全部 标题 作者
关键词 摘要

OALib Journal期刊
ISSN: 2333-9721
费用:99美元

查看量下载量

相关文章

更多...

A Study of the Deformation, Network, and Aging of Polyethylene Oxide Films by Infrared Spectroscopy and Calorimetric Measurements

DOI: 10.1155/2012/432046

Full-Text   Cite this paper   Add to My Lib

Abstract:

The calorimetric and infrared (IR) spectroscopy measurements of polyethylene oxide (PEO) are used to evaluate the deformation and relaxation that films experience during a temperature cycle (30°C–90°C–30°C). After melting, the intensity of some bands decreases by 10 to 70%. During the temperature cycle, the C–O band in the 1100?cm?1 region and the C–C–O deformation bands at 650 and 500?cm?1 show some new features. A network of cooperative oxygen-hydrogen interactions between the PEO chains form in films with special history, namely, in thermally treated films, in thin films prepared from gel forming solutions, and in thick films after aging. The interchain interaction network is suggested from the IR absorption bands in the 1200 and 900?cm?1 region and also from small bands at 1144 and 956?cm?1. The network seems absent or reduced in thin films. IR spectroscopy appears a sensitive technique to study chain conformations in PEO films and in other materials where order, disorder, and the formation of intermolecular interactions coexist. 1. Introduction The physico-chemical properties of pure polyethylenoxide (PEO) such as crystallinity [1–3], thermal properties [2, 3], and morphology [4, 5] have been investigated. The polar and nonpolar parts of the PEO sequence give rise to a wide range of properties unknown to polyolefins. An intriguing property of PEO in dilute and very dilute solutions is the formation of stable clusters [6, 7]. Nonequilibrium effects related to the polymer-solvent interactions have been studied [8]. Associations have been investigated by several techniques in order to understand the thermodynamics of their origin and obtain some insight into protein-water interactions [9]. The effect of shear on solutions and resulting degradation has been analysed [10]. The vibrational spectra of oriented PEO films have been measured [11, 12] and the positions of the bands were compared to those calculated. Structural models and comparison with the IR spectra of small molecules have suggested the assignments of the bands between 3000 and 400?cm?1 observed for the solid and for the melt. Ionic conductivity, effect of surface on conformations, and crystallinity have been investigated in PEO systems in fundamental and applied FTIR studies [13–16]. FTIR spectroscopy is used to study the specific interactions between the PEO chains and small molecules [13]. Chain-chain interactions in composites and chain-ion interactions leave a trace on the vibrational spectrum. They increase the parallel portion of the vibrations at the expanse of the perpendicular

