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Synthesis and Liquid Crystalline Behavior of Random Copolymer of Poly(ethylene oxide) Macromonomer and Liquid Crystalline Monomer by the Photon Transmission Technique
Authors:Sevtap Yildiz  Faruk Yilmaz  Haluk Özbek  Önder Pekcan  Koi˙chi˙ Ito
Institution:1. Istanbul Technical University, Department of Physics , Istanbul , Turkey sevtap@itu.edu.tr;3. Istanbul Technical University, Department of Chemistry , Istanbul , Turkey;4. Gebze Institute of Technology, Department of Chemistry , Gebze , Kocaeli , Turkey;5. Istanbul Technical University, Department of Physics , Istanbul , Turkey;6. Feza Gursey Institute , Istanbul , Turkey;7. I?ik University, Department of Physics , Istanbul , Turkey;8. Department of Materials Science , Toyohashi University of Technology , Toyohashi , Japan;9. 34-1 Kitazawa, Takashi-hongo, Toyohashi , 441-8153 , Japan
Abstract:Random copolymers of poly(ethylene oxide) macromonomer with p‐vinylbenzyl end‐functional group (PEOVB) and liquid crystalline monomer, namely 6‐(4‐cyanobiphenyl‐4′‐oxy)hexyl acrylate (COA), were prepared by conventional free radical polymerization. A living anionic polymerization technique was employed for the synthesis of PEO macromonomers bearing p‐vinylbenzyl moiety at one end. The photon transmission method was also applied to study the phase transitions of COA monomer and its random copolymer with PEO. It was found that, for both samples, the nematic‐smectic A transition is continuous, but the critical fluctuation regions do not allow to obtain 3D XY values. Instead, we have obtained the values close to mean field regime. Scaling of thermal hystersis for random copolymer sample near the nematic‐isotropic transition was studied as well. Thermal hysteresis loops were produced under linearly varying temperature. It was shown that the areas of the hysteresis loops scale with the temperature scanning rate with an exponent being equal to 0.614 which is in good agreement with the field‐theoretical value.
Keywords:PEO macromonomer  liquid crystalline monomer  photon transmission method  nematic and smectic ordering  critical exponent  scaling of thermal hysteresis
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