Revealing the rich dynamics of glass-forming systems by modification of composition and change of thermodynamic conditions
Secondary relaxations have been classified into two types, depending on whether they are related to the structural α-relaxation in properties or not. Those secondary relaxations that are related to the α-relaxation may have fundamental importance, and are called the Johari–Goldstein (JG) β-relaxatio...
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Veröffentlicht in: | Journal of non-crystalline solids 2015-01, Vol.407, p.98-105 |
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description | Secondary relaxations have been classified into two types, depending on whether they are related to the structural α-relaxation in properties or not. Those secondary relaxations that are related to the α-relaxation may have fundamental importance, and are called the Johari–Goldstein (JG) β-relaxations. Two polar molecular glass-formers, one flexible and another rigid, dissolved in apolar host with higher glass transition temperature are studied by broadband dielectric spectroscopy at ambient and elevated pressure. The neat flexible glass-former diethylphthalate (DEP) has a resolved secondary relaxation which, unlike the α-relaxation, is insensitive to pressure and hence is not the JG β-relaxation. In the solution, the JG β-relaxation of DEP shows up in experiment and its relaxation time τβ is pressure and temperature dependent like τα. The result supports the universal presence of the JG β-relaxation in all glass-formers, and the separation between τα and τβ is determined by intermolecular interaction. The rigid glass-former is cyano-benzene (CNBz) and its secondary relaxation involves the entire molecule is necessarily the JG β-relaxation. The dielectric relaxation spectra obtained at a number of combinations of pressure and temperature at constant τα show not only unchanged is the frequency dispersion of the α-relaxation but also τβ. The remarkable results indicate that the JG β-relaxation bears a strong connection to the α-relaxation, and the two relaxations are inseparable when considering the dynamics of glass-forming systems. Experimentally, τα has been found to be a function of the product variables, T/ργ, where ρ is the density and γ is a material constant. From the \invariance of the ratio, τα/τβ, to change of thermodynamic conditions seen in our experiment as well in other systems, it follows that τβ is also a function of T/ργ, with the same γ at least approximately. Since the JG β-relaxation is the precursor of the α-relaxation, causality implies that the T/ργ-dependence originates from the JG β-relaxation and is passed on to the α-relaxation.
•Dielectric spectra of polar molecules in apolar matrices show secondary processes.•Pressure experiments reveal the intermolecular character of JG β-relaxation.•Coupling Model can rationalize the connection between JG β- and α-relaxation. |
doi_str_mv | 10.1016/j.jnoncrysol.2014.10.025 |
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•Dielectric spectra of polar molecules in apolar matrices show secondary processes.•Pressure experiments reveal the intermolecular character of JG β-relaxation.•Coupling Model can rationalize the connection between JG β- and α-relaxation.</description><identifier>ISSN: 0022-3093</identifier><identifier>EISSN: 1873-4812</identifier><identifier>DOI: 10.1016/j.jnoncrysol.2014.10.025</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Binary mixtures ; Broadband ; Constants ; Density ; Dynamical systems ; Dynamics ; Glass formation ; Glass transition ; Intermolecular relaxation ; Pressure ; Relaxation time ; Secondary relaxation ; Thermodynamics</subject><ispartof>Journal of non-crystalline solids, 2015-01, Vol.407, p.98-105</ispartof><rights>2014 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c487t-3fea094156da5b81c5c0249899702ee89b1e88ed0f66c0cf578538e3f8738833</citedby><cites>FETCH-LOGICAL-c487t-3fea094156da5b81c5c0249899702ee89b1e88ed0f66c0cf578538e3f8738833</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0022309314005456$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27903,27904,65309</link.rule.ids></links><search><creatorcontrib>Shahin Thayyil, M.</creatorcontrib><creatorcontrib>Ngai, K.L.</creatorcontrib><creatorcontrib>Prevosto, D.