References

[1]  P. Lightfoot, M. A. Mehta, and P. G. Bruce, “Crystal structure of the polymer electrolyte poly(ethylene oxide)3:LiCF3SO3,” Science, vol. 262, no. 5135, pp. 883–885, 1993.
[2]  B. Wunderlich, Macromolecular Physics, vol. 3, Academic Press, London, UK, 1980.
[3]  G. Strobl, The Physics of Polymers, Springer, Berlin, Germany, 1997.
[4]  J. M. Schultz and M. J. Miles, “AFM study of morphological development during the melt-crystallization of poly(ethylene oxide),” Journal of Polymer Science B, vol. 36, no. 13, pp. 2311–2325, 1998.
[5]  K. Dalnoki-Veress, J. A. Forrest, M. V. Massa, A. Pratt, and A. Williams, “Crystal growth rate in ultrathin films of poly(ethylene oxide),” Journal of Polymer Science B, vol. 39, no. 21, pp. 2615–2621, 2001.
[6]  M. Polverari and T. G. M. Van De Ven, “Dilute aqueous poly(ethylene oxide) solutions: clusters and single molecules in thermodynamic equilibrium,” Journal of Physical Chemistry, vol. 100, no. 32, pp. 13687–13695, 1996.
[7]  D. L. Ho, B. Hammouda, and S. R. Kline, “Clustering of poly(ethylene oxide) in water revisited,” Journal of Polymer Science B, vol. 41, no. 1, pp. 135–138, 2002.
[8]  A. K. Khasanova and B. A. Wolf, “PEO/CHCl3. Crystallinity of the polymer and vapor pressure of the solvent. Equilibrium and nonequilibrium phenomena,” Macromolecules, vol. 36, no. 17, pp. 6645–6652, 2003.
[9]  M. Duval, “Monitoring of cluster formation and elimination in PEO solutions,” Macromolecules, vol. 33, no. 21, pp. 7862–7867, 2000.
[10]  M. Duval and F. Boué, “Dilute polyethylene oxide aqueous solutions in a turbulent flow,” Macromolecules, vol. 40, no. 23, pp. 8384–8388, 2007.
[11]  T. Miyazawa, K. Fukushima, and Y. Ideguchi, “Molecular vibrations and structure of high polymers. III. Polarized infrared spectra, normal vibrations, and helical conformation of polyethylene glycol,” The Journal of Chemical Physics, vol. 37, no. 12, pp. 2764–2776, 1962.
[12]  H. Matsuura and T. Miyazawa, “Vibrational analysis of molten poly (ethylene glycol),” Journal of Polymer Science Part A-2, vol. 7, pp. 1735–1744, 1969.
[13]  R. Frech, S. Chintapalli, P. G. Bruce, and C. A. Vincent, “Crystalline and amorphous phases in the poly(ethylene oxide)-LiCF3SO3 system,” Macromolecules, vol. 32, no. 3, pp. 808–813, 1999.
[14]  Y. Geng, G. Wang, Y. Cong, L. Bai, L. Li, and C. Yang, “Surface adsorption-induced conformational ordering and crystallization of polyethylene oxide,” Journal of Polymer Science B, vol. 48, no. 2, pp. 106–112, 2010.
[15]  M. Spitzer, E. Sabadini, and W. Loh, “Entropically driven partitioning of ethylene oxide oligomers and polymers in aqueous/organic biphasic systems,” Journal of Physical Chemistry B, vol. 106, no. 48, pp. 12448–12452, 2002.
[16]  J. M. Harris, Polyethylene Glycol Chemistry, Biotechnical and Biomedical Applications, Plenum Press, New York, NY, USA, 1992.
[17]  F. Gouanvé, H. Phuong-Nguyen, Z. F. Hamida, and G. Delmas, “A new technique to characterize mono-molecular micelles in random ethylene-propylene copolymers,” Colloid and Polymer Science, vol. 283, no. 9, pp. 994–1006, 2005.
[18]  H. Phuong-Nguyen, Melting Behaviour of Strained Crystals of Ultra High Molecular Weight Polyethylene with and without Solvent, Ph.D. thesis, McGill University, Montreal, Canada, 1990.
[19]  H. Phuong-Nguyen and G. Delmas, “Arrested melting due to strain in ultrahigh molecular weight polyethylene,” Macromolecules, vol. 25, no. 1, pp. 408–413, 1992.
[20]  H. Phuong-Nguyen and G. Delmas, “Thermal analysis and model of ultrahigh molecular weight polyethylene gels,” Macromolecules, vol. 25, no. 1, pp. 414–421, 1992.
