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Glass transition - Wikipedia

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<span class="vector-toc-numb">2</span> <span>Formal definitions</span> </div> </a> <ul id="toc-Formal_definitions-sublist" class="vector-toc-list"> </ul> </li> <li id="toc-Transition_temperature_Tg" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#Transition_temperature_Tg"> <div class="vector-toc-text"> <span class="vector-toc-numb">3</span> <span>Transition temperature <i>T</i><sub>g</sub></span> </div> </a> <button aria-controls="toc-Transition_temperature_Tg-sublist" class="cdx-button cdx-button--weight-quiet cdx-button--icon-only vector-toc-toggle"> <span class="vector-icon mw-ui-icon-wikimedia-expand"></span> <span>Toggle Transition temperature <i>T</i><sub>g</sub> subsection</span> </button> <ul id="toc-Transition_temperature_Tg-sublist" class="vector-toc-list"> <li id="toc-Polymers" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Polymers"> <div class="vector-toc-text"> <span class="vector-toc-numb">3.1</span> <span>Polymers</span> </div> </a> <ul id="toc-Polymers-sublist" class="vector-toc-list"> </ul> </li> <li id="toc-Silicates_and_other_covalent_network_glasses" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Silicates_and_other_covalent_network_glasses"> <div class="vector-toc-text"> <span class="vector-toc-numb">3.2</span> <span>Silicates and other covalent network glasses</span> </div> </a> <ul id="toc-Silicates_and_other_covalent_network_glasses-sublist" class="vector-toc-list"> </ul> </li> </ul> </li> <li id="toc-Linear_heat_capacity" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#Linear_heat_capacity"> <div class="vector-toc-text"> <span class="vector-toc-numb">4</span> <span>Linear heat capacity</span> </div> </a> <button aria-controls="toc-Linear_heat_capacity-sublist" class="cdx-button cdx-button--weight-quiet cdx-button--icon-only vector-toc-toggle"> <span class="vector-icon mw-ui-icon-wikimedia-expand"></span> <span>Toggle Linear heat capacity subsection</span> </button> <ul id="toc-Linear_heat_capacity-sublist" class="vector-toc-list"> <li id="toc-Experimental_data" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Experimental_data"> <div class="vector-toc-text"> <span class="vector-toc-numb">4.1</span> <span>Experimental data</span> </div> </a> <ul id="toc-Experimental_data-sublist" class="vector-toc-list"> </ul> </li> </ul> </li> <li id="toc-Kauzmann&#039;s_paradox" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#Kauzmann&#039;s_paradox"> <div class="vector-toc-text"> <span class="vector-toc-numb">5</span> <span>Kauzmann's paradox</span> </div> </a> <button aria-controls="toc-Kauzmann&#039;s_paradox-sublist" class="cdx-button cdx-button--weight-quiet cdx-button--icon-only vector-toc-toggle"> <span class="vector-icon mw-ui-icon-wikimedia-expand"></span> <span>Toggle Kauzmann's paradox subsection</span> </button> <ul id="toc-Kauzmann&#039;s_paradox-sublist" class="vector-toc-list"> <li id="toc-Possible_resolutions" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Possible_resolutions"> <div class="vector-toc-text"> <span class="vector-toc-numb">5.1</span> <span>Possible resolutions</span> </div> </a> <ul id="toc-Possible_resolutions-sublist" class="vector-toc-list"> </ul> </li> </ul> </li> <li id="toc-In_specific_materials" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#In_specific_materials"> <div class="vector-toc-text"> <span class="vector-toc-numb">6</span> <span>In specific materials</span> </div> </a> <button aria-controls="toc-In_specific_materials-sublist" class="cdx-button cdx-button--weight-quiet cdx-button--icon-only vector-toc-toggle"> <span class="vector-icon mw-ui-icon-wikimedia-expand"></span> <span>Toggle In specific materials subsection</span> </button> <ul id="toc-In_specific_materials-sublist" class="vector-toc-list"> <li id="toc-Silica,_SiO2" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Silica,_SiO2"> <div class="vector-toc-text"> <span class="vector-toc-numb">6.1</span> <span>Silica, SiO<sub>2</sub></span> </div> </a> <ul id="toc-Silica,_SiO2-sublist" class="vector-toc-list"> </ul> </li> <li id="toc-Polymers_2" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Polymers_2"> <div class="vector-toc-text"> <span class="vector-toc-numb">6.2</span> <span>Polymers</span> </div> </a> <ul id="toc-Polymers_2-sublist" class="vector-toc-list"> </ul> </li> </ul> </li> <li id="toc-Mechanics_of_vitrification" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#Mechanics_of_vitrification"> <div class="vector-toc-text"> <span class="vector-toc-numb">7</span> <span>Mechanics of vitrification</span> </div> </a> <button aria-controls="toc-Mechanics_of_vitrification-sublist" class="cdx-button cdx-button--weight-quiet cdx-button--icon-only vector-toc-toggle"> <span class="vector-icon mw-ui-icon-wikimedia-expand"></span> <span>Toggle Mechanics of vitrification subsection</span> </button> <ul id="toc-Mechanics_of_vitrification-sublist" class="vector-toc-list"> <li id="toc-Electronic_structure" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#Electronic_structure"> <div class="vector-toc-text"> <span class="vector-toc-numb">7.1</span> <span>Electronic structure</span> </div> </a> <ul id="toc-Electronic_structure-sublist" class="vector-toc-list"> </ul> </li> </ul> </li> <li id="toc-See_also" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#See_also"> <div class="vector-toc-text"> <span class="vector-toc-numb">8</span> <span>See also</span> </div> </a> <ul id="toc-See_also-sublist" class="vector-toc-list"> </ul> </li> <li id="toc-References" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#References"> <div class="vector-toc-text"> <span class="vector-toc-numb">9</span> <span>References</span> </div> </a> <ul id="toc-References-sublist" class="vector-toc-list"> </ul> </li> <li id="toc-External_links" class="vector-toc-list-item vector-toc-level-1 vector-toc-list-item-expanded"> <a class="vector-toc-link" href="#External_links"> <div class="vector-toc-text"> <span class="vector-toc-numb">10</span> <span>External links</span> </div> </a> <ul id="toc-External_links-sublist" class="vector-toc-list"> </ul> </li> </ul> </div> </div> </nav> </div> </div> <div class="mw-content-container"> <main id="content" class="mw-body"> <header class="mw-body-header vector-page-titlebar"> <nav aria-label="Contents" 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href="https://de.wikipedia.org/wiki/Glas%C3%BCbergang" title="Glasübergang – German" lang="de" hreflang="de" data-title="Glasübergang" data-language-autonym="Deutsch" data-language-local-name="German" class="interlanguage-link-target"><span>Deutsch</span></a></li><li class="interlanguage-link interwiki-el mw-list-item"><a href="https://el.wikipedia.org/wiki/%CE%A5%CE%B1%CE%BB%CF%8E%CE%B4%CE%B7%CF%82_%CE%BC%CE%B5%CF%84%CE%AC%CF%80%CF%84%CF%89%CF%83%CE%B7" title="Υαλώδης μετάπτωση – Greek" lang="el" hreflang="el" data-title="Υαλώδης μετάπτωση" data-language-autonym="Ελληνικά" data-language-local-name="Greek" class="interlanguage-link-target"><span>Ελληνικά</span></a></li><li class="interlanguage-link