On well-posedness of Ericksen-Leslie's paraboloc-hyperbolic liquid crystal model
arXiv:1612.04616 · doi:10.1137/18M1167310
Abstract
We establish the following well-posedness results on Ericksen-Leslie's parabolic-hyperbolic liquid crystal model: 1, if the dissipation coefficients β= μ_4 - 4 μ_6 > 0, and the size of the initial energy E^{in} is small enough, then the life span of the solution is at least -O(\ln E^{in}); 2, for the special case that the coefficients μ_1 = μ_2 = μ_3 = μ_5 = μ_6 = 0, for which the model is the Navier-Stokes equations coupled with the wave map from \mathbb{R}^n to \mathbb{S}^2, the same existence result holds but without the smallness restriction on the size of the initial data; 3, with further constraints on the coefficients, namely α= μ_4 - 4 μ_6 - \tfrac{ (|λ_1| - 7 λ_2)^2 }η - \tfrac{ 2 ( 7 |λ_1| - 2λ_2 )^2 }{ |λ_1| } > 0 and μ_2 < μ_3, the global classical solution with small initial data can be established. A relation between the Lagrangian multiplier and the geometric constraint |d|=1 plays a key role in the proof.
34 pages. arXiv admin note: text overlap with arXiv:1105.2180 by other authors
Cited by in corpus (9)
- Small data global regularity for 3-D Ericksen-Leslie's hyperbolic liquid crystal model without kinematic transport
- Global Well-posedness for the Three Dimensional Simplified Inertial Ericksen-Leslie Systems Near Equilibrium
- Poiseuille flow of nematic liquid crystals via the full Ericksen-Leslie model
- The zero inertia limit of Ericksen-Leslie's model for liquid crystals
- Small data global regularity for simplified 3-D Ericksen-Leslie's compressible hyperbolic liquid crystal model
- Entropy inequality and energy dissipation of inertial Qian-Sheng model for nematic liquid crystals
- Incompressible limit of the Ericksen-Leslie hyperbolic liquid crystal model in compressible flow
- Uniqueness of weak solutions for the general Ericksen-Leslie system with Ginzburg-Landau penalization in T^2
- On a Reversible Gray-Scott Type System from Energetic Variational Approach and Its Irreversible Limit