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Dynamics of Cellulose−Water Interfaces: NMR Spin−Lattice Relaxation Times Calculated from Atomistic Computer Simulations
Solid-state nuclear magnetic resonance (CP/MAS 13C NMR) spectroscopy has often been used to study cellulose structure, but some features of the cellulose NMR spectrum are not yet fully understood. One such feature is a doublet around 84 ppm, a signal that has been proposed to originate from C4 atoms...
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Published in: | The journal of physical chemistry. B 2008-03, Vol.112 (9), p.2590-2595 |
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description | Solid-state nuclear magnetic resonance (CP/MAS 13C NMR) spectroscopy has often been used to study cellulose structure, but some features of the cellulose NMR spectrum are not yet fully understood. One such feature is a doublet around 84 ppm, a signal that has been proposed to originate from C4 atoms at cellulose fibril surfaces. The two peaks yield different T 1, differing by approximately a factor of 2 at 75 MHz. In this study, we calculate T 1 from C4−H4 vector dynamics obtained from molecular dynamics computer simulations of cellulose I β−water interfacial systems. Calculated and experimentally obtained T 1 values for C4 atoms in surface chains fell within the same order of magnitude, 3−20 s. This means that the applied force field reproduces relevant surface dynamics for the cellulose−water interface sufficiently well. Furthermore, a difference in T 1 of about a factor of 2 in the range of Larmor frequencies 25−150 MHz was found for C4 atoms in chains located on top of two different crystallographic planes, namely, (110) and (11̄0). A previously proposed explanation that the C4 peak doublet could derive from surfaces parallel to different crystallographic planes is herewith strengthened by computationally obtained evidence. Another suggested basis for this difference is that the doublet originates from C4 atoms located in surface anhydro-glucose units with hydroxymethyl groups pointing either inward or outward. This was also tested within this study but was found to yield no difference in calculated T 1. |
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One such feature is a doublet around 84 ppm, a signal that has been proposed to originate from C4 atoms at cellulose fibril surfaces. The two peaks yield different T 1, differing by approximately a factor of 2 at 75 MHz. In this study, we calculate T 1 from C4−H4 vector dynamics obtained from molecular dynamics computer simulations of cellulose I β−water interfacial systems. Calculated and experimentally obtained T 1 values for C4 atoms in surface chains fell within the same order of magnitude, 3−20 s. This means that the applied force field reproduces relevant surface dynamics for the cellulose−water interface sufficiently well. Furthermore, a difference in T 1 of about a factor of 2 in the range of Larmor frequencies 25−150 MHz was found for C4 atoms in chains located on top of two different crystallographic planes, namely, (110) and (11̄0). A previously proposed explanation that the C4 peak doublet could derive from surfaces parallel to different crystallographic planes is herewith strengthened by computationally obtained evidence. Another suggested basis for this difference is that the doublet originates from C4 atoms located in surface anhydro-glucose units with hydroxymethyl groups pointing either inward or outward. 