Atomistic understanding of the network dilation anomaly in ion-exchanged glass
Chemically strengthened glasses are of increasing technological importance for personal electronic devices, tablet computers, and a variety of other applications. However, there are many unexplained phenomena associated with the physics of the ion exchange process used for strengthening. One of the...
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Veröffentlicht in: | Journal of non-crystalline solids 2012-01, Vol.358 (2), p.316-320 |
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description | Chemically strengthened glasses are of increasing technological importance for personal electronic devices, tablet computers, and a variety of other applications. However, there are many unexplained phenomena associated with the physics of the ion exchange process used for strengthening. One of the most puzzling of these is the anomalous behavior of the network dilation coefficient, i.e., the parameter governing the amount of linear strain of the glass per unit of alkali ions exchanged, which is inevitably a factor of 2–4 higher for as-melted glasses as compared to chemically strengthened versions of the same glass compositions prepared via ion exchange. In this paper, we investigate the atomistic origin of this discrepancy between as-melted and ion-exchanged glasses based on molecular dynamics simulations of a series of alkali tetrasilicate glasses, viz., xNa2O·(20−x)K2O·80SiO2 (mol%). The network dilation coefficient of the ion-exchanged glasses is dependent on composition and ranges from 30% to 54% of the ideal value obtained from the as-melted glasses. This anomalous behavior of the network dilation coefficient is explained in terms of different local environments between sodium and potassium sites in the glass network and a two-stage relaxation process of the local potassium environment after ion exchange.
► Network dilation coefficient describes the amount of strain per unit change in alkali. ► Network dilation of ion-exchanged glass is less than that of as-melted glasses. ► Molecular dynamics simulations reveal the atomic origin of the network dilation anomaly. ► Network dilation anomaly due to K+ coordination in as-melted vs. ion-exchanged glasses. |
doi_str_mv | 10.1016/j.jnoncrysol.2011.09.034 |
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► Network dilation coefficient describes the amount of strain per unit change in alkali. ► Network dilation of ion-exchanged glass is less than that of as-melted glasses. ► Molecular dynamics simulations reveal the atomic origin of the network dilation anomaly. ► Network dilation anomaly due to K+ coordination in as-melted vs. ion-exchanged glasses.</description><identifier>ISSN: 0022-3093</identifier><identifier>EISSN: 1873-4812</identifier><identifier>DOI: 10.1016/j.jnoncrysol.2011.09.034</identifier><identifier>CODEN: JNCSBJ</identifier><language>eng</language><publisher>Oxford: Elsevier B.V</publisher><subject>Coefficients ; Computer simulation ; Condensed matter: structure, mechanical and thermal properties ; Dilation ; Disordered solids ; Exact sciences and technology ; Exchanging ; Glass ; Glasses ; Ion exchange ; Mechanical properties ; Molecular dynamics ; Networks ; Physics ; Potassium ; Silicates ; Sodium ; Structure of solids and liquids; crystallography</subject><ispartof>Journal of non-crystalline solids, 2012-01, Vol.358 (2), p.316-320</ispartof><rights>2011 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c446t-19963137dfe78ab56436051a98415fa794c6d5243e4b9ec30f1f667be548ceac3</citedby><cites>FETCH-LOGICAL-c446t-19963137dfe78ab56436051a98415fa794c6d5243e4b9ec30f1f667be548ceac3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jnoncrysol.2011.09.034$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=25298978$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Tandia, Adama</creatorcontrib><creatorcontrib>Vargheese, K. Deenamma</creatorcontrib><creatorcontrib>Mauro, John C.</creatorcontrib><creatorcontrib>Varshneya, Arun K.</creatorcontrib><title>Atomistic understanding of the network dilation anomaly in ion-exchanged glass</title><title>Journal of non-crystalline solids</title><description>Chemically strengthened glasses are of increasing technological importance for personal electronic devices, tablet computers, and a variety of other applications. However, there are many unexplained phenomena associated with the physics of the ion exchange process used for strengthening. One of the most puzzling of these is the anomalous behavior of the network dilation coefficient, i.e., the parameter governing the amount of linear strain of the glass per unit of alkali ions exchanged, which is inevitably a factor of 2–4 higher for as-melted glasses as compared to chemically strengthened versions of the same glass compositions prepared via ion exchange. In this paper, we investigate the atomistic origin of this discrepancy between as-melted and ion-exchanged glasses based on molecular dynamics simulations of a series of alkali tetrasilicate glasses, viz., xNa2O·(20−x)K2O·80SiO2 (mol%). The network dilation coefficient of the ion-exchanged glasses is dependent on composition and ranges from 30% to 54% of the ideal value obtained from the as-melted glasses. This anomalous behavior of the network dilation coefficient is explained in terms of different local environments between sodium and potassium sites in the glass network and a two-stage relaxation process of the local potassium environment after ion exchange.