interwiki-es mw-list-item"><a href="https://es.wikipedia.org/wiki/Transici%C3%B3n_V%C3%ADtrea" title="Transición Vítrea – Spanish" lang="es" hreflang="es" data-title="Transición Vítrea" data-language-autonym="Español" data-language-local-name="Spanish" class="interlanguage-link-target"><span>Español</span></a></li><li class="interlanguage-link interwiki-fa mw-list-item"><a href="https://fa.wikipedia.org/wiki/%D8%AF%D9%85%D8%A7%DB%8C_%D8%A7%D9%86%D8%AA%D9%82%D8%A7%D9%84_%D8%B4%DB%8C%D8%B4%D9%87" title="دمای انتقال شیشه – Persian" lang="fa" hreflang="fa" data-title="دمای انتقال شیشه" data-language-autonym="فارسی" data-language-local-name="Persian" class="interlanguage-link-target"><span>فارسی</span></a></li><li class="interlanguage-link interwiki-fr mw-list-item"><a href="https://fr.wikipedia.org/wiki/Transition_vitreuse" title="Transition vitreuse – French" lang="fr" hreflang="fr" data-title="Transition vitreuse" data-language-autonym="Français" data-language-local-name="French" class="interlanguage-link-target"><span>Français</span></a></li><li class="interlanguage-link interwiki-ko mw-list-item"><a href="https://ko.wikipedia.org/wiki/%EC%9C%A0%EB%A6%AC_%EC%A0%84%EC%9D%B4" title="유리 전이 – Korean" lang="ko" hreflang="ko" data-title="유리 전이" data-language-autonym="한국어" data-language-local-name="Korean" class="interlanguage-link-target"><span>한국어</span></a></li><li class="interlanguage-link interwiki-hi mw-list-item"><a href="https://hi.wikipedia.org/wiki/%E0%A4%95%E0%A4%BE%E0%A4%9A_%E0%A4%B8%E0%A4%82%E0%A4%95%E0%A5%8D%E0%A4%B0%E0%A4%AE%E0%A4%A3" title="काच संक्रमण – Hindi" lang="hi" hreflang="hi" data-title="काच संक्रमण" data-language-autonym="हिन्दी" data-language-local-name="Hindi" class="interlanguage-link-target"><span>हिन्दी</span></a></li><li class="interlanguage-link interwiki-he mw-list-item"><a href="https://he.wikipedia.org/wiki/%D7%98%D7%9E%D7%A4%D7%A8%D7%98%D7%95%D7%A8%D7%AA_%D7%9E%D7%A2%D7%91%D7%A8_%D7%96%D7%9B%D7%95%D7%9B%D7%99%D7%AA%D7%99" title="טמפרטורת מעבר זכוכיתי – Hebrew" lang="he" hreflang="he" data-title="טמפרטורת מעבר זכוכיתי" data-language-autonym="עברית" data-language-local-name="Hebrew" class="interlanguage-link-target"><span>עברית</span></a></li><li class="interlanguage-link interwiki-ml mw-list-item"><a href="https://ml.wikipedia.org/wiki/%E0%B4%97%E0%B5%8D%E0%B4%B2%E0%B4%BE%E0%B4%B8%E0%B5%8D%E0%B4%B8%E0%B5%8D_%E0%B4%9F%E0%B5%8D%E0%B4%B0%E0%B4%BE%E0%B5%BB%E0%B4%B8%E0%B5%80%E0%B4%B7%E0%B5%BB" title="ഗ്ലാസ്സ് ട്രാൻസീഷൻ – Malayalam" lang="ml" hreflang="ml" data-title="ഗ്ലാസ്സ് ട്രാൻസീഷൻ" data-language-autonym="മലയാളം" data-language-local-name="Malayalam" class="interlanguage-link-target"><span>മലയാളം</span></a></li><li class="interlanguage-link interwiki-nl mw-list-item"><a href="https://nl.wikipedia.org/wiki/Glasovergang" title="Glasovergang – Dutch" lang="nl" hreflang="nl" data-title="Glasovergang" data-language-autonym="Nederlands" data-language-local-name="Dutch" class="interlanguage-link-target"><span>Nederlands</span></a></li><li class="interlanguage-link interwiki-ja mw-list-item"><a href="https://ja.wikipedia.org/wiki/%E3%82%AC%E3%83%A9%E3%82%B9%E8%BB%A2%E7%A7%BB%E7%82%B9" title="ガラス転移点 – Japanese" lang="ja" hreflang="ja" data-title="ガラス転移点" 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interwiki-tr mw-list-item"><a href="https://tr.wikipedia.org/wiki/Cams%C4%B1_ge%C3%A7i%C5%9F_s%C4%B1cakl%C4%B1%C4%9F%C4%B1" title="Camsı geçiş sıcaklığı – Turkish" lang="tr" hreflang="tr" data-title="Camsı geçiş sıcaklığı" data-language-autonym="Türkçe" data-language-local-name="Turkish" class="interlanguage-link-target"><span>Türkçe</span></a></li><li class="interlanguage-link interwiki-uk mw-list-item"><a href="https://uk.wikipedia.org/wiki/%D0%92%D1%96%D1%82%D1%80%D0%B8%D1%84%D1%96%D0%BA%D0%B0%D1%86%D1%96%D1%8F" title="Вітрифікація – Ukrainian" lang="uk" hreflang="uk" data-title="Вітрифікація" data-language-autonym="Українська" data-language-local-name="Ukrainian" class="interlanguage-link-target"><span>Українська</span></a></li><li class="interlanguage-link interwiki-vi mw-list-item"><a href="https://vi.wikipedia.org/wiki/%C4%90i%E1%BB%83m_chuy%E1%BB%83n_d%E1%BB%8Bch_l%E1%BB%8Fng-r%E1%BA%AFn" title="Điểm chuyển dịch lỏng-rắn – Vietnamese" lang="vi" hreflang="vi" data-title="Điểm 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id="mw-content-subtitle"></div></div> <div id="mw-content-text" class="mw-body-content"><div class="mw-content-ltr mw-parser-output" lang="en" dir="ltr"><figure class="mw-default-size" typeof="mw:File/Thumb"><a href="/wiki/File:Two-dimensional_schematic_diagram_of_quartz,_silica,_and_silica-based_glass.png" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/5/53/Two-dimensional_schematic_diagram_of_quartz%2C_silica%2C_and_silica-based_glass.png/220px-Two-dimensional_schematic_diagram_of_quartz%2C_silica%2C_and_silica-based_glass.png" decoding="async" width="220" height="138" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/5/53/Two-dimensional_schematic_diagram_of_quartz%2C_silica%2C_and_silica-based_glass.png/330px-Two-dimensional_schematic_diagram_of_quartz%2C_silica%2C_and_silica-based_glass.png 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/5/53/Two-dimensional_schematic_diagram_of_quartz%2C_silica%2C_and_silica-based_glass.png/440px-Two-dimensional_schematic_diagram_of_quartz%2C_silica%2C_and_silica-based_glass.png 2x" data-file-width="2143" data-file-height="1344" /></a><figcaption>Two-dimensional, schematic, representation of the lattices of quartz (a), silica (b), and of silica based glasses (c).<sup id="cite_ref-1" class="reference"><a href="#cite_note-1"><span class="cite-bracket">&#91;</span>1<span class="cite-bracket">&#93;</span></a></sup></figcaption></figure> <div class="shortdescription nomobile noexcerpt noprint searchaux" style="display:none">Reversible transition in amorphous materials</div> <p>The <b>glass–liquid transition</b>, or <b>glass transition</b>, is the gradual and <a href="/wiki/Reversible_reaction" title="Reversible reaction">reversible</a> transition in <a href="/wiki/Amorphous_solid" title="Amorphous solid">amorphous</a> materials (or in amorphous regions within <a href="/wiki/Crystallinity" title="Crystallinity">semicrystalline</a> materials) from a hard and relatively brittle "glassy" state into a viscous or rubbery state as the temperature is increased.