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B</title><addtitle>J. Phys. Chem. B</addtitle><description>Solid-state nuclear magnetic resonance (CP/MAS 13C NMR) spectroscopy has often been used to study cellulose structure, but some features of the cellulose NMR spectrum are not yet fully understood. One such feature is a doublet around 84 ppm, a signal that has been proposed to originate from C4 atoms at cellulose fibril surfaces. The two peaks yield different T 1, differing by approximately a factor of 2 at 75 MHz. In this study, we calculate T 1 from C4−H4 vector dynamics obtained from molecular dynamics computer simulations of cellulose I β−water interfacial systems. Calculated and experimentally obtained T 1 values for C4 atoms in surface chains fell within the same order of magnitude, 3−20 s. This means that the applied force field reproduces relevant surface dynamics for the cellulose−water interface sufficiently well. Furthermore, a difference in T 1 of about a factor of 2 in the range of Larmor frequencies 25−150 MHz was found for C4 atoms in chains located on top of two different crystallographic planes, namely, (110) and (11̄0). A previously proposed explanation that the C4 peak doublet could derive from surfaces parallel to different crystallographic planes is herewith strengthened by computationally obtained evidence. Another suggested basis for this difference is that the doublet originates from C4 atoms located in surface anhydro-glucose units with hydroxymethyl groups pointing either inward or outward. This was also tested within this study but was found to yield no difference in calculated T 1.</description><subject>Algorithms</subject><subject>Carbon - chemistry</subject><subject>Cellulose - chemistry</subject><subject>cellulose-water interface</subject><subject>Chemistry</subject><subject>Computer Simulation</subject><subject>Fysikalisk kemi</subject><subject>Kemi</subject><subject>Magnetic Resonance Spectroscopy - methods</subject><subject>Models, Molecular</subject><subject>molecular dynamics</subject><subject>NATURAL SCIENCES</subject><subject>NATURVETENSKAP</subject><subject>Organic chemistry</subject><subject>Organisk kemi</subject><subject>Physical chemistry</subject><subject>Polymer chemistry</subject><subject>Polymerkemi</subject><subject>Rotation</subject><subject>spin-lattice relaxation times</subject><subject>Surface Properties</subject><subject>Water - chemistry</subject><issn>1520-6106</issn><issn>1520-5207</issn><issn>1520-5207</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNqN0U1v0zAcBvAIgdgYHPgCyBeQEAr43cluVTropPKitQKJi-Um_zB3SRzsZGwnOMKVj7hPgqtWnZA4cHBsxT8_lvwkyWOCXxJMyat1jxWXnAx3kkMiKE7jUHd3a0mwPEgehLDGmAqayfvJAcmolEyQw-T79LozrS0DcjUqoGnGxgW4-fn7kxnAo9MufmtTQji--fELvXt7hha97eL-3AyDLQGdQWOuzGBdh5a2hYAK05RjE09XqPauRZPBtTZEiwrX9uMmdWHbjYhnwsPkXm2aAI9281GyfH2yLGbp_P2b02IyT42gbEhVzliJy5zmjPJKcWowZFmG60qtuOCCEAAQVUYIXtUZECYFBcBKVqWpgLKj5MU2NnyDflzp3tvW-GvtjNVT-3Ginf-ivdU0V5j9n74YznXOlYj6-Vafm-YvOpvM9eYfxgyzTOFLEu2zre29-zpCGHR8mzI-u-nAjUHH2zlWlN-Glt6F4KHeJxOsN6XrfenRPtmFjqsWqlu5azmCdAtiD3C13zf-QkvFlNDLDwtNPk9nXJKFVtE_3XpTBr12o-9iNf-4-A9YqMXh</recordid><startdate>20080306</startdate><enddate>20080306</enddate><creator>Bergenstråhle, Malin</creator><creator>Wohlert, Jakob</creator><creator>Larsson, Per Tomas</creator><creator>Mazeau, Karim</creator><creator>Berglund, Lars A</creator><general>American Chemical Society</general><scope>BSCLL</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>1XC</scope><scope>ADTPV</scope><scope>AOWAS</scope><scope>D8V</scope></search><sort><creationdate>20080306</creationdate><title>Dynamics of Cellulose−Water Interfaces: NMR Spin−Lattice Relaxation Times Calculated from Atomistic Computer Simulations</title><author>Bergenstråhle, Malin ; Wohlert, Jakob ; Larsson, Per Tomas ; Mazeau, Karim ; Berglund, Lars A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a523t-7933c0c929324d742a0e8880fd7b454511eee5d8110bf8e13652ee076dcade23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>Algorithms</topic><topic>Carbon - chemistry</topic><topic>Cellulose - chemistry</topic><topic>cellulose-water interface</topic><topic>Chemistry</topic><topic>Computer Simulation</topic><topic>Fysikalisk kemi</topic><topic>Kemi</topic><topic>Magnetic Resonance Spectroscopy - methods</topic><topic>Models, Molecular</topic><topic>molecular dynamics</topic><topic>NATURAL SCIENCES</topic><topic>NATURVETENSKAP</topic><topic>Organic chemistry</topic><topic>Organisk kemi</topic><topic>Physical chemistry</topic><topic>Polymer chemistry</topic><topic>Polymerkemi</topic><topic>Rotation</topic><topic>spin-lattice relaxation times</topic><topic>Surface Properties</topic><topic>Water - chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bergenstråhle, Malin</creatorcontrib><creatorcontrib>Wohlert, Jakob</creatorcontrib><creatorcontrib>Larsson, Per Tomas</creatorcontrib><creatorcontrib>Mazeau, Karim</creatorcontrib><creatorcontrib>Berglund, Lars A</creatorcontrib><collection>Istex</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>SwePub</collection><collection>SwePub Articles</collection><collection>SWEPUB Kungliga Tekniska Högskolan</collection><jtitle>The journal of physical chemistry. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bergenstråhle, Malin</au><au>Wohlert, Jakob</au><au>Larsson, Per Tomas</au><au>Mazeau, Karim</au><au>Berglund, Lars A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dynamics of Cellulose−Water Interfaces: NMR Spin−Lattice Relaxation Times Calculated from Atomistic Computer Simulations</atitle><jtitle>The journal of physical chemistry. B</jtitle><addtitle>J. Phys. Chem. B</addtitle><date>2008-03-06</date><risdate>2008</risdate><volume>112</volume><issue>9</issue><spage>2590</spage><epage>2595</epage><pages>2590-2595</pages><issn>1520-6106</issn><issn>1520-5207</issn><eissn>1520-5207</eissn><abstract>Solid-state nuclear magnetic resonance (CP/MAS 13C NMR) spectroscopy has often been used to study cellulose structure, but some features of the cellulose NMR spectrum are not yet fully understood. One such feature is a doublet around 84 ppm, a signal that has been proposed to originate from C4 atoms at cellulose fibril surfaces. The two peaks yield different T 1, differing by approximately a factor of 2 at 75 MHz. In this study, we calculate T 1 from C4−H4 vector dynamics obtained from molecular dynamics computer simulations of cellulose I β−water interfacial systems. Calculated and experimentally obtained T 1 values for C4 atoms in surface chains fell within the same order of magnitude, 3−20 s. This means that the applied force field reproduces relevant surface dynamics for the cellulose−water interface sufficiently well. Furthermore, a difference in T 1 of about a factor of 2 in the range of Larmor frequencies 25−150 MHz was found for C4 atoms in chains located on top of two different crystallographic planes, namely, (110) and (11̄0). A previously proposed explanation that the C4 peak doublet could derive from surfaces parallel to different crystallographic planes is herewith strengthened by computationally obtained evidence. Another suggested basis for this difference is that the doublet originates from C4 atoms located in surface anhydro-glucose units with hydroxymethyl groups pointing either inward or outward. This was also tested within this study but was found to yield no difference in calculated T 1.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>18266351</pmid><doi>10.1021/jp074641t</doi><tpages>6</tpages></addata></record> |
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subjects | Algorithms Carbon - chemistry Cellulose - chemistry cellulose-water interface Chemistry Computer Simulation Fysikalisk kemi Kemi Magnetic Resonance Spectroscopy - methods Models, Molecular molecular dynamics NATURAL SCIENCES NATURVETENSKAP Organic chemistry Organisk kemi Physical chemistry Polymer chemistry Polymerkemi Rotation spin-lattice relaxation times Surface Properties Water - chemistry |
title | Dynamics of Cellulose−Water Interfaces: NMR Spin−Lattice Relaxation Times Calculated from Atomistic Computer Simulations |
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