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Artículo

Polymer-Dispersed Liquid Crystals with Co-continuous Structures Generated by Polymerization-Induced Phase Separation of EBBA-Epoxy Solutions

Hoppe, Cristina ElenaIcon ; Galante, Maria JoseIcon ; Oyanguren, Patricia AngelicaIcon ; Williams, Roberto Juan JoseIcon
Fecha de publicación: 07/2002
Editorial: American Chemical Society
Revista: Macromolecules
ISSN: 0024-9297
Idioma: Inglés
Tipo de recurso: Artículo publicado
Clasificación temática:
Físico-Química, Ciencia de los Polímeros, Electroquímica; Ingeniería de los Materiales

Resumen

Polymer-dispersed liquid crystals (PDLCs), consisting of a dispersion of LC-rich domains in a polymer matrix, are used in different types of electrooptical devices. Their efficiency can in principle be increased if the LC domains exhibit a uniform characteristic size in the range of the wavelength of visible light. In an attempt to generate this type of morphology, a model PDLC system based on a 50 wt % solution of N-4-ethoxybenzylidene-4‘-n-butylaniline (EBBA) in an epoxy monomer (diglycidyl ether of bisphenol A, DGEBA) was analyzed. The polymerization-induced phase separation was performed at 80 °C, using a tertiary amine as initiator (benzyldimethylamine, BDMA). By selecting an initial concentration located close to the critical composition to promote spinodal demixing, co-continuous morphologies were obtained, which were rapidly fixed by gelation. The conversion of epoxy groups (p) was followed by near-infrared spectroscopy (NIR). At p = 0.28, phase separation took place as revealed by transmission optical microscopy (TOM) and by the acceleration observed in the isothermal cure rate. Gelation took place at p = 0.35, soon after the cloud point. Although the primary structure was arrested by gelation, the LC-rich phase was continuously enriched in pure EBBA, as revealed by the increase in TNI with conversion monitored by differential scanning calorimetry (DSC). Co-continuous structures remained unmodified after the storage of PDLCs for several months. The nematic range of the LC-rich phase at p = 1 was comprised between 34 °C (melting point) and TNI = 68 °C. A 57% of the initial LC was present in nematic domains at 40 °C, as determined by the variation of the FTIR absorbance of a characteristic LC peak between isotropic and nematic states. Therefore, a possible route to obtain PDLCs with a uniform characteristic size of LC domains is to start with a composition close to the critical one and select conditions to produce liquid−liquid demixing soon before gelation.
Palabras clave: Pdlc , Epoxy , Polymerization Induced Phase Separation
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info:eu-repo/semantics/openAccess Excepto donde se diga explícitamente, este item se publica bajo la siguiente descripción: Creative Commons Attribution-NonCommercial-ShareAlike 2.5 Unported (CC BY-NC-SA 2.5)
Identificadores
URI: http://hdl.handle.net/11336/78219
URL: https://pubs.acs.org/doi/abs/10.1021/ma0200120
DOI: http://dx.doi.org/10.1021/ma0200120
Colecciones
Articulos(INTEMA)
Articulos de INST.DE INV.EN CIENCIA Y TECNOL.MATERIALES (I)
Citación
Hoppe, Cristina Elena; Galante, Maria Jose; Oyanguren, Patricia Angelica; Williams, Roberto Juan Jose; Polymer-Dispersed Liquid Crystals with Co-continuous Structures Generated by Polymerization-Induced Phase Separation of EBBA-Epoxy Solutions; American Chemical Society; Macromolecules; 35; 16; 7-2002; 6324-6331
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