<sup id="cite_ref-iso11357-2_2-0" class="reference"><a href="#cite_note-iso11357-2-2"><span class="cite-bracket">&#91;</span>2<span class="cite-bracket">&#93;</span></a></sup> An amorphous solid that exhibits a glass transition is called a <a href="/wiki/Glass" title="Glass">glass</a>. The reverse transition, achieved by <a href="/wiki/Supercooling" title="Supercooling">supercooling</a> a <a href="/wiki/Viscous_liquid" title="Viscous liquid">viscous liquid</a> into the glass state, is called <a href="/wiki/Vitrification" title="Vitrification">vitrification</a>. </p><p>The <b>glass-transition temperature</b> <i>T</i><sub>g</sub> of a material characterizes the range of temperatures over which this glass transition occurs (as an experimental definition, typically marked as 100 s of relaxation time). It is always lower than the <a href="/wiki/Melting_point" title="Melting point">melting temperature</a>, <i>T</i><sub>m</sub>, of the crystalline state of the material, if one exists, because the glass is a higher energy state (or enthalpy at constant pressure) than the corresponding crystal. </p><p>Hard plastics like <a href="/wiki/Polystyrene" title="Polystyrene">polystyrene</a> and <a href="/wiki/Poly(methyl_methacrylate)" title="Poly(methyl methacrylate)">poly(methyl methacrylate)</a> are used well below their glass transition temperatures, i.e., when they are in their glassy state. Their <i>T</i><sub>g</sub> values are both at around 100&#160;°C (212&#160;°F). Rubber <a href="/wiki/Elastomer" title="Elastomer">elastomers</a> like <a href="/wiki/Synthetic_rubber" title="Synthetic rubber">polyisoprene</a> and <a href="/wiki/Butyl_rubber" title="Butyl rubber">polyisobutylene</a> are used above their <i>T</i><sub>g</sub>, that is, in the rubbery state, where they are soft and flexible; <a href="/wiki/Cross-link" title="Cross-link">crosslinking</a> prevents free flow of their molecules, thus endowing rubber with a set shape at room temperature (as opposed to a viscous liquid).<sup id="cite_ref-3" class="reference"><a href="#cite_note-3"><span class="cite-bracket">&#91;</span>3<span class="cite-bracket">&#93;</span></a></sup> </p><p>Despite the change in the physical properties of a material through its glass transition, the transition is not considered a <a href="/wiki/Phase_transition" title="Phase transition">phase transition</a>; rather it is a phenomenon extending over a range of temperature and defined by one of several conventions.<sup id="cite_ref-Debenedetti_4-0" class="reference"><a href="#cite_note-Debenedetti-4"><span class="cite-bracket">&#91;</span>4<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-Angell_5-0" class="reference"><a href="#cite_note-Angell-5"><span class="cite-bracket">&#91;</span>5<span class="cite-bracket">&#93;</span></a></sup> Such conventions include a constant cooling rate (20 kelvins per minute (36&#160;°F/min))<sup id="cite_ref-iso11357-2_2-1" class="reference"><a href="#cite_note-iso11357-2-2"><span class="cite-bracket">&#91;</span>2<span class="cite-bracket">&#93;</span></a></sup> and a viscosity threshold of 10<sup>12</sup> <a href="/wiki/Pa%C2%B7s" class="mw-redirect" title="Pa·s">Pa·s</a>, among others. Upon cooling or heating through this glass-transition range, the material also exhibits a smooth step in the <a href="/wiki/Thermal_expansion" title="Thermal expansion">thermal-expansion coefficient</a> and in the <a href="/wiki/Specific_heat" class="mw-redirect" title="Specific heat">specific heat</a>, with the location of these effects again being dependent on the history of the material.<sup id="cite_ref-z1_6-0" class="reference"><a href="#cite_note-z1-6"><span class="cite-bracket">&#91;</span>6<span class="cite-bracket">&#93;</span></a></sup> The question of whether some phase transition underlies the glass transition is a matter of ongoing research.<sup id="cite_ref-Debenedetti_4-1" class="reference"><a href="#cite_note-Debenedetti-4"><span class="cite-bracket">&#91;</span>4<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-Angell_5-1" class="reference"><a href="#cite_note-Angell-5"><span class="cite-bracket">&#91;</span>5<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-7" class="reference"><a href="#cite_note-7"><span class="cite-bracket">&#91;</span>7<span class="cite-bracket">&#93;</span></a></sup><sup class="noprint Inline-Template" style="white-space:nowrap;">&#91;<i><a href="/wiki/Wikipedia:Manual_of_Style/Dates_and_numbers#Chronological_items" title="Wikipedia:Manual of Style/Dates and numbers"><span title="The time period mentioned near this tag is ambiguous. (October 2020)">when?</span></a></i>&#93;</sup> </p> <style data-mw-deduplicate="TemplateStyles:r1224211176">.mw-parser-output .quotebox{background-color:#F9F9F9;border:1px solid #aaa;box-sizing:border-box;padding:10px;font-size:88%;max-width:100%}.mw-parser-output .quotebox.floatleft{margin:.5em 1.4em .8em 0}.mw-parser-output .quotebox.floatright{margin:.5em 0 .8em 1.4em}.mw-parser-output .quotebox.centered{overflow:hidden;position:relative;margin:.5em auto .8em auto}.mw-parser-output .quotebox.floatleft span,.mw-parser-output .quotebox.floatright span{font-style:inherit}.mw-parser-output .quotebox>blockquote{margin:0;padding:0;border-left:0;font-family:inherit;font-size:inherit}.mw-parser-output .quotebox-title{text-align:center;font-size:110%;font-weight:bold}.mw-parser-output .quotebox-quote>:first-child{margin-top:0}.mw-parser-output .quotebox-quote:last-child>:last-child{margin-bottom:0}.mw-parser-output .quotebox-quote.quoted:before{font-family:"Times New Roman",serif;font-weight:bold;font-size:large;color:gray;content:" “ ";vertical-align:-45%;line-height:0}.mw-parser-output .quotebox-quote.quoted:after{font-family:"Times New Roman",serif;font-weight:bold;font-size:large;color:gray;content:" ” ";line-height:0}.mw-parser-output .quotebox .left-aligned{text-align:left}.mw-parser-output .quotebox .right-aligned{text-align:right}.mw-parser-output .quotebox .center-aligned{text-align:center}.mw-parser-output .quotebox .quote-title,.mw-parser-output .quotebox .quotebox-quote{display:block}.mw-parser-output .quotebox cite{display:block;font-style:normal}@media screen and (max-width:640px){.mw-parser-output .quotebox{width:100%!important;margin:0 0 .8em!important;float:none!important}}</style><div class="quotebox pullquote floatright" style="width:30%; ;"> <div class="quotebox-title" style=""><a href="/wiki/International_Union_of_Pure_and_Applied_Chemistry" title="International Union of Pure and Applied Chemistry">IUPAC</a> definition</div> <blockquote class="quotebox-quote left-aligned" style=""> <p><b>Glass transition</b> (in polymer science): process in which a polymer melt changes on cooling to a polymer glass or a polymer glass changes on heating to a polymer melt.<sup id="cite_ref-Stefano_et_al_2011_8-0" class="reference"><a href="#cite_note-Stefano_et_al_2011-8"><span class="cite-bracket">&#91;</span>8<span class="cite-bracket">&#93;</span></a></sup> </p> <ol><li>Phenomena occurring at the glass transition of polymers are still subject to ongoing scientific investigation and debate. The glass transition presents features of a second-order transition since thermal studies often indicate that the molar Gibbs energies, molar enthalpies, and the molar volumes of the two phases, i.e., the melt and the glass, are equal, while the heat capacity and the expansivity are discontinuous. However, the glass transition is generally not regarded as a thermodynamic transition in view of the inherent difficulty in reaching equilibrium in a polymer glass or in a polymer melt at temperatures close to the glass-transition temperature.</li> <li>In the case of polymers, conformational changes of segments, typically consisting of 10–20 main-chain atoms, become infinitely slow below the glass transition temperature.</li> <li>In a partially crystalline polymer the glass transition occurs only in the amorphous parts of the material.</li> <li>The definition is different from that in ref.