Abstract
For any nematic liquid crystal having a negative dielectric anisotropy ε α, in a homeotropic texture sandwiched between two parallel plates with a sufficiently large distance L between them, and under a square external electric field excitation E 0(t) = ±E 0 and a static magnetic field H perpendicular to the plates, the applied external voltage V at the threshold of the electrohydrodynamic instability and the square S 2 of the quantity S = qL/π are linear functions of the Fréedericksz transition voltage V F . Here π/L is equal to the wave number of the distortion along the Z‐axis perpendicular to the walls and q is the wave number of distortion along any X‐direction perpendicular to the Z‐axis. S 2 is also a linear function of voltage V. The two lines V F (V F) and V(V F) intersect at a value of voltage V 0 such that V = V F = V 0, which depends only on frequency. With experimental measurements around the point V 0, one may compute the ratio of the elastic constants, K 11/K 33 where K 11 and K 33 are the splay and bend elastic constants, respectively, and by combining the slopes of the two lines S 2(V F) and S 2(V), one may obtain an estimate of the ratio of the dielectric constants ε∥/ε⊥.