Size-Dependent Transitions in Grafted Polymer Brushes
The partition function of a grafted polymer brush was calculated as a sum over all possible configurations, each of them being an ensemble of n 1, n 2, ...n i , ... loops having 2, 4, ..., 2i, ... segments. A system of equations for the most likely configuration has been obtained, and it was conclud...
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Veröffentlicht in: | The journal of physical chemistry. B 2013-08, Vol.117 (32), p.9532-9539 |
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creator | Manciu, Marian Bosse, Courtney Ruckenstein, Eli |
description | The partition function of a grafted polymer brush was calculated as a sum over all possible configurations, each of them being an ensemble of n 1, n 2, ...n i , ... loops having 2, 4, ..., 2i, ... segments. A system of equations for the most likely configuration has been obtained, and it was concluded that no solution exists for an infinite chain, with nonvanishing interactions between segments and surface. This implies that an infinite chain is either collapsed on the surface (for attractive interactions) or is forming a stretched brush (for repulsive interactions). However, for finite chains, a solution could be found. When the attractive segment–surface interaction becomes sufficiently strong, the brush collapses on the surface (the “loops” to “trains” transition). When the interaction is repulsive and sufficiently strong, the brush becomes stretched, with most segments belonging to open loops which do not return to the surface (the “loops” to “tails” transition). The critical values of the segment–surface interaction, for which the above transitions occur, depend on the length of the polymer chain as well as on other physical properties of the brush, such as the segment–segment and segment–solvent interactions and the grafting density. |
doi_str_mv | 10.1021/jp403309t |
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A system of equations for the most likely configuration has been obtained, and it was concluded that no solution exists for an infinite chain, with nonvanishing interactions between segments and surface. This implies that an infinite chain is either collapsed on the surface (for attractive interactions) or is forming a stretched brush (for repulsive interactions). However, for finite chains, a solution could be found. When the attractive segment–surface interaction becomes sufficiently strong, the brush collapses on the surface (the “loops” to “trains” transition). When the interaction is repulsive and sufficiently strong, the brush becomes stretched, with most segments belonging to open loops which do not return to the surface (the “loops” to “tails” transition). The critical values of the segment–surface interaction, for which the above transitions occur, depend on the length of the polymer chain as well as on other physical properties of the brush, such as the segment–segment and segment–solvent interactions and the grafting density.</description><identifier>ISSN: 1520-6106</identifier><identifier>EISSN: 1520-5207</identifier><identifier>DOI: 10.1021/jp403309t</identifier><identifier>PMID: 23879714</identifier><language>eng</language><publisher>Washington, DC: American Chemical Society</publisher><subject>Applied sciences ; Brushes ; Chains ; Density ; Exact sciences and technology ; Grafting ; Mathematical analysis ; Physical chemistry ; Physical properties ; Physicochemistry of polymers ; Segments</subject><ispartof>The journal of physical chemistry. 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When the interaction is repulsive and sufficiently strong, the brush becomes stretched, with most segments belonging to open loops which do not return to the surface (the “loops” to “tails” transition). The critical values of the segment–surface interaction, for which the above transitions occur, depend on the length of the polymer chain as well as on other physical properties of the brush, such as the segment–segment and segment–solvent interactions and the grafting density.</description><subject>Applied sciences</subject><subject>Brushes</subject><subject>Chains</subject><subject>Density</subject><subject>Exact sciences and technology</subject><subject>Grafting</subject><subject>Mathematical analysis</subject><subject>Physical chemistry</subject><subject>Physical properties</subject><subject>Physicochemistry of polymers</subject><subject>Segments</subject><issn>1520-6106</issn><issn>1520-5207</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNqF0E1LwzAYwPEgipvTg19AehH0UM1Lk7RHnTqFgYLzXNLkKXb0ZeZpD_PTW13dLoKH8OTw4wn5E3LK6BWjnF0vVxEVgibtHhkzyWnYH70_3BWjakSOEJeUcsljdUhGXMQ60SwaE_lafEJ4ByuoHdRtsPCmxqItmhqDog5m3uQtuOClKdcV-ODWd_gOeEwOclMinAxzQt4e7hfTx3D-PHua3sxDI0TchsrIzNgsVpbGGZeS0lhoaqTInHIm4lIJqTXPOHMRixQ4p13ORcZ4om0OkZiQi83elW8-OsA2rQq0UJamhqbDlGkppEiYTv6nEVc_AVRPLzfU-gbRQ56ufFEZv04ZTb-DptugvT0b1nZZBW4rfwv24HwABq0p876fLXDntNL9F8XOGYvpsul83Yf748EvTE6HKw</recordid><startdate>20130815</startdate><enddate>20130815</enddate><creator>Manciu, Marian</creator><creator>Bosse, Courtney</creator><creator>Ruckenstein, Eli</creator><general>American Chemical Society</general><scope>IQODW</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20130815</creationdate><title>Size-Dependent Transitions in Grafted Polymer Brushes</title><author>Manciu, Marian ; Bosse, Courtney ; Ruckenstein, Eli</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a338t-6a5bacb86c08b255008370a53bd6da425635772b21d4146edd7df23b1297cfe43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Applied sciences</topic><topic>Brushes</topic><topic>Chains</topic><topic>Density</topic><topic>Exact sciences and technology</topic><topic>Grafting</topic><topic>Mathematical analysis</topic><topic>Physical chemistry</topic><topic>Physical properties</topic><topic>Physicochemistry of polymers</topic><topic>Segments</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Manciu, Marian</creatorcontrib><creatorcontrib>Bosse, Courtney</creatorcontrib><creatorcontrib>Ruckenstein, Eli</creatorcontrib><collection>Pascal-Francis</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>The journal of physical chemistry. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Manciu, Marian</au><au>Bosse, Courtney</au><au>Ruckenstein, Eli</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Size-Dependent Transitions in Grafted Polymer Brushes</atitle><jtitle>The journal of physical chemistry. B</jtitle><addtitle>J. Phys. Chem. B</addtitle><date>2013-08-15</date><risdate>2013</risdate><volume>117</volume><issue>32</issue><spage>9532</spage><epage>9539</epage><pages>9532-9539</pages><issn>1520-6106</issn><eissn>1520-5207</eissn><abstract>The partition function of a grafted polymer brush was calculated as a sum over all possible configurations, each of them being an ensemble of n 1, n 2, ...n i , ... loops having 2, 4, ..., 2i, ... segments. A system of equations for the most likely configuration has been obtained, and it was concluded that no solution exists for an infinite chain, with nonvanishing interactions between segments and surface. This implies that an infinite chain is either collapsed on the surface (for attractive interactions) or is forming a stretched brush (for repulsive interactions). However, for finite chains, a solution could be found. When the attractive segment–surface interaction becomes sufficiently strong, the brush collapses on the surface (the “loops” to “trains” transition). When the interaction is repulsive and sufficiently strong, the brush becomes stretched, with most segments belonging to open loops which do not return to the surface (the “loops” to “tails” transition). The critical values of the segment–surface interaction, for which the above transitions occur, depend on the length of the polymer chain as well as on other physical properties of the brush, such as the segment–segment and segment–solvent interactions and the grafting density.</abstract><cop>Washington, DC</cop><pub>American Chemical Society</pub><pmid>23879714</pmid><doi>10.1021/jp403309t</doi><tpages>8</tpages></addata></record> |
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subjects | Applied sciences Brushes Chains Density Exact sciences and technology Grafting Mathematical analysis Physical chemistry Physical properties Physicochemistry of polymers Segments |
title | Size-Dependent Transitions in Grafted Polymer Brushes |
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