<sup id="cite_ref-9" class="reference"><a href="#cite_note-9"><span class="cite-bracket">&#91;</span>9<span class="cite-bracket">&#93;</span></a></sup></li> <li>The commonly used term “glass-rubber transition” for glass transition is not recommended.<sup id="cite_ref-Stefano_et_al_2011_8-1" class="reference"><a href="#cite_note-Stefano_et_al_2011-8"><span class="cite-bracket">&#91;</span>8<span class="cite-bracket">&#93;</span></a></sup></li></ol> </blockquote> </div> <meta property="mw:PageProp/toc" /> <div class="mw-heading mw-heading2"><h2 id="Characteristics">Characteristics</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=1" title="Edit section: Characteristics"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p>The glass transition of a liquid to a solid-like state may occur with either cooling or compression.<sup id="cite_ref-Hansen&amp;McDonald_10-0" class="reference"><a href="#cite_note-Hansen&amp;McDonald-10"><span class="cite-bracket">&#91;</span>10<span class="cite-bracket">&#93;</span></a></sup> The transition comprises a smooth increase in the viscosity of a material by as much as 17 <a href="/wiki/Order_of_magnitude" title="Order of magnitude">orders of magnitude</a> within a temperature range of 500 K without any pronounced change in material structure.<sup id="cite_ref-11" class="reference"><a href="#cite_note-11"><span class="cite-bracket">&#91;</span>11<span class="cite-bracket">&#93;</span></a></sup> This transition is in contrast to the <a href="/wiki/Freezing" title="Freezing">freezing</a> or <a href="/wiki/Crystallization" title="Crystallization">crystallization</a> transition, which is a first-order <a href="/wiki/Phase_transition" title="Phase transition">phase transition</a> in the <a href="/wiki/Phase_transition#Ehrenfest_classification" title="Phase transition">Ehrenfest classification</a> and involves discontinuities in thermodynamic and dynamic properties such as volume, energy, and viscosity. In many materials that normally undergo a freezing transition, rapid cooling will avoid this phase transition and instead result in a glass transition at some lower temperature. Other materials, such as many <a href="/wiki/Polymers" class="mw-redirect" title="Polymers">polymers</a>, lack a well defined crystalline state and easily form glasses, even upon very slow cooling or compression. The tendency for a material to form a glass while quenched is called glass forming ability. This ability depends on the composition of the material and can be predicted by the <a href="/wiki/Rigidity_theory_(physics)" title="Rigidity theory (physics)">rigidity theory</a>.<sup id="cite_ref-phillips1979_12-0" class="reference"><a href="#cite_note-phillips1979-12"><span class="cite-bracket">&#91;</span>12<span class="cite-bracket">&#93;</span></a></sup> </p><p>Below the transition temperature range, the glassy structure does not relax in accordance with the cooling rate used. The expansion coefficient for the glassy state is roughly equivalent to that of the crystalline solid. If slower cooling rates are used, the increased time for structural <a href="/wiki/Relaxation_(physics)" title="Relaxation (physics)">relaxation</a> (or intermolecular rearrangement) to occur may result in a higher density glass product. Similarly, by <a href="/wiki/Annealing_(glass)" title="Annealing (glass)">annealing</a> (and thus allowing for slow structural relaxation) the glass structure in time approaches an equilibrium density corresponding to the supercooled liquid at this same temperature. <i>T</i><sub>g</sub> is located at the intersection between the cooling curve (volume versus temperature) for the glassy state and the supercooled liquid.<sup id="cite_ref-CM_13-0" class="reference"><a href="#cite_note-CM-13"><span class="cite-bracket">&#91;</span>13<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-14" class="reference"><a href="#cite_note-14"><span class="cite-bracket">&#91;</span>14<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-15" class="reference"><a href="#cite_note-15"><span class="cite-bracket">&#91;</span>15<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-16" class="reference"><a href="#cite_note-16"><span class="cite-bracket">&#91;</span>16<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-17" class="reference"><a href="#cite_note-17"><span class="cite-bracket">&#91;</span>17<span class="cite-bracket">&#93;</span></a></sup> </p><p>The configuration of the glass in this temperature range changes slowly with time towards the equilibrium structure. The principle of the minimization of the <a href="/wiki/Gibbs_free_energy" title="Gibbs free energy">Gibbs free energy</a> provides the thermodynamic driving force necessary for the eventual change. At somewhat higher temperatures than <i>T</i><sub>g</sub>, the structure corresponding to equilibrium at any temperature is achieved quite rapidly. In contrast, at considerably lower temperatures, the configuration of the glass remains sensibly stable over increasingly extended periods of time. </p><p>Thus, the liquid-glass transition is not a transition between states of <a href="/wiki/Thermodynamic_equilibrium" title="Thermodynamic equilibrium">thermodynamic equilibrium</a>. It is widely believed that the true equilibrium state is always crystalline. Glass is believed to exist in a kinetically locked state, and its entropy, density, and so on, depend on the thermal history. Therefore, the glass transition is primarily a dynamic phenomenon. Time and temperature are interchangeable quantities (to some extent) when dealing with glasses, a fact often expressed in the <a href="/wiki/Time%E2%80%93temperature_superposition" title="Time–temperature superposition">time–temperature superposition</a> principle. On cooling a liquid, <i>internal degrees of freedom successively fall out of equilibrium</i>. However, there is a longstanding debate whether there is an underlying second-order phase transition in the hypothetical limit of infinitely long relaxation times.<sup class="noprint Inline-Template" style="margin-left:0.1em; white-space:nowrap;">&#91;<i><a href="/wiki/Wikipedia:Please_clarify" title="Wikipedia:Please clarify"><span title="The text near this tag may need clarification or removal of jargon. (June 2016)">clarification needed</span></a></i>&#93;</sup><sup id="cite_ref-z1_6-1" class="reference"><a href="#cite_note-z1-6"><span class="cite-bracket">&#91;</span>6<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-18" class="reference"><a href="#cite_note-18"><span class="cite-bracket">&#91;</span>18<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-19" class="reference"><a href="#cite_note-19"><span class="cite-bracket">&#91;</span>19<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-20" class="reference"><a href="#cite_note-20"><span class="cite-bracket">&#91;</span>20<span class="cite-bracket">&#93;</span></a></sup> </p><p>In a more recent model of glass transition, the glass transition temperature corresponds to the temperature at which the largest openings between the vibrating elements in the liquid matrix become smaller than the smallest cross-sections of the elements or parts of them when the temperature is decreasing. As a result of the fluctuating input of thermal energy into the liquid matrix, the harmonics of the oscillations are constantly disturbed and temporary cavities ("free volume") are created between the elements, the number and size of which depend on the temperature. The glass transition temperature <i>T</i><sub>g0</sub> defined in this way is a fixed material constant of the disordered (non-crystalline) state that is dependent only on the pressure. As a result of the increasing inertia of the molecular matrix when approaching <i>T</i><sub>g0</sub>, the setting of the thermal equilibrium is successively delayed, so that the usual measuring methods for determining the glass transition temperature in principle deliver <i>T</i><sub>g</sub> values that are too high. In principle, the slower the temperature change rate is set during the measurement, the closer the measured <i>T</i><sub>g</sub> value <i>T</i><sub>g0</sub> approaches.