Effect of Noncovalent Dispersion of Poly(Ethylene Oxide) in Columnar Polyether-Based Discotic Liquid Crystal on the Ionic Conductivity and Dynamics of Lithium Ions
The ionic conductivity of an electrolyte is represented by a product of carrier density, charge (electric), and ionic mobility. The overall goal of this study was to provide an insight into the influence of lithium ion conductivity and dynamic when a continuous discotic liquid crystal (DLC) matrix o...
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description | The ionic conductivity of an electrolyte is represented by a product of carrier density, charge (electric), and ionic mobility. The overall goal of this study was to provide an insight into the influence of lithium ion conductivity and dynamic when a continuous discotic liquid crystal (DLC) matrix of hexaazatrinapthylene-polyether, HATN-TEG-1, is doped with a small amount of polyethylene oxide (PEO, 5% of MW 8000). The favorable non-covalent interactions between PEO and the DLC triethylene glycol side-chains is supported by the maintenance of the mesophase. The lithium ionic conductivity of HATN-TEG-1 was found to be 1.1 × 10−6 S cm−1, which is better than the corresponding HATN-TEG-1-5%PEO-8000 with a value of 6.06 × 10−7 S cm−1. These results are further supported by the dynamics of the lithium ions in HATN-TEG-1 and HATN-TEG-1-5%PEO-8000 as characterized by 7Li, and 1H NMR spin-lattice relaxation time and self-diffusion coefficient measurements. Though the additional PEO was found to increase the ion carriers, the significant lowering of the ionic conductivity may be attributed to the more pronounced decrease of the mobility of the ionic part when the HATN-TEG-1 matrix is dispersed with PEO. This finding indicates that the doping of 5% PEO onto the matrix of HATN-TEG-1 DLC has an adverse effect on both its diffusion rate and ion conductivity. |
doi_str_mv | 10.3390/cryst9120627 |
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The overall goal of this study was to provide an insight into the influence of lithium ion conductivity and dynamic when a continuous discotic liquid crystal (DLC) matrix of hexaazatrinapthylene-polyether, HATN-TEG-1, is doped with a small amount of polyethylene oxide (PEO, 5% of MW 8000). The favorable non-covalent interactions between PEO and the DLC triethylene glycol side-chains is supported by the maintenance of the mesophase. The lithium ionic conductivity of HATN-TEG-1 was found to be 1.1 × 10−6 S cm−1, which is better than the corresponding HATN-TEG-1-5%PEO-8000 with a value of 6.06 × 10−7 S cm−1. These results are further supported by the dynamics of the lithium ions in HATN-TEG-1 and HATN-TEG-1-5%PEO-8000 as characterized by 7Li, and 1H NMR spin-lattice relaxation time and self-diffusion coefficient measurements. Though the additional PEO was found to increase the ion carriers, the significant lowering of the ionic conductivity may be attributed to the more pronounced decrease of the mobility of the ionic part when the HATN-TEG-1 matrix is dispersed with PEO. This finding indicates that the doping of 5% PEO onto the matrix of HATN-TEG-1 DLC has an adverse effect on both its diffusion rate and ion conductivity.</description><identifier>ISSN: 2073-4352</identifier><identifier>EISSN: 2073-4352</identifier><identifier>DOI: 10.3390/cryst9120627</identifier><language>eng</language><publisher>Basel: MDPI AG</publisher><subject>Carrier density ; Charge density ; Current carriers ; Diffusion coefficient ; Diffusion effects ; Diffusion rate ; Dispersion ; Electrolytes ; Ethylene oxide ; Ion currents ; Ionic mobility ; Ions ; Liquid crystals ; Lithium ; Lithium ions ; Lithium isotopes ; NMR ; Nuclear magnetic resonance ; Polyethylene ; Polyethylene oxide ; Polymer blends ; Polyvinyl alcohol ; Relaxation time ; Self diffusion ; Spectrum analysis ; Spin-lattice relaxation ; Triethylene glycol</subject><ispartof>Crystals (Basel), 2019-12, Vol.9 (12), p.627</ispartof><rights>2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c301t-8f287706629fcba38d0024a45c82cd902ca771abfdadc8dff5730d1232240dc63</citedby><cites>FETCH-LOGICAL-c301t-8f287706629fcba38d0024a45c82cd902ca771abfdadc8dff5730d1232240dc63</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,861,27905,27906</link.rule.ids></links><search><creatorcontrib>Hwang, Jih-Dar</creatorcontrib><creatorcontrib>Chen, Po-Ying</creatorcontrib><creatorcontrib>Ding, Shang-Wu</creatorcontrib><creatorcontrib>Ong, Chi Wi</creatorcontrib><title>Effect of Noncovalent Dispersion of Poly(Ethylene Oxide) in Columnar Polyether-Based Discotic Liquid Crystal on the Ionic Conductivity and Dynamics of Lithium Ions</title><title>Crystals (Basel)</title><description>The ionic conductivity of an electrolyte is represented by a product of carrier density, charge (electric), and ionic mobility. The overall goal of this study was to provide an insight into the influence of lithium ion conductivity and dynamic when a continuous discotic liquid crystal (DLC) matrix of hexaazatrinapthylene-polyether, HATN-TEG-1, is doped with a small amount of polyethylene oxide (PEO, 5% of MW 8000). The favorable non-covalent interactions between PEO and the DLC triethylene glycol side-chains is supported by the maintenance of the mesophase. The lithium ionic conductivity of HATN-TEG-1 was found to be 1.1 × 10−6 S cm−1, which is better than the corresponding HATN-TEG-1-5%PEO-8000 with a value of 6.06 × 10−7 S cm−1. These results are further supported by the dynamics of the lithium ions in HATN-TEG-1 and HATN-TEG-1-5%PEO-8000 as characterized by 7Li, and 1H NMR spin-lattice relaxation time and self-diffusion coefficient measurements. Though the additional PEO was found to increase the ion carriers, the significant lowering of the ionic conductivity may be attributed to the more pronounced decrease of the mobility of the ionic part when the HATN-TEG-1 matrix is dispersed with PEO. This finding indicates that the doping of 5% PEO onto the matrix of HATN-TEG-1 DLC has an adverse effect on both its diffusion rate and ion conductivity.</description><subject>Carrier density</subject><subject>Charge density</subject><subject>Current carriers</subject><subject>Diffusion coefficient</subject><subject>Diffusion effects</subject><subject>Diffusion rate</subject><subject>Dispersion</subject><subject>Electrolytes</subject><subject>Ethylene oxide</subject><subject>Ion currents</subject><subject>Ionic mobility</subject><subject>Ions</subject><subject>Liquid crystals</subject><subject>Lithium</subject><subject>Lithium ions</subject><subject>Lithium isotopes</subject><subject>NMR</subject><subject>Nuclear magnetic resonance</subject><subject>Polyethylene</subject><subject>Polyethylene oxide</subject><subject>Polymer blends</subject><subject>Polyvinyl alcohol</subject><subject>Relaxation time</subject><subject>Self diffusion</subject><subject>Spectrum analysis</subject><subject>Spin-lattice relaxation</subject><subject>Triethylene glycol</subject><issn>2073-4352</issn><issn>2073-4352</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNpNkUtOwzAQhi0EEhV0xwEssQGJgGMncbqEUKBSRFnAOnL9UF0ldms7FTkPF8WhLDqbGen_5g3AVYruCZmhB-4GH2YpRgWmJ2CCESVJRnJ8ehSfg6n3GxSNFojSdAJ-5kpJHqBV8N0abveslSbAZ-230nltzah82Ha4mYf1EDUJl99ayFuoDaxs23eGuT9AhrV0yRPzUozp3AbNYa13vRawGmdjLYzlIgUX1kStskb0POi9DgNkJmYNhnWa-7FlrcNa992I-ktwpljr5fTfX4Cvl_ln9ZbUy9dF9VgnnKA0JKXCJaWoKPBM8RUjpUAIZyzLeYm5mCHMWVyZrZRggpdCqZwSJFJMMM6Q4AW5ANeHultnd730odnY3pnYssE5jactCpJF6u5AcWe9d1I1W6c75oYmRc34ieb4E-QXxcp-uQ</recordid><startdate>20191201</startdate><enddate>20191201</enddate><creator>Hwang, Jih-Dar</creator><creator>Chen, Po-Ying</creator><creator>Ding, Shang-Wu</creator><creator>Ong, Chi Wi</creator><general>MDPI AG</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope></search><sort><creationdate>20191201</creationdate><title>Effect of Noncovalent Dispersion of Poly(Ethylene Oxide) in Columnar Polyether-Based Discotic Liquid Crystal on the Ionic Conductivity and Dynamics of Lithium Ions</title><author>Hwang, Jih-Dar ; Chen, Po-Ying ; Ding, Shang-Wu ; Ong, Chi