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Structure,equilibrium and viscoelastic mechanical behaviour of polyurethane networks based on triisocyanate and poly(oxypropylene)diols
Institution:1. Department of Chemistry and Biochemistry, Texas Christian University, Fort Worth, TX, USA;2. Department of Chemistry and Biochemistry, The University of Texas at Arlington, Arlington, TX, USA;1. IPREM, Équipe de Physique et Chimie des Polymères, CNRS UMR 5254, Université de Pau et des Pays de l’Adour, Hélioparc, 2 Avenue du Président Angot, 64053, Pau, France;2. Univ. Bordeaux, IMS, CNRS UMR 5218, F-33400, Talence, France;3. Aix Marseille Univ, CNRS, Institut de Chimie Radicalaire ICR, UMR 7273, F-13397, Marseille, France;4. Laboratoire Ondes et Matière d''Aquitaine LOMA, Université Bordeaux, CNRS, UMR 5798, 33405, Talence, France;1. Laboratoire de Physico-Chimie des Matériaux et des Electrolytes pour l’Energie (PCM2E), EA 6299, Avenue Monge Faculté des Sciences, Parc de Grandmont, 37200 Tours, France;2. Synthèse et Isolement de Molécules BioActives (SIMBA), EA 7502 Laboratoire de Chimie Physique, Faculté de Pharmacie 31, avenue Monge, 37200 Tours, France;3. Université de Sfax, Institue Supérieure de Biotechnologie de Sfax, Laboratoire de Chimie Médicinale et Environnementale, 3018 Sfax, Tunisia
Abstract:Using the theory of branching processes, the detailed structure of polyurethane networks from poly(oxypropylene)diols (PPDs), monofunctional alcohol (cyclohexanol) and triisocyanate prepared at various initial ratios of the reactive groups rHDOH]PPD/NCO] = 0·5−1·7 was characterized in terms of the number, size and structure of elastically active network chains (EANCs), backbone and dangling chains. From an analysis of the dependence of the critical molar ratio at gelation rHDc on dilution it follows that PPD samples are composed of molecules bearing primary and secondary hydroxy groups. The branching theory, in which the presence of both primary and secondary hydroxy groups in PPDs is accounted for, adequately describes the dependence of the mass fraction of the sol ws on rHD when no side reactions occur in the system (networks in the range rHD ≥ 1 or networks with monofunctional alcohols). The equilibrium photoelastic behaviour can be described by the junction-fluctuation theory with front factor A = 1 without entanglement contribution. The frequency-temperature superposition can be performed for all networks; the temperature dependence of the horizontal shift factor satisfies the WLF equation. While the position of the main transition region of viscoelastic functions on temperature or frequency depends on the content of the polar triisocyanate component, the shape of these functions at the end of the transition is determined predominantly by the concentration of EANCs.
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