<sup id="cite_ref-21" class="reference"><a href="#cite_note-21"><span class="cite-bracket">&#91;</span>21<span class="cite-bracket">&#93;</span></a></sup> Techniques such as <a href="/wiki/Dynamic_mechanical_analysis" title="Dynamic mechanical analysis">dynamic mechanical analysis</a> can be used to measure the glass transition temperature.<sup id="cite_ref-22" class="reference"><a href="#cite_note-22"><span class="cite-bracket">&#91;</span>22<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading2"><h2 id="Formal_definitions">Formal definitions</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=2" title="Edit section: Formal definitions"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p>The definition of the glass and the glass transition are not settled, and many definitions have been proposed over the past century.<sup id="cite_ref-:1_23-0" class="reference"><a href="#cite_note-:1-23"><span class="cite-bracket">&#91;</span>23<span class="cite-bracket">&#93;</span></a></sup> </p><p><a href="/wiki/Francis_Simon" title="Francis Simon">Franz Simon</a>:<sup id="cite_ref-24" class="reference"><a href="#cite_note-24"><span class="cite-bracket">&#91;</span>24<span class="cite-bracket">&#93;</span></a></sup> Glass is a rigid material obtained from freezing-in a supercooled liquid in a narrow temperature range. </p><p><a href="/wiki/William_Houlder_Zachariasen" title="William Houlder Zachariasen">Zachariasen</a>:<sup id="cite_ref-25" class="reference"><a href="#cite_note-25"><span class="cite-bracket">&#91;</span>25<span class="cite-bracket">&#93;</span></a></sup> Glass is a topologically disordered network, with short range order equivalent to that in the corresponding crystal.<sup id="cite_ref-26" class="reference"><a href="#cite_note-26"><span class="cite-bracket">&#91;</span>26<span class="cite-bracket">&#93;</span></a></sup> </p><p>Glass is a "frozen liquid” (i.e., liquids where ergodicity has been broken), which spontaneously relax towards the supercooled liquid state over a long enough time. </p><p>Glasses are thermodynamically non-equilibrium kinetically stabilized amorphous solids, in which the molecular disorder and the thermodynamic properties corresponding to the state of the respective under-cooled melt at a temperature <i>T*</i> are frozen-in. Hereby <i>T*</i> differs from the actual temperature <i>T</i>.<sup id="cite_ref-27" class="reference"><a href="#cite_note-27"><span class="cite-bracket">&#91;</span>27<span class="cite-bracket">&#93;</span></a></sup> </p><p>Glass is a nonequilibrium, non-crystalline condensed state of matter that exhibits a glass transition. The structure of glasses is similar to that of their parent supercooled liquids (SCL), and they spontaneously relax toward the SCL state. Their ultimate fate is to solidify, i.e., crystallize.<sup id="cite_ref-:1_23-1" class="reference"><a href="#cite_note-:1-23"><span class="cite-bracket">&#91;</span>23<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading2"><h2 id="Transition_temperature_Tg">Transition temperature <i>T</i><sub>g</sub></h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=3" title="Edit section: Transition temperature Tg"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p><span class="anchor" id="Transition_temperature"></span> </p> <style data-mw-deduplicate="TemplateStyles:r1251242444">.mw-parser-output .ambox{border:1px solid #a2a9b1;border-left:10px solid #36c;background-color:#fbfbfb;box-sizing:border-box}.mw-parser-output .ambox+link+.ambox,.mw-parser-output .ambox+link+style+.ambox,.mw-parser-output .ambox+link+link+.ambox,.mw-parser-output .ambox+.mw-empty-elt+link+.ambox,.mw-parser-output .ambox+.mw-empty-elt+link+style+.ambox,.mw-parser-output .ambox+.mw-empty-elt+link+link+.ambox{margin-top:-1px}html body.mediawiki .mw-parser-output .ambox.mbox-small-left{margin:4px 1em 4px 0;overflow:hidden;width:238px;border-collapse:collapse;font-size:88%;line-height:1.25em}.mw-parser-output .ambox-speedy{border-left:10px solid #b32424;background-color:#fee7e6}.mw-parser-output .ambox-delete{border-left:10px solid #b32424}.mw-parser-output .ambox-content{border-left:10px solid #f28500}.mw-parser-output .ambox-style{border-left:10px solid #fc3}.mw-parser-output .ambox-move{border-left:10px solid #9932cc}.mw-parser-output .ambox-protection{border-left:10px solid #a2a9b1}.mw-parser-output .ambox .mbox-text{border:none;padding:0.25em 0.5em;width:100%}.mw-parser-output .ambox .mbox-image{border:none;padding:2px 0 2px 0.5em;text-align:center}.mw-parser-output .ambox .mbox-imageright{border:none;padding:2px 0.5em 2px 0;text-align:center}.mw-parser-output .ambox .mbox-empty-cell{border:none;padding:0;width:1px}.mw-parser-output .ambox .mbox-image-div{width:52px}@media(min-width:720px){.mw-parser-output .ambox{margin:0 10%}}@media print{body.ns-0 .mw-parser-output .ambox{display:none!important}}</style><table class="box-More_citations_needed_section plainlinks metadata ambox ambox-content ambox-Refimprove" role="presentation"><tbody><tr><td class="mbox-image"><div class="mbox-image-div"><span typeof="mw:File"><a href="/wiki/File:Question_book-new.svg" class="mw-file-description"><img alt="" src="//upload.wikimedia.org/wikipedia/en/thumb/9/99/Question_book-new.svg/50px-Question_book-new.svg.png" decoding="async" width="50" height="39" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/en/thumb/9/99/Question_book-new.svg/75px-Question_book-new.svg.png 1.5x, //upload.wikimedia.org/wikipedia/en/thumb/9/99/Question_book-new.svg/100px-Question_book-new.svg.png 2x" data-file-width="512" data-file-height="399" /></a></span></div></td><td class="mbox-text"><div class="mbox-text-span">This section <b>needs additional citations for <a href="/wiki/Wikipedia:Verifiability" title="Wikipedia:Verifiability">verification</a></b>.<span class="hide-when-compact"> Please help <a href="/wiki/Special:EditPage/Glass_transition" title="Special:EditPage/Glass transition">improve this article</a> by <a href="/wiki/Help:Referencing_for_beginners" title="Help:Referencing for beginners">adding citations to reliable sources</a>&#32;in this section. Unsourced material may be challenged and removed.