</creatorcontrib><creatorcontrib>Capaccioli, S.</creatorcontrib><title>Revealing the rich dynamics of glass-forming systems by modification of composition and change of thermodynamic conditions</title><title>Journal of non-crystalline solids</title><description>Secondary relaxations have been classified into two types, depending on whether they are related to the structural α-relaxation in properties or not. Those secondary relaxations that are related to the α-relaxation may have fundamental importance, and are called the Johari–Goldstein (JG) β-relaxations. Two polar molecular glass-formers, one flexible and another rigid, dissolved in apolar host with higher glass transition temperature are studied by broadband dielectric spectroscopy at ambient and elevated pressure. The neat flexible glass-former diethylphthalate (DEP) has a resolved secondary relaxation which, unlike the α-relaxation, is insensitive to pressure and hence is not the JG β-relaxation. In the solution, the JG β-relaxation of DEP shows up in experiment and its relaxation time τβ is pressure and temperature dependent like τα. The result supports the universal presence of the JG β-relaxation in all glass-formers, and the separation between τα and τβ is determined by intermolecular interaction. The rigid glass-former is cyano-benzene (CNBz) and its secondary relaxation involves the entire molecule is necessarily the JG β-relaxation. The dielectric relaxation spectra obtained at a number of combinations of pressure and temperature at constant τα show not only unchanged is the frequency dispersion of the α-relaxation but also τβ. The remarkable results indicate that the JG β-relaxation bears a strong connection to the α-relaxation, and the two relaxations are inseparable when considering the dynamics of glass-forming systems. Experimentally, τα has been found to be a function of the product variables, T/ργ, where ρ is the density and γ is a material constant. From the \invariance of the ratio, τα/τβ, to change of thermodynamic conditions seen in our experiment as well in other systems, it follows that τβ is also a function of T/ργ, with the same γ at least approximately. Since the JG β-relaxation is the precursor of the α-relaxation, causality implies that the T/ργ-dependence originates from the JG β-relaxation and is passed on to the α-relaxation.
•Dielectric spectra of polar molecules in apolar matrices show secondary processes.•Pressure experiments reveal the intermolecular character of JG β-relaxation.•Coupling Model can rationalize the connection between JG β- and α-relaxation.</description><subject>Binary mixtures</subject><subject>Broadband</subject><subject>Constants</subject><subject>Density</subject><subject>Dynamical systems</subject><subject>Dynamics</subject><subject>Glass formation</subject><subject>Glass transition</subject><subject>Intermolecular relaxation</subject><subject>Pressure</subject><subject>Relaxation time</subject><subject>Secondary relaxation</subject><subject>Thermodynamics</subject><issn>0022-3093</issn><issn>1873-4812</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqNkU1LBDEMhosouH78hx69zNpO56M9qvgFgiDeS7eT7naZaddmFMZfb8cVPGouIcmTF5KXEMrZkjPeXG6X2xCDTRPGflkyXuX2kpX1AVlw2Yqikrw8JAvGyrIQTIljcoK4ZTlaIRfk8wU-wPQ-rOm4AZq83dBuCmbwFml0dN0bxMLFNMwITjjCgHQ10SF23nlrRh_DDNo47CL679KEjtqNCWuYJ1k3ZXovmrnQfVN4Ro6c6RHOf_Ipeb27fb15KJ6e7x9vrp4KW8l2LIQDw1TF66Yz9UpyW1tWVkoq1bISQKoVBymhY65pLLOubmUtJAiXr5dSiFNysZfdpfj2DjjqwaOFvjcB4jtq3qhKtVUpm3-gTX5bI6TKqNyjNkXEBE7vkh9MmjRnejZGb_WvMXo2Zp5kY_Lq9X4V8tEfHpJG6yFY6HwCO-ou-r9FvgD9CJ6p</recordid><startdate>20150101</startdate><enddate>20150101</enddate><creator>Shahin Thayyil, M.</creator><creator>Ngai, K.L.</creator><creator>Prevosto, D.</creator><creator>Capaccioli, S.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7TN</scope><scope>F1W</scope><scope>H95</scope><scope>L.G</scope></search><sort><creationdate>20150101</creationdate><title>Revealing the rich dynamics of glass-forming systems by modification of composition and change of thermodynamic conditions</title><author>Shahin Thayyil, M. ; Ngai, K.L. ; Prevosto, D. ; Capaccioli, S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c487t-3fea094156da5b81c5c0249899702ee89b1e88ed0f66c0cf578538e3f8738833</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Binary mixtures</topic><topic>Broadband</topic><topic>Constants</topic><topic>Density</topic><topic>Dynamical systems</topic><topic>Dynamics</topic><topic>Glass formation</topic><topic>Glass transition</topic><topic>Intermolecular relaxation</topic><topic>Pressure</topic><topic>Relaxation time</topic><topic>Secondary relaxation</topic><topic>Thermodynamics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shahin Thayyil, M.