Is It not Time to Go back to Tamman’s Tg?
Based on the analysis of numerous experimental data, it is shown that the currently generally accepted glass transition temperature T g is not correct. It was the result of borrowing from G. Tamman the symbol T g , which corresponds to the temperature at which a liquid in a viscous flow is transform...
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Veröffentlicht in: | Russian microelectronics 2017-12, Vol.46 (8), p.612-621 |
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creator | Minaev, V. S. Parfenov, N. M. Timoshenkov, S. P. Vassiliev, V. P. Kalugin, V. V. Mukimov, D. Zh |
description | Based on the analysis of numerous experimental data, it is shown that the currently generally accepted glass transition temperature
T
g
is not correct. It was the result of borrowing from G. Tamman the symbol
T
g
, which corresponds to the temperature at which a liquid in a viscous flow is transformed into a solid brittle glassy state, and using it instead of the symbol Tw. The latter corresponded to the bending temperature (for Tamman) on the property–temperature curve of glass-forming substances lying above Tamman’s
T
g
. The disclosed physico-chemical nature of the temperature curve Tw (currently, generally taken to be
T
g
), which is the temperature of the reverse direction of the interconversion of nanofragment patterns (of polymorphs) of the high- and low-temperature polymorphs that coexist in a vitreous substance, is based on the application of polymer-polymorphing representations of the structure of glass-forming substances. In the past few decades, the discovery of the preendothermal effect located, just as Tamman’s
T
g
, below the standard
T
g
, confirms the correctness of Tamman’s
T
g
characterized by the increased specific heat of the heated glass. |
doi_str_mv | 10.1134/S1063739717080121 |
format | Article |
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T
g
is not correct. It was the result of borrowing from G. Tamman the symbol
T
g
, which corresponds to the temperature at which a liquid in a viscous flow is transformed into a solid brittle glassy state, and using it instead of the symbol Tw. The latter corresponded to the bending temperature (for Tamman) on the property–temperature curve of glass-forming substances lying above Tamman’s
T
g
. The disclosed physico-chemical nature of the temperature curve Tw (currently, generally taken to be
T
g
), which is the temperature of the reverse direction of the interconversion of nanofragment patterns (of polymorphs) of the high- and low-temperature polymorphs that coexist in a vitreous substance, is based on the application of polymer-polymorphing representations of the structure of glass-forming substances. In the past few decades, the discovery of the preendothermal effect located, just as Tamman’s
T
g
, below the standard
T
g
, confirms the correctness of Tamman’s
T
g
characterized by the increased specific heat of the heated glass.</description><identifier>ISSN: 1063-7397</identifier><identifier>EISSN: 1608-3415</identifier><identifier>DOI: 10.1134/S1063739717080121</identifier><language>eng</language><publisher>Moscow: Pleiades Publishing</publisher><subject>Electrical Engineering ; Engineering</subject><ispartof>Russian microelectronics, 2017-12, Vol.46 (8), p.612-621</ispartof><rights>Pleiades Publishing, Ltd. 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c851-d6f67008396e0ea65fdf061d1a180202e1f458f41e6175128c4dc3563de875b83</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1134/S1063739717080121$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1134/S1063739717080121$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27923,27924,41487,42556,51318</link.rule.ids></links><search><creatorcontrib>Minaev, V. S.</creatorcontrib><creatorcontrib>Parfenov, N. M.</creatorcontrib><creatorcontrib>Timoshenkov, S. P.</creatorcontrib><creatorcontrib>Vassiliev, V. P.</creatorcontrib><creatorcontrib>Kalugin, V. V.</creatorcontrib><creatorcontrib>Mukimov, D. Zh</creatorcontrib><title>Is It not Time to Go back to Tamman’s Tg?</title><title>Russian microelectronics</title><addtitle>Russ Microelectron</addtitle><description>Based on the analysis of numerous experimental data, it is shown that the currently generally accepted glass transition temperature
T
g
is not correct. It was the result of borrowing from G. Tamman the symbol
T
g
, which corresponds to the temperature at which a liquid in a viscous flow is transformed into a solid brittle glassy state, and using it instead of the symbol Tw. The latter corresponded to the bending temperature (for Tamman) on the property–temperature curve of glass-forming substances lying above Tamman’s