</span> <span class="date-container"><i>(<span class="date">July 2009</span>)</i></span><span class="hide-when-compact"><i> (<small><a href="/wiki/Help:Maintenance_template_removal" title="Help:Maintenance template removal">Learn how and when to remove this message</a></small>)</i></span></div></td></tr></tbody></table> <figure class="mw-default-size" typeof="mw:File/Thumb"><a href="/wiki/File:Tgdilatometric.gif" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/7/7b/Tgdilatometric.gif/220px-Tgdilatometric.gif" decoding="async" width="220" height="150" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/7/7b/Tgdilatometric.gif/330px-Tgdilatometric.gif 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/7/7b/Tgdilatometric.gif/440px-Tgdilatometric.gif 2x" data-file-width="2569" data-file-height="1752" /></a><figcaption>Determination of <i>T</i><sub>g</sub> by <a href="/wiki/Dilatometer" title="Dilatometer">dilatometry</a>.</figcaption></figure> <figure class="mw-default-size" typeof="mw:File/Thumb"><a href="/wiki/File:Tgdscenglish.svg" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/1/16/Tgdscenglish.svg/220px-Tgdscenglish.svg.png" decoding="async" width="220" height="182" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/1/16/Tgdscenglish.svg/330px-Tgdscenglish.svg.png 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/1/16/Tgdscenglish.svg/440px-Tgdscenglish.svg.png 2x" data-file-width="420" data-file-height="348" /></a><figcaption>Measurement of <i>T</i><sub>g</sub> (the temperature at the point A) by differential scanning calorimetry</figcaption></figure> <p>Refer to the figure on the bottom right plotting the heat capacity as a function of temperature. In this context, <i>T</i><sub>g</sub> is the temperature corresponding to point A on the curve.<sup id="cite_ref-tgmeasurement_28-0" class="reference"><a href="#cite_note-tgmeasurement-28"><span class="cite-bracket">&#91;</span>28<span class="cite-bracket">&#93;</span></a></sup> </p><p>Different operational definitions of the glass transition temperature <i>T</i><sub>g</sub> are in use, and several of them are endorsed as accepted scientific standards. Nevertheless, all definitions are arbitrary, and all yield different numeric results: at best, values of <i>T</i><sub>g</sub> for a given substance agree within a few kelvins. One definition refers to the <a href="/wiki/Viscosity" title="Viscosity">viscosity</a>, fixing <i>T</i><sub>g</sub> at a value of 10<sup>13</sup> poise (or 10<sup>12</sup> Pa·s). As evidenced experimentally, this value is close to the <a href="/wiki/Annealing_(glass)" title="Annealing (glass)">annealing point</a> of many glasses.<sup id="cite_ref-29" class="reference"><a href="#cite_note-29"><span class="cite-bracket">&#91;</span>29<span class="cite-bracket">&#93;</span></a></sup> </p><p>In contrast to viscosity, the <a href="/wiki/Thermal_expansion" title="Thermal expansion">thermal expansion</a>, <a href="/wiki/Heat_capacity" title="Heat capacity">heat capacity</a>, shear modulus, and many other properties of inorganic <a href="/wiki/Glass" title="Glass">glasses</a> show a relatively sudden change at the glass transition temperature. Any such step or kink can be used to define <i>T</i><sub>g</sub>. To make this definition reproducible, the cooling or heating rate must be specified. </p><p>The most frequently used definition of <i>T</i><sub>g</sub> uses the energy release on heating in <a href="/wiki/Differential_scanning_calorimetry" title="Differential scanning calorimetry">differential scanning calorimetry</a> (DSC, see figure). Typically, the sample is first cooled with 10 K/min and then heated with that same speed. </p><p>Yet another definition of <i>T</i><sub>g</sub> uses the kink in <a href="/wiki/Dilatometer" title="Dilatometer">dilatometry</a> (a.k.a. thermal expansion): refer to the figure on the top right. Here, heating rates of 3–5&#160;K/min (5.4–9.0&#160;°F/min) are common. The linear sections below and above <i>T</i><sub>g</sub> are colored green. <i>T</i><sub>g</sub> is the temperature at the intersection of the red regression lines.<sup id="cite_ref-tgmeasurement_28-1" class="reference"><a href="#cite_note-tgmeasurement-28"><span class="cite-bracket">&#91;</span>28<span class="cite-bracket">&#93;</span></a></sup> </p><p>Summarized below are <i>T</i><sub>g</sub> values characteristic of certain classes of materials. </p> <div class="mw-heading mw-heading3"><h3 id="Polymers">Polymers</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=4" title="Edit section: Polymers"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <table class="wikitable sortable"> <tbody><tr> <th>Material </th> <th><i>T</i><sub>g</sub> (°C) </th> <th><i>T</i><sub>g</sub> (°F) </th> <th>Commercial name </th></tr> <tr> <td><a href="/wiki/Tire" title="Tire">Tire</a> rubber </td> <td style="text-align:right;">−70 </td> <td style="text-align:right;">−94<sup id="cite_ref-30" class="reference"><a href="#cite_note-30"><span class="cite-bracket">&#91;</span>30<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyvinylidene_fluoride" title="Polyvinylidene fluoride">Polyvinylidene fluoride</a> (PVDF) </td> <td style="text-align:right;">−35 </td> <td style="text-align:right;">−31<sup id="cite_ref-Ibeh_31-0" class="reference"><a href="#cite_note-Ibeh-31"><span class="cite-bracket">&#91;</span>31<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polypropylene" title="Polypropylene">Polypropylene</a> (PP atactic) </td> <td style="text-align:right;">−20 </td> <td style="text-align:right;">−4<sup id="cite_ref-PVC_32-0" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyvinyl_fluoride" title="Polyvinyl fluoride">Polyvinyl fluoride</a> (PVF) </td> <td style="text-align:right;">−20 </td> <td style="text-align:right;">−4<sup id="cite_ref-Ibeh_31-1" class="reference"><a href="#cite_note-Ibeh-31"><span class="cite-bracket">&#91;</span>31<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polypropylene" title="Polypropylene">Polypropylene</a> (PP isotactic) </td> <td style="text-align:right;">0 </td> <td style="text-align:right;">32<sup id="cite_ref-PVC_32-1" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Poly-3-hydroxybutyrate" class="mw-redirect" title="Poly-3-hydroxybutyrate">Poly-3-hydroxybutyrate</a> (PHB) </td> <td style="text-align:right;">15 </td> <td style="text-align:right;">59<sup id="cite_ref-PVC_32-2" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyvinyl_acetate" title="Polyvinyl acetate">Poly(vinyl acetate)</a> (PVAc) </td> <td style="text-align:right;">30 </td> <td style="text-align:right;">86<sup id="cite_ref-PVC_32-3" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polychlorotrifluoroethylene" title="Polychlorotrifluoroethylene">Polychlorotrifluoroethylene</a> (PCTFE) </td> <td style="text-align:right;">45 </td> <td style="text-align:right;">113<sup id="cite_ref-Ibeh_31-2" class="reference"><a href="#cite_note-Ibeh-31"><span class="cite-bracket">&#91;</span>31<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyamide" title="Polyamide">Polyamide</a> (PA) </td> <td style="text-align:right;">47–60 </td> <td style="text-align:right;">117–140 </td> <td>Nylon-6,x </td></tr> <tr> <td><a href="/wiki/Polylactic_acid" title="Polylactic acid">Polylactic acid</a> (PLA) </td> <td style="text-align:right;">60–65 </td> <td style="text-align:right;">140–149 </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyethylene_terephthalate" title="Polyethylene terephthalate">Polyethylene terephthalate</a> (PET) </td> <td style="text-align:right;">70 </td> <td style="text-align:right;">158<sup id="cite_ref-PVC_32-4" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyvinyl_chloride" title="Polyvinyl chloride">Poly(vinyl chloride)</a> (PVC) </td> <td style="text-align:right;">80 </td> <td style="text-align:right;">176<sup id="cite_ref-PVC_32-5" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polyvinyl_alcohol" title="Polyvinyl alcohol">Poly(vinyl alcohol)</a> (PVA) </td> <td style="text-align:right;">85 </td> <td style="text-align:right;">185<sup id="cite_ref-PVC_32-6" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polystyrene" title="Polystyrene">Polystyrene</a> (PS) </td> <td style="text-align:right;">95 </td> <td style="text-align:right;">203<sup id="cite_ref-PVC_32-7" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Poly(methyl_methacrylate)" title="Poly(methyl methacrylate)">Poly(methyl methacrylate)</a> (PMMA atactic) </td> <td style="text-align:right;">105 </td> <td style="text-align:right;">221<sup id="cite_ref-PVC_32-8" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td>Plexiglas, Perspex </td></tr> <tr> <td><a href="/wiki/Acrylonitrile_butadiene_styrene" title="Acrylonitrile butadiene styrene">Acrylonitrile butadiene styrene</a> (ABS) </td> <td style="text-align:right;">105 </td> <td style="text-align:right;">221<sup id="cite_ref-ABS_33-0" class="reference"><a href="#cite_note-ABS-33"><span class="cite-bracket">&#91;</span>33<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr> <tr> <td><a href="/wiki/Polytetrafluoroethylene" title="Polytetrafluoroethylene">Polytetrafluoroethylene</a> (PTFE) </td> <td style="text-align:right;">115 </td> <td style="text-align:right;">239<sup id="cite_ref-34" class="reference"><a href="#cite_note-34"><span class="cite-bracket">&#91;</span>34<span class="cite-bracket">&#93;</span></a></sup> </td> <td>Teflon </td></tr> <tr> <td><a href="/wiki/Polycarbonate" title="Polycarbonate">Poly(carbonate)</a> (PC) </td> <td style="text-align:right;">145 </td> <td style="text-align:right;">293<sup id="cite_ref-PVC_32-9" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td>Lexan </td></tr> <tr> <td><a href="/wiki/Polysulfone" title="Polysulfone">Polysulfone</a> </td> <td style="text-align:right;">185 </td> <td style="text-align:right;">365 </td> <td> </td></tr> <tr> <td><a href="/wiki/Polynorbornene" class="mw-redirect" title="Polynorbornene">Polynorbornene</a> </td> <td style="text-align:right;">215 </td> <td style="text-align:right;">419<sup id="cite_ref-PVC_32-10" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </td> <td> </td></tr></tbody></table> <p>Dry <a href="/wiki/Nylon" title="Nylon">nylon-6</a> has a glass transition temperature of 47&#160;°C (117&#160;°F).<sup id="cite_ref-35" class="reference"><a href="#cite_note-35"><span class="cite-bracket">&#91;</span>35<span class="cite-bracket">&#93;</span></a></sup> Nylon-6,6 in the dry state has a glass transition temperature of about 70&#160;°C (158&#160;°F).<sup id="cite_ref-36" class="reference"><a href="#cite_note-36"><span class="cite-bracket">&#91;</span>36<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-37" class="reference"><a href="#cite_note-37"><span class="cite-bracket">&#91;</span>37<span class="cite-bracket">&#93;</span></a></sup> Whereas <a href="/wiki/Polyethene" class="mw-redirect" title="Polyethene">polyethene</a> has a glass transition range of −130 to −80&#160;°C (−202 to −112&#160;°F)<sup id="cite_ref-38" class="reference"><a href="#cite_note-38"><span class="cite-bracket">&#91;</span>38<span class="cite-bracket">&#93;</span></a></sup> The above are only mean values, as the glass transition temperature depends on the cooling rate and molecular weight distribution and could be influenced by additives. For a semi-crystalline material, such as <a href="/wiki/Polyethene" class="mw-redirect" title="Polyethene">polyethene</a> that is 60–80% crystalline at room temperature, the quoted glass transition refers to what happens to the amorphous part of the material upon cooling. </p> <div class="mw-heading mw-heading3"><h3 id="Silicates_and_other_covalent_network_glasses">Silicates and other covalent network glasses</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=5" title="Edit section: Silicates and other covalent network glasses"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <table class="wikitable sortable"> <tbody><tr> <th>Material </th> <th><i>T</i><sub>g</sub> (°C) </th> <th><i>T</i><sub>g</sub> (°F) </th></tr> <tr> <td><a href="/wiki/Chalcogenide" title="Chalcogenide">Chalcogenide</a> GeSbTe </td> <td style="text-align:right;">150 </td> <td style="text-align:right;">302<sup id="cite_ref-39" class="reference"><a href="#cite_note-39"><span class="cite-bracket">&#91;</span>39<span class="cite-bracket">&#93;</span></a></sup> </td></tr> <tr> <td><a href="/wiki/Chalcogenide" title="Chalcogenide">Chalcogenide</a> AsGeSeTe </td> <td style="text-align:right;">245 </td> <td style="text-align:right;">473 </td></tr> <tr> <td><a href="/wiki/ZBLAN" title="ZBLAN">ZBLAN</a> fluoride glass </td> <td style="text-align:right;">235 </td> <td style="text-align:right;">455 </td></tr> <tr> <td><a href="/wiki/Tellurium_dioxide" title="Tellurium dioxide">Tellurium dioxide</a> </td> <td style="text-align:right;">280 </td> <td style="text-align:right;">536 </td></tr> <tr> <td>Fluoroaluminate </td> <td style="text-align:right;">400 </td> <td style="text-align:right;">752 </td></tr> <tr> <td><a href="/wiki/Soda-lime_glass" class="mw-redirect" title="Soda-lime glass">Soda-lime glass</a> </td> <td style="text-align:right;">520–600 </td> <td style="text-align:right;">968–1,112 </td></tr> <tr> <td><a href="/wiki/Fused_quartz" title="Fused quartz">Fused quartz</a> (approximate) </td> <td style="text-align:right;">1,200 </td> <td style="text-align:right;">2,200<sup id="cite_ref-40" class="reference"><a href="#cite_note-40"><span class="cite-bracket">&#91;</span>40<span class="cite-bracket">&#93;</span></a></sup> </td></tr></tbody></table> <div class="mw-heading mw-heading2"><h2 id="Linear_heat_capacity">Linear heat capacity</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=6" title="Edit section: Linear heat capacity"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <figure class="mw-default-size" typeof="mw:File/Thumb"><a href="/wiki/File:Specific_heat_of_several_glassy_solids.png" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/6/68/Specific_heat_of_several_glassy_solids.png/220px-Specific_heat_of_several_glassy_solids.png" decoding="async" width="220" height="309" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/6/68/Specific_heat_of_several_glassy_solids.png/330px-Specific_heat_of_several_glassy_solids.png 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/6/68/Specific_heat_of_several_glassy_solids.png/440px-Specific_heat_of_several_glassy_solids.png 2x" data-file-width="1496" data-file-height="2098" /></a><figcaption>Specific heat of several noncrystalline solids, plotted as <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle (T^{2},c/T)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mo stretchy="false">(</mo> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>2</mn> </mrow> </msup> <mo>,</mo> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mo>/</mo> </mrow> <mi>T</mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle (T^{2},c/T)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/f18627fc67751795348618cbf2a5366ffa7affbf" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:9.423ex; height:3.176ex;" alt="{\displaystyle (T^{2},c/T)}"></span> graph, showing linear dependence component in the low-temperature regime.