Abstract
One of the most fascinating aspects of liquid crystals is the Fredericks transition, which can occur when a finite sample of nematic liquid crystal is subjected to an externally applied magnetic or electric field. It is well-known that the director orientation throughout a sample of liquid crystal may be affected by a sufficiently strong magnetic or electric field. More specifically, the director alignment throughout a thin sample of nematic liquid crystal will not be influenced by the external magnetic or electric field when its magnitude is less than the critical field strength or Fredericks threshold, but will be influenced by the external field and start to adjust its orientation whenever the magnitude of the field is above the critical field strength. This change in the director alignment after the magnitude of the field increases beyond the critical field strength is called the Fredericks transition. It is exactly this important aspect of liquid crystals that provides many applications of liquid crystals for displays.
In this chapter we first review the classical Fredericks transition in a liquid crystal layer where analytical solutions can be obtained. After this warm-up, we provide a detailed analysis in modeling electrically induced Fredericks transition. We conclude the chapter with some future perspectives.
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Acknowledgment and Disclaimer
Hong Zhou would like to thank the Office of Naval Research (ONR) for supporting this work. The views expressed in this document are those of the authors and do not reflect the official policy or position of the Department of Defense or the U.S. Government.
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Zhou, H., Choate, E.P., Wang, H. (2015). Optical Fredericks Transition in a Nematic Liquid Crystal Layer. In: Thakur, V., Kessler, M. (eds) Liquid Crystalline Polymers. Springer, Cham. https://doi.org/10.1007/978-3-319-20270-9_11
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DOI: https://doi.org/10.1007/978-3-319-20270-9_11
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