Abstract

In this paper, we consider the long-time behavior of the liquid crystals equations of compressible flow. We prove that if the static state ds minimizes the Ginzburg-Landau approximation energy, then the finite energy weak solutions (ρ, u, d)(t, x) converges to (ρs, 0, ds)(x) with unique density function ρs, which satisfies the conservation of mass.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call