Monte Carlo Simulation of Head-to-Head, Tail-to-Tail Polypropylene and Its Mixing with Polyethylene in the Melt

Simulations have been performed at 473 K for one-component melts of polyethylene (PE) and head-to-head, tail-to-tail polypropylene (hhPP) as well as a mixture of the two species. The densities are 0.760, 0.753, and 0.756 g/cm3 for these three NVT simulations, respectively. The Monte Carlo simulation...

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Veröffentlicht in:Macromolecules 2001-05, Vol.34 (10), p.3389-3395
Hauptverfasser: Akten, E. Demet, Mattice, Wayne L
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description Simulations have been performed at 473 K for one-component melts of polyethylene (PE) and head-to-head, tail-to-tail polypropylene (hhPP) as well as a mixture of the two species. The densities are 0.760, 0.753, and 0.756 g/cm3 for these three NVT simulations, respectively. The Monte Carlo simulation uses coarse-grained representations of the chains on a sparsely occupied high coordination lattice. The short-range intramolecular interactions are controlled by rotational isomeric state models for the two types of chains, and the intermolecular interactions are represented by a discretized version of Lennard-Jones potential energy functions. Equilibrated coarse-grained replicas are reverse-mapped to atomistically detailed models in continuous space. The pair correlation functions clearly demonstrate the onset of demixing for the two-component melt, which is qualitatively consistent with the conclusion from small-angle neutron scattering reported by Jeon et al. [Macromolecules 1998, 31, 3340]. Analysis of the components of the energy in the simulations shows that the positive energy change on mixing is completely dominated by the intermolecular Lennard-Jones contributions, with negligible contributions from the short-range intramolecular interactions in the rotational isomeric state models. Quantitative comparison with experiment shows that the χ deduced from the simulations is larger than the χ deduced from the experiments. Several factors in the experiments and in the simulations may contribute to the quantitative difference.
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The pair correlation functions clearly demonstrate the onset of demixing for the two-component melt, which is qualitatively consistent with the conclusion from small-angle neutron scattering reported by Jeon et al. [Macromolecules 1998, 31, 3340]. Analysis of the components of the energy in the simulations shows that the positive energy change on mixing is completely dominated by the intermolecular Lennard-Jones contributions, with negligible contributions from the short-range intramolecular interactions in the rotational isomeric state models. Quantitative comparison with experiment shows that the χ deduced from the simulations is larger than the χ deduced from the experiments. 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Demet</creatorcontrib><creatorcontrib>Mattice, Wayne L</creatorcontrib><title>Monte Carlo Simulation of Head-to-Head, Tail-to-Tail Polypropylene and Its Mixing with Polyethylene in the Melt</title><title>Macromolecules</title><addtitle>Macromolecules</addtitle><description>Simulations have been performed at 473 K for one-component melts of polyethylene (PE) and head-to-head, tail-to-tail polypropylene (hhPP) as well as a mixture of the two species. The densities are 0.760, 0.753, and 0.756 g/cm3 for these three NVT simulations, respectively. The Monte Carlo simulation uses coarse-grained representations of the chains on a sparsely occupied high coordination lattice. The short-range intramolecular interactions are controlled by rotational isomeric state models for the two types of chains, and the intermolecular interactions are represented by a discretized version of Lennard-Jones potential energy functions. Equilibrated coarse-grained replicas are reverse-mapped to atomistically detailed models in continuous space. The pair correlation functions clearly demonstrate the onset of demixing for the two-component melt, which is qualitatively consistent with the conclusion from small-angle neutron scattering reported by Jeon et al. [Macromolecules 1998, 31, 3340]. Analysis of the components of the energy in the simulations shows that the positive energy change on mixing is completely dominated by the intermolecular Lennard-Jones contributions, with negligible contributions from the short-range intramolecular interactions in the rotational isomeric state models. Quantitative comparison with experiment shows that the χ deduced from the simulations is larger than the χ deduced from the experiments. Several factors in the experiments and in the simulations may contribute to the quantitative difference.</description><subject>Applied sciences</subject><subject>Exact sciences and technology</subject><subject>Organic polymers</subject><subject>Physicochemistry of polymers</subject><subject>Properties and characterization</subject><subject>Structure, morphology and analysis</subject><issn>0024-9297</issn><issn>1520-5835</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNptkE1PGzEQhq0KpIbQQ_-BDxSpEkv9md09QlQ-BFEjkdKjNet4ialjp7ajJv--u12EOHB6ZzzPvGO9CH2m5JwSRr-tgRBGSl5_QCMqGSlkxeUBGnWvoqhZXX5ERyk9E0KpFHyEwiz4bPAUogv4wa63DrINHocW3xhYFjkUvZ7hBVjXd73ieXD7TQybvTPeYPBLfJsTntmd9U_4r82r_4TJqwGwHueVwTPj8jE6bMEl8-lFx-jn1ffF9Ka4_3F9O724L4BLmQshKilBc82aRgCrBdG8bmsOxjQcRMUoZ1zQiViStiRQsUY2JW00g5K1XcHH6HTw7b75Z2tSVmubtHEOvAnbpNikolTwqgO_DqCOIaVoWrWJdg1xryhRfaTqNdKOPXkxhaTBtRG8tunNApe0lh1WDJhN2exexxB_q0nJS6kW8wf1eHdNfj3Wl6q3_TLwoJN6Dtvou2TeOf8PEjGPtw</recordid><startdate>20010508</startdate><enddate>20010508</enddate><creator>Akten, E. 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Demet ; Mattice, Wayne L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a355t-44855ac3c2bb4a2940c39f93aeeb3a48213234164d0f70a82b5b71bc2a72f71b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><topic>Applied sciences</topic><topic>Exact sciences and technology</topic><topic>Organic polymers</topic><topic>Physicochemistry of polymers</topic><topic>Properties and characterization</topic><topic>Structure, morphology and analysis</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Akten, E. 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Demet</au><au>Mattice, Wayne L</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Monte Carlo Simulation of Head-to-Head, Tail-to-Tail Polypropylene and Its Mixing with Polyethylene in the Melt</atitle><jtitle>Macromolecules</jtitle><addtitle>Macromolecules</addtitle><date>2001-05-08</date><risdate>2001</risdate><volume>34</volume><issue>10</issue><spage>3389</spage><epage>3395</epage><pages>3389-3395</pages><issn>0024-9297</issn><eissn>1520-5835</eissn><coden>MAMOBX</coden><abstract>Simulations have been performed at 473 K for one-component melts of polyethylene (PE) and head-to-head, tail-to-tail polypropylene (hhPP) as well as a mixture of the two species. The densities are 0.760, 0.753, and 0.756 g/cm3 for these three NVT simulations, respectively. The Monte Carlo simulation uses coarse-grained representations of the chains on a sparsely occupied high coordination lattice. 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Quantitative comparison with experiment shows that the χ deduced from the simulations is larger than the χ deduced from the experiments. Several factors in the experiments and in the simulations may contribute to the quantitative difference.</abstract><cop>Washington, DC</cop><pub>American Chemical Society</pub><doi>10.1021/ma0020739</doi><tpages>7</tpages></addata></record>
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Exact sciences and technology
Organic polymers
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Properties and characterization
Structure, morphology and analysis
title Monte Carlo Simulation of Head-to-Head, Tail-to-Tail Polypropylene and Its Mixing with Polyethylene in the Melt
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