[21]  G. Delmas, “Irreversible formation of a network during melting/dissolution of nascent PE,” Journal of Polymer Science B, vol. 31, no. 13, pp. 2011–2018, 1993.
[22]  H. Phuong-Nguyen and G. Delmas, “Information given by slow melting on phase content and maximum drawability of high molecular weight polyethylene films,” Journal of Materials Science, vol. 29, no. 14, pp. 3612–3620, 1994.
[23]  X. Zhang, H. Phuong-Nguyen, P. Bernazzani, I. Lapes, and G. Delmas, “Information on the noncrystalline phase of nascent iPP given by slow calorimetry,” Canadian Journal of Chemistry, vol. 75, no. 10, pp. 1354–1362, 1997.
[24]  H. Phuong-Nguyen and G. Delmas, “Crystallization of Isotactic Poly (propylene) in Solution as Followed by Slow Calorimetry,” Collection of Czechoslovak Chemical Communications, vol. 60, pp. 1905–1924, 1995.
[25]  H. Phuong-Nguyen, G. Charlet, and G. Delmas, “Slow calorimetry and heat of fusion of poly(4-methyl pentene-1),” Journal of Thermal Analysis, vol. 46, no. 3-4, pp. 809–832, 1996.
[26]  Z. Ferhat-Hamida, H. Phuong-Nguyen, P. Bernazzani, A. Haine, and G. Delmas, “LLDPE's grown with metallocene and Ziegler-Natta catalysts: events in the melt and FTIR analysis,” Journal of Materials Science, vol. 42, no. 9, pp. 3138–3154, 2007.
[27]  I. Jedidi, Z. Ferhat-Hamida, and G. Delmas, “Calorimetry in nonstandard conditions: the noncrystalline phases of linear polyethylene,” Journal of Polymer Science B, vol. 45, no. 15, pp. 1932–1949, 2007.
[28]  P. Bernazzani, Contr?le de la morphologie des systèmes amylose-eau et caractérisation par DSC lent et FTIR, Ph.D. thesis, University of Quebec at Trois-Rivières, Trois-Rivières, Canada, 2000.
[29]  P. Bernazzani, V. T. Bich, H. Phuong-Nguyen et al., “FTIR analysis of the phase content in lowdensity polyethylene,” Canadian Journal of Chemistry, vol. 76, no. 11, pp. 1674–1687, 1998.
[30]  P. Bernazzani, Analyse de la composition phasique du polyéthylène par FTIR: Mise en évidence d’une phase tendue, M.S. thesis, University of Quebec, Montreal, Canada, 1994.
[31]  A. Ajji, J. Guèvremont, K. C. Cole, and M. M. Dumoulin, “Orientation and structure of drawn poly(ethylene terephthalate),” Polymer, vol. 37, no. 16, pp. 3707–3714, 1996.
[32]  P. Bernazzani, C. Chapados, and G. Delmas, “Double-helical network in amylose as seen by slow calorimetry and FTIR,” Journal of Polymer Science B, vol. 38, no. 12, pp. 1662–1677, 2000.
[33]  P. Bernazzani, C. Chapados, and G. Delmas, “Phase change in amylose-water mixtures as seen by Fourier transform infrared,” Biopolymers, vol. 58, no. 3, pp. 305–318, 2001.
[34]  J. M. Marentette and G. R. Brown, “The crystallization of poly(ethylene oxide) in blends with neat and plasticized poly(vinyl chloride),” Polymer, vol. 39, no. 6-7, pp. 1415–1427, 1998.
[35]  C. Bergeron, A. Potier, E. Perrier, and G. Delmas, Part 2 of this work, to be published.
[36]  A. Potier, “Report 2002,” University of Quebec at Montreal and IUT- University of Auvergne 2002.
[37]  A. Pages, “Report 2007,” University of Quebec at Montreal and IUT- University of Auvergne 2007.
[38]  J. Morales, “Report 2005,” University of Quebec at Montreal and IUT- University of Auvergne.
[39]  E. Perrier, “Report 2003,” University of Quebec at Montreal and IUT- University of Auvergne.
[40]  A. Cohade, “Report 2003,” University of Quebec at Montreal and IUT- University of Auvergne.
[41]  J. Bent, L. R. Hutchings, R. W. Richards et al., “Neutron-mapping polymer flow: scattering, flow visualization, and molecular theory,” Science, vol. 301, no. 5640, pp. 1691–1695, 2003.

Full-Text

comments powered by Disqus

Contact Us

service@oalib.com

QQ:3279437679

WhatsApp +8615387084133