TY - JOUR
T1 - Synthesis and liquid crystalline behavior of random copolymer of poly(ethylene oxide) macromonomer and liquid crystalline monomer by the photon transmission technique
AU - Yildiz, Sevtap
AU - Yilmaz, Faruk
AU - Özbek, Haluk
AU - Pekcan, Önder
AU - Ito, Koichi
AU - Yagci, Yusuf
PY - 2005/12
Y1 - 2005/12
N2 - Random copolymers of poly(ethylene oxide) macromonomer with pvinylbenzyl endfunctional group (PEOVB) and liquid crystalline monomer, namely 6(4cyanobiphenyl4′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 pvinylbenzyl 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 nematicsmectic 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 nematicisotropic 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 fieldtheoretical value.
AB - Random copolymers of poly(ethylene oxide) macromonomer with pvinylbenzyl endfunctional group (PEOVB) and liquid crystalline monomer, namely 6(4cyanobiphenyl4′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 pvinylbenzyl 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 nematicsmectic 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 nematicisotropic 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 fieldtheoretical value.
KW - Critical exponent
KW - Liquid crystalline monomer
KW - Nematic and smectic ordering
KW - PEO macromonomer
KW - Photon transmission method
KW - Scaling of thermal hysteresis
UR - http://www.scopus.com/inward/record.url?scp=29144511530&partnerID=8YFLogxK
U2 - 10.1080/10601320500246602
DO - 10.1080/10601320500246602
M3 - Article
AN - SCOPUS:29144511530
SN - 1060-1325
VL - 42 A
SP - 1573
EP - 1588
JO - Journal of Macromolecular Science - Pure and Applied Chemistry
JF - Journal of Macromolecular Science - Pure and Applied Chemistry
IS - 12
ER -