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Global existence of weak solutions of the nematic liquid crystal flow in dimensions three

Abstract

For any bounded smooth domain Ξ©βŠ‚R3\Omega\subset\mathbb R^3, we establish the global existence of a weak solution u:Ω×(0,+∞)β†’R3Γ—S2u:\Omega\times (0,+\infty)\to\mathbb R^3\times\mathbb S^2 of the initial-boundary value (or the Cauchy) problem of the simplified Ericksen-Leslie system (1.1) modeling the hydrodynamic flow of nematic liquid crystals for any initial and boundary (or Cauchy) data (u0.d0)∈HΓ—H1(Ξ©,S2(u_0. d_0)\in {\bf H}\times H^1(\Omega,\mathbb S^2), with d0(Ξ©)βŠ‚S+2d_0(\Omega)\subset\mathbb S^2_+ (the upper hemisphere). Furthermore, (u,du,d) satisfies the global energy inequality (1.4).Comment: 24 page

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