Freedericksz transition

The Fréedericksz transition is a phase transition in liquid crystals produced when a sufficiently strong electric or magnetic field is applied to a liquid crystal in an undistorted state. Below a certain field threshold the director remains undistorted. As the field value is gradually increased from this threshold, the director begins to twist until it's aligned with the field. In this fashion the Fréedericksz transition can occur in three different configurations known as the twist, bend, and splay geometries. The phase transition was first observed by Fréedericksz and Repiewa in 1927. In this first experiment of theirs, one of the walls of the cell was concave so as to produce a variation in thickness along the cell. The phase transition is named in honor of the Russian physicist Vsevolod Frederiks.

If a nematic liquid crystal that is confined between two parallel plates that induce a planar anchoring is placed in a sufficiently high constant electric field then the director will be distorted. If under zero field the director aligns along the x-axis then upon application of an electric field along the y-axis the director will be given by:

Under this arrangement the distortion free energy density becomes:

The total energy per unit volume stored in the distortion and the electric field is given by:

The free energy per unit area is then:

Minimizing this using calculus of variations gives:

Rewriting this in terms of ${\displaystyle \zeta ={\frac {z}{d}}}$ and ${\displaystyle \xi _{d}=d^{-1}{\sqrt {\frac {K_{2}}{\epsilon _{0}\Delta \chi _{e}E^{2}}}}}$ where ${\displaystyle d}$ is the separation distance between the two plates results in the equation simplifying to:

...
Wikipedia