</creatorcontrib><creatorcontrib>Ngai, K.L.</creatorcontrib><creatorcontrib>Prevosto, D.</creatorcontrib><creatorcontrib>Capaccioli, S.</creatorcontrib><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><collection>Oceanic Abstracts</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 1: Biological Sciences & Living Resources</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><jtitle>Journal of non-crystalline solids</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shahin Thayyil, M.</au><au>Ngai, K.L.</au><au>Prevosto, D.</au><au>Capaccioli, S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Revealing the rich dynamics of glass-forming systems by modification of composition and change of thermodynamic conditions</atitle><jtitle>Journal of non-crystalline solids</jtitle><date>2015-01-01</date><risdate>2015</risdate><volume>407</volume><spage>98</spage><epage>105</epage><pages>98-105</pages><issn>0022-3093</issn><eissn>1873-4812</eissn><abstract>Secondary relaxations have been classified into two types, depending on whether they are related to the structural α-relaxation in properties or not. Those secondary relaxations that are related to the α-relaxation may have fundamental importance, and are called the Johari–Goldstein (JG) β-relaxations. Two polar molecular glass-formers, one flexible and another rigid, dissolved in apolar host with higher glass transition temperature are studied by broadband dielectric spectroscopy at ambient and elevated pressure. The neat flexible glass-former diethylphthalate (DEP) has a resolved secondary relaxation which, unlike the α-relaxation, is insensitive to pressure and hence is not the JG β-relaxation. In the solution, the JG β-relaxation of DEP shows up in experiment and its relaxation time τβ is pressure and temperature dependent like τα. The result supports the universal presence of the JG β-relaxation in all glass-formers, and the separation between τα and τβ is determined by intermolecular interaction. The rigid glass-former is cyano-benzene (CNBz) and its secondary relaxation involves the entire molecule is necessarily the JG β-relaxation. The dielectric relaxation spectra obtained at a number of combinations of pressure and temperature at constant τα show not only unchanged is the frequency dispersion of the α-relaxation but also τβ. The remarkable results indicate that the JG β-relaxation bears a strong connection to the α-relaxation, and the two relaxations are inseparable when considering the dynamics of glass-forming systems. Experimentally, τα has been found to be a function of the product variables, T/ργ, where ρ is the density and γ is a material constant. From the \invariance of the ratio, τα/τβ, to change of thermodynamic conditions seen in our experiment as well in other systems, it follows that τβ is also a function of T/ργ, with the same γ at least approximately. Since the JG β-relaxation is the precursor of the α-relaxation, causality implies that the T/ργ-dependence originates from the JG β-relaxation and is passed on to the α-relaxation.
•Dielectric spectra of polar molecules in apolar matrices show secondary processes.•Pressure experiments reveal the intermolecular character of JG β-relaxation.•Coupling Model can rationalize the connection between JG β- and α-relaxation.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.jnoncrysol.2014.10.025</doi><tpages>8</tpages></addata></record> |
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subjects | Binary mixtures Broadband Constants Density Dynamical systems Dynamics Glass formation Glass transition Intermolecular relaxation Pressure Relaxation time Secondary relaxation Thermodynamics |
title | Revealing the rich dynamics of glass-forming systems by modification of composition and change of thermodynamic conditions |
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