Volume 39, Issue 3 pp. 286-299
Article

Relaxation behavior of acrylate and methacrylate polymers containing dioxacyclopentane rings in the side chains

Felix García

Felix García

Departamento de Química Orgánica, Universidad de Burgos, 09001 Burgos, Spain

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Abel García-Bernabé

Abel García-Bernabé

Departamento de Termodinámica Aplicada, ETSII, Universidad Politécnica de Valencia, 46022 Valencia, Spain

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Vicente Compañ

Vicente Compañ

Departamento de Ciencias Experimentales, Universitat Jaume I, 12080 Castellón, Spain

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Ricardo Díaz-Calleja

Ricardo Díaz-Calleja

Departamento de Termodinámica Aplicada, ETSII, Universidad Politécnica de Valencia, 46022 Valencia, Spain

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Julio Guzmán

Julio Guzmán

Instituto de Ciencia y Tecnología de Polímeros (CSIC), 28006 Madrid, Spain

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Evaristo Riande

Corresponding Author

Evaristo Riande

Instituto de Ciencia y Tecnología de Polímeros (CSIC), 28006 Madrid, Spain

Instituto de Ciencia y Tecnología de Polímeros (CSIC), 28006 Madrid, SpainSearch for more papers by this author

Abstract

The synthesis of poly[(2,2-dimethyl-1,3-dioxolan-4-yl) methyl acrylate)] (PACGA) and poly[(2,2-dimethyl-1,3-dioxolan-4-yl) methyl methacrylate] (PMCGA) is reported. Both polymers present dielectric and mechanical β subglass absorptions at −128 and −115 °C, respectively, at 1 Hz, followed by ostensible glass–rubber or α relaxations centered in the vicinity of 0 and 67 °C, respectively, at the same frequency. The values of the activation energy of both the mechanical and dielectric β absorptions lie in the vicinity of 10 kcal mol−1. The critical interpretation of the relaxation behavior of PMCGA suggests that dipolar intramolecular correlations play a dominant role in the response of the polymer to an electric field. The subglass relaxations of PACGA and PMCGA are further compared with the relaxation behavior of poly(1,3-dioxane acrylate), poly(1,3-dioxane methacrylate), and other polymers in the glassy state. The strong conductive processes observed in PMCGA at low frequencies and high temperatures were studied under the assumption that that these processes arise from Maxwell–Wagner–Sillars effects occurring in the bulk combined with Nernst–Planckian electrodynamic effects caused by interfacial polarization in the films. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 39: 286–299, 2001

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