, etc.…”
Section: T) = U(x T) Q(x + E I T) = Q(x T) For (X T) ∈mentioning
confidence: 99%
“…The main difficulty in handling the current full coupled system with ξ ∈ R is due to the fact that for ξ = 0 the system (1.1)-(1.5) no longer enjoys certain maximum principle for the Q-equation (1.3), which is instead true in the case in which ξ = 0 (see, e.g., [17,Theorem 3]). Due to the loss of control on Q in L ∞ (0, T ; L ∞ ), extra difficulties arise in obtaining estimates for those highly nonlinear terms of the system (see Proposition 12).…”
Section: T) = U(x T) Q(x + E I T) = Q(x T) For (X T) ∈mentioning
confidence: 99%
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“…The existence of weak solutions and a uniqueness criteria have been already studied (see [11] for a Cauchy problem in the whole R 3 and [7] for a initial-boundary problem in a bounded domain Ω).…”
Section: Introductionmentioning
confidence: 99%
“…The existence of weak solutions and a uniqueness criteria have been already studied (see [11] for a Cauchy problem in the whole R 3 and [7] for a initial-boundary problem in a bounded domain Ω).Nevertheless, results on strong regularity have only been treated in [11] for a Cauchy problem in the whole R 3 .In this paper, imposing Dirichlet or Neumann boundary conditions, we show the existence and uniqueness of a local in time weak solution with weak regularity for the time derivative of the velocity and the tensor variables (u, Q). Moreover, we gives a regularity criteria implying that this solution is global in time.…”
mentioning
confidence: 99%