► Network dilation coefficient describes the amount of strain per unit change in alkali. ► Network dilation of ion-exchanged glass is less than that of as-melted glasses. ► Molecular dynamics simulations reveal the atomic origin of the network dilation anomaly. ► Network dilation anomaly due to K+ coordination in as-melted vs. ion-exchanged glasses.</description><subject>Coefficients</subject><subject>Computer simulation</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Dilation</subject><subject>Disordered solids</subject><subject>Exact sciences and technology</subject><subject>Exchanging</subject><subject>Glass</subject><subject>Glasses</subject><subject>Ion exchange</subject><subject>Mechanical properties</subject><subject>Molecular dynamics</subject><subject>Networks</subject><subject>Physics</subject><subject>Potassium</subject><subject>Silicates</subject><subject>Sodium</subject><subject>Structure of solids and liquids; crystallography</subject><issn>0022-3093</issn><issn>1873-4812</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqFkE9PAyEQxYnRxFr9DlyMp11hYXfhWBv_JY1e9EwoO9tSt1CBqv320tTo0blMJnnvTd4PIUxJSQltrlflynlnwi76oawIpSWRJWH8CI2oaFnBBa2O0YiQqioYkewUncW4InlaJkboaZL82sZkDd66DkJM2nXWLbDvcVoCdpA-fXjDnR10st5h7fxaDztsHc5nAV9mqd0COrwYdIzn6KTXQ4SLnz1Gr3e3L9OHYvZ8_zidzArDeZMKKmXDKGu7Hlqh53XDWUNqqqXgtO51K7lpurriDPhcgmGkp33TtHOouTCgDRujq0PuJvj3LcSkcgkDw6Ad-G1UOV4SzinPSnFQmuBjDNCrTbBrHXaKErUnqFbqj6DaE1REqkwwWy9_nuho9NAH7YyNv_6qrqSQrci6m4MOcuMPC0FFY8EZ6GwAk1Tn7f_PvgFz_o0q</recordid><startdate>20120115</startdate><enddate>20120115</enddate><creator>Tandia, Adama</creator><creator>Vargheese, K. 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Deenamma ; Mauro, John C. ; Varshneya, Arun K.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c446t-19963137dfe78ab56436051a98415fa794c6d5243e4b9ec30f1f667be548ceac3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Coefficients</topic><topic>Computer simulation</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Dilation</topic><topic>Disordered solids</topic><topic>Exact sciences and technology</topic><topic>Exchanging</topic><topic>Glass</topic><topic>Glasses</topic><topic>Ion exchange</topic><topic>Mechanical properties</topic><topic>Molecular dynamics</topic><topic>Networks</topic><topic>Physics</topic><topic>Potassium</topic><topic>Silicates</topic><topic>Sodium</topic><topic>Structure of solids and liquids; crystallography</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tandia, Adama</creatorcontrib><creatorcontrib>Vargheese, K. Deenamma</creatorcontrib><creatorcontrib>Mauro, John C.</creatorcontrib><creatorcontrib>Varshneya, Arun K.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Ceramic Abstracts</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>Journal of non-crystalline solids</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tandia, Adama</au><au>Vargheese, K. Deenamma</au><au>Mauro, John C.</au><au>Varshneya, Arun K.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Atomistic understanding of the network dilation anomaly in ion-exchanged glass</atitle><jtitle>Journal of non-crystalline solids</jtitle><date>2012-01-15</date><risdate>2012</risdate><volume>358</volume><issue>2</issue><spage>316</spage><epage>320</epage><pages>316-320</pages><issn>0022-3093</issn><eissn>1873-4812</eissn><coden>JNCSBJ</coden><abstract>Chemically strengthened glasses are of increasing technological importance for personal electronic devices, tablet computers, and a variety of other applications. However, there are many unexplained phenomena associated with the physics of the ion exchange process used for strengthening. One of the most puzzling of these is the anomalous behavior of the network dilation coefficient, i.e., the parameter governing the amount of linear strain of the glass per unit of alkali ions exchanged, which is inevitably a factor of 2–4 higher for as-melted glasses as compared to chemically strengthened versions of the same glass compositions prepared via ion exchange. In this paper, we investigate the atomistic origin of this discrepancy between as-melted and ion-exchanged glasses based on molecular dynamics simulations of a series of alkali tetrasilicate glasses, viz., xNa2O·(20−x)K2O·80SiO2 (mol%). The network dilation coefficient of the ion-exchanged glasses is dependent on composition and ranges from 30% to 54% of the ideal value obtained from the as-melted glasses. This anomalous behavior of the network dilation coefficient is explained in terms of different local environments between sodium and potassium sites in the glass network and a two-stage relaxation process of the local potassium environment after ion exchange.
► Network dilation coefficient describes the amount of strain per unit change in alkali. ► Network dilation of ion-exchanged glass is less than that of as-melted glasses. ► Molecular dynamics simulations reveal the atomic origin of the network dilation anomaly. ► Network dilation anomaly due to K+ coordination in as-melted vs. ion-exchanged glasses.</abstract><cop>Oxford</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jnoncrysol.2011.09.034</doi><tpages>5</tpages></addata></record> |
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subjects | Coefficients Computer simulation Condensed matter: structure, mechanical and thermal properties Dilation Disordered solids Exact sciences and technology Exchanging Glass Glasses Ion exchange Mechanical properties Molecular dynamics Networks Physics Potassium Silicates Sodium Structure of solids and liquids crystallography |
title | Atomistic understanding of the network dilation anomaly in ion-exchanged glass |
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