MS, Kent State University, 2019, College of Arts and Sciences / Department of Mathematical Sciences
The study presented here utilizes analytical and numerical methods to explore magnetic field induced Fr&eecute;edericksz transitions in a homeotropic cholesteric liquid crystal film with negative magnetic anisotropy. The director field is assumed to vary only across the gap thickness. The Oseen-Frank bulk energy and Rapini-Papoular surface energy are sought to model the equilibrium configurations of the director field, which is a compromise among torques from boundary anchoring, material elasticity, and magnetic field. In the strong anchoring case, the director field is uniform if the gap distance is sufficiently small in the absence of the field. As the magnetic field strength increases, a first-order transition to a distorted configuration occurs if the intrinsic pitch is small, and a second-order transition occurs if the intrinsic pitch is large. As the anchoring strength on the boundary weakens, the critical field strength for a distorted configuration shifts to a lower value, and a second-order transition becomes first-order. As the field strength further increases, there is a second transition to a simple twist configuration. Detailed analyses near the bifurcation points were conducted to gain insight into finding the globally stable solution. The full numerical bifurcation
diagrams contain both first- and second-order transitions for both the strong and weak anchoring. We discover that there are certain attributes that can be varied to arrive at similar evolutions in transitions for the strong and weak boundary anchoring systems.
Committee: Xiaoyu Zheng PhD (Advisor); Ulrike Vorhauer PhD (Committee Member); Eugene C. Gartland Jr./PhD (Committee Member)
Subjects: Applied Mathematics