T
g
. The disclosed physico-chemical nature of the temperature curve Tw (currently, generally taken to be
T
g
), which is the temperature of the reverse direction of the interconversion of nanofragment patterns (of polymorphs) of the high- and low-temperature polymorphs that coexist in a vitreous substance, is based on the application of polymer-polymorphing representations of the structure of glass-forming substances. In the past few decades, the discovery of the preendothermal effect located, just as Tamman’s
T
g
, below the standard
T
g
, confirms the correctness of Tamman’s
T
g
characterized by the increased specific heat of the heated glass.</description><subject>Electrical Engineering</subject><subject>Engineering</subject><issn>1063-7397</issn><issn>1608-3415</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp9j8FOwzAQRC0EEqXwAdx8R4FdO167J4QqKJEqcSD3yHXsqoXEyA4HbvwGv8eXkKjckDjNSLNvNcPYJcI1oixvnhFIarnQqMEACjxiMyQwhSxRHY9-jIspP2VnOe8BEIBoxq6qzKuB93Hg9a7zfIh8FfnGupfJ1rbrbP_9-ZV5vb09ZyfBvmZ_8atzVj_c18vHYv20qpZ368IZhUVLgTSAkQvy4C2p0AYgbNGiAQHCYyiVCSV6Qq1QGFe2TiqSrTdabYycMzy8dSnmnHxo3tKus-mjQWimsc2fsSMjDkweb_utT80-vqd-bPkP9ANnZlNP</recordid><startdate>201712</startdate><enddate>201712</enddate><creator>Minaev, V. S.</creator><creator>Parfenov, N. M.</creator><creator>Timoshenkov, S. P.</creator><creator>Vassiliev, V. P.</creator><creator>Kalugin, V. V.</creator><creator>Mukimov, D. Zh</creator><general>Pleiades Publishing</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>201712</creationdate><title>Is It not Time to Go back to Tamman’s Tg?</title><author>Minaev, V. S. ; Parfenov, N. M. ; Timoshenkov, S. P. ; Vassiliev, V. P. ; Kalugin, V. V. ; Mukimov, D. Zh</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c851-d6f67008396e0ea65fdf061d1a180202e1f458f41e6175128c4dc3563de875b83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Electrical Engineering</topic><topic>Engineering</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Minaev, V. S.</creatorcontrib><creatorcontrib>Parfenov, N. M.</creatorcontrib><creatorcontrib>Timoshenkov, S. P.</creatorcontrib><creatorcontrib>Vassiliev, V. P.</creatorcontrib><creatorcontrib>Kalugin, V. V.</creatorcontrib><creatorcontrib>Mukimov, D. Zh</creatorcontrib><collection>CrossRef</collection><jtitle>Russian microelectronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Minaev, V. S.</au><au>Parfenov, N. M.</au><au>Timoshenkov, S. P.</au><au>Vassiliev, V. P.</au><au>Kalugin, V. V.</au><au>Mukimov, D. Zh</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Is It not Time to Go back to Tamman’s Tg?</atitle><jtitle>Russian microelectronics</jtitle><stitle>Russ Microelectron</stitle><date>2017-12</date><risdate>2017</risdate><volume>46</volume><issue>8</issue><spage>612</spage><epage>621</epage><pages>612-621</pages><issn>1063-7397</issn><eissn>1608-3415</eissn><abstract>Based on the analysis of numerous experimental data, it is shown that the currently generally accepted glass transition temperature
T
g
is not correct. It was the result of borrowing from G. Tamman the symbol
T
g
, which corresponds to the temperature at which a liquid in a viscous flow is transformed into a solid brittle glassy state, and using it instead of the symbol Tw. The latter corresponded to the bending temperature (for Tamman) on the property–temperature curve of glass-forming substances lying above Tamman’s
T
g
. The disclosed physico-chemical nature of the temperature curve Tw (currently, generally taken to be
T
g
), which is the temperature of the reverse direction of the interconversion of nanofragment patterns (of polymorphs) of the high- and low-temperature polymorphs that coexist in a vitreous substance, is based on the application of polymer-polymorphing representations of the structure of glass-forming substances. In the past few decades, the discovery of the preendothermal effect located, just as Tamman’s
T
g
, below the standard
T
g
, confirms the correctness of Tamman’s
T
g
characterized by the increased specific heat of the heated glass.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S1063739717080121</doi><tpages>10</tpages></addata></record> |
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language | eng |
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source | Springer journals |
subjects | Electrical Engineering Engineering |
title | Is It not Time to Go back to Tamman’s Tg? |
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