Wi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c301t-8f287706629fcba38d0024a45c82cd902ca771abfdadc8dff5730d1232240dc63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Carrier density</topic><topic>Charge density</topic><topic>Current carriers</topic><topic>Diffusion coefficient</topic><topic>Diffusion effects</topic><topic>Diffusion rate</topic><topic>Dispersion</topic><topic>Electrolytes</topic><topic>Ethylene oxide</topic><topic>Ion currents</topic><topic>Ionic mobility</topic><topic>Ions</topic><topic>Liquid crystals</topic><topic>Lithium</topic><topic>Lithium ions</topic><topic>Lithium isotopes</topic><topic>NMR</topic><topic>Nuclear magnetic resonance</topic><topic>Polyethylene</topic><topic>Polyethylene oxide</topic><topic>Polymer blends</topic><topic>Polyvinyl alcohol</topic><topic>Relaxation time</topic><topic>Self diffusion</topic><topic>Spectrum analysis</topic><topic>Spin-lattice relaxation</topic><topic>Triethylene glycol</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hwang, Jih-Dar</creatorcontrib><creatorcontrib>Chen, Po-Ying</creatorcontrib><creatorcontrib>Ding, Shang-Wu</creatorcontrib><creatorcontrib>Ong, Chi Wi</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Research Database</collection><collection>Materials Science Database</collection><collection>Materials Science Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><jtitle>Crystals (Basel)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hwang, Jih-Dar</au><au>Chen, Po-Ying</au><au>Ding, Shang-Wu</au><au>Ong, Chi Wi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of Noncovalent Dispersion of Poly(Ethylene Oxide) in Columnar Polyether-Based Discotic Liquid Crystal on the Ionic Conductivity and Dynamics of Lithium Ions</atitle><jtitle>Crystals (Basel)</jtitle><date>2019-12-01</date><risdate>2019</risdate><volume>9</volume><issue>12</issue><spage>627</spage><pages>627-</pages><issn>2073-4352</issn><eissn>2073-4352</eissn><abstract>The ionic conductivity of an electrolyte is represented by a product of carrier density, charge (electric), and ionic mobility. The overall goal of this study was to provide an insight into the influence of lithium ion conductivity and dynamic when a continuous discotic liquid crystal (DLC) matrix of hexaazatrinapthylene-polyether, HATN-TEG-1, is doped with a small amount of polyethylene oxide (PEO, 5% of MW 8000). The favorable non-covalent interactions between PEO and the DLC triethylene glycol side-chains is supported by the maintenance of the mesophase. The lithium ionic conductivity of HATN-TEG-1 was found to be 1.1 × 10−6 S cm−1, which is better than the corresponding HATN-TEG-1-5%PEO-8000 with a value of 6.06 × 10−7 S cm−1. These results are further supported by the dynamics of the lithium ions in HATN-TEG-1 and HATN-TEG-1-5%PEO-8000 as characterized by 7Li, and 1H NMR spin-lattice relaxation time and self-diffusion coefficient measurements. Though the additional PEO was found to increase the ion carriers, the significant lowering of the ionic conductivity may be attributed to the more pronounced decrease of the mobility of the ionic part when the HATN-TEG-1 matrix is dispersed with PEO. This finding indicates that the doping of 5% PEO onto the matrix of HATN-TEG-1 DLC has an adverse effect on both its diffusion rate and ion conductivity.</abstract><cop>Basel</cop><pub>MDPI AG</pub><doi>10.3390/cryst9120627</doi><oa>free_for_read</oa></addata></record> |
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subjects | Carrier density Charge density Current carriers Diffusion coefficient Diffusion effects Diffusion rate Dispersion Electrolytes Ethylene oxide Ion currents Ionic mobility Ions Liquid crystals Lithium Lithium ions Lithium isotopes NMR Nuclear magnetic resonance Polyethylene Polyethylene oxide Polymer blends Polyvinyl alcohol Relaxation time Self diffusion Spectrum analysis Spin-lattice relaxation Triethylene glycol |
title | Effect of Noncovalent Dispersion of Poly(Ethylene Oxide) in Columnar Polyether-Based Discotic Liquid Crystal on the Ionic Conductivity and Dynamics of Lithium Ions |
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