<sup id="cite_ref-:2_41-0" class="reference"><a href="#cite_note-:2-41"><span class="cite-bracket">&#91;</span>41<span class="cite-bracket">&#93;</span></a></sup></figcaption></figure> <p>In 1971, Zeller and <a href="/wiki/Robert_Otto_Pohl" title="Robert Otto Pohl">Pohl</a> discovered that <sup id="cite_ref-42" class="reference"><a href="#cite_note-42"><span class="cite-bracket">&#91;</span>42<span class="cite-bracket">&#93;</span></a></sup> when glass is at a very low temperature ~1K, its specific heat has a linear component: <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle c\approx c_{1}T+c_{3}T^{3}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>c</mi> <mo>&#x2248;<!-- ≈ --></mo> <msub> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>1</mn> </mrow> </msub> <mi>T</mi> <mo>+</mo> <msub> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>3</mn> </mrow> </msub> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>3</mn> </mrow> </msup> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle c\approx c_{1}T+c_{3}T^{3}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/64083590772dc2c49588709f6a5e77bc0a2fce78" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.671ex; width:15.478ex; height:3.009ex;" alt="{\displaystyle c\approx c_{1}T+c_{3}T^{3}}"></span>. This is an unusual effect, because crystal material typically has <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle c\propto T^{3}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>c</mi> <mo>&#x221D;<!-- ∝ --></mo> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>3</mn> </mrow> </msup> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle c\propto T^{3}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/c761a6c248cea53ecaceb0237d9e375a40868ff1" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:6.88ex; height:2.676ex;" alt="{\displaystyle c\propto T^{3}}"></span>, as in the <a href="/wiki/Debye_model" title="Debye model">Debye model</a>. This was explained by the two-level system hypothesis,<sup id="cite_ref-43" class="reference"><a href="#cite_note-43"><span class="cite-bracket">&#91;</span>43<span class="cite-bracket">&#93;</span></a></sup> which states that a glass is populated by two-level systems, which look like a double potential well separated by a wall. The wall is high enough such that resonance tunneling does not occur, but thermal tunneling does occur. Namely, if the two wells have energy difference <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \Delta E\sim k_{B}T}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo>&#x223C;<!-- ∼ --></mo> <msub> <mi>k</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>B</mi> </mrow> </msub> <mi>T</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \Delta E\sim k_{B}T}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/ae149ded1431380bde659659f029ba3c4b83fe11" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.671ex; width:11.137ex; height:2.509ex;" alt="{\displaystyle \Delta E\sim k_{B}T}"></span>, then a particle in one well can tunnel to the other well by thermal interaction with the environment. Now, imagine that there are many two-level systems in the glass, and their <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \Delta E}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \Delta E}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/345f0ed5ff6ec6eddc5f908d379f032c52f119c2" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:3.711ex; height:2.176ex;" alt="{\displaystyle \Delta E}"></span> is randomly distributed but fixed ("quenched disorder"), then as temperature drops, more and more of these two-level levels are frozen out (meaning that it takes such a long time for a tunneling to occur, that they cannot be experimentally observed). </p><p>Consider a single two-level system that is not frozen-out, whose energy gap is <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \Delta E=O(1/\beta )}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo>=</mo> <mi>O</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mrow class="MJX-TeXAtom-ORD"> <mo>/</mo> </mrow> <mi>&#x03B2;<!-- β --></mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \Delta E=O(1/\beta )}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/475d6f8f56790b63c53df3e3658c3b42923d3eaa" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:14.049ex; height:2.843ex;" alt="{\displaystyle \Delta E=O(1/\beta )}"></span>. It is in a Boltzmann distribution, so its average energy <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle ={\frac {\beta \Delta E}{e^{\beta \Delta E}-1}}\beta ^{-1}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mo>=</mo> <mrow class="MJX-TeXAtom-ORD"> <mfrac> <mrow> <mi>&#x03B2;<!-- β --></mi> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mrow> <mrow> <msup> <mi>e</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>&#x03B2;<!-- β --></mi> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mrow> </msup> <mo>&#x2212;<!-- − --></mo> <mn>1</mn> </mrow> </mfrac> </mrow> <msup> <mi>&#x03B2;<!-- β --></mi> <mrow class="MJX-TeXAtom-ORD"> <mo>&#x2212;<!-- − --></mo> <mn>1</mn> </mrow> </msup> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle ={\frac {\beta \Delta E}{e^{\beta \Delta E}-1}}\beta ^{-1}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/fcfb1e0fe5a09ad841adad321b92a4531817118c" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.338ex; width:15.844ex; height:5.843ex;" alt="{\displaystyle ={\frac {\beta \Delta E}{e^{\beta \Delta E}-1}}\beta ^{-1}}"></span>. </p><p>Now, assume that the two-level systems are all quenched, so that each <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \Delta E}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \Delta E}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/345f0ed5ff6ec6eddc5f908d379f032c52f119c2" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:3.711ex; height:2.176ex;" alt="{\displaystyle \Delta E}"></span> varies little with temperature. In that case, we can write <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle n(\Delta E)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>n</mi> <mo stretchy="false">(</mo> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle n(\Delta E)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/af877de3f2b5041e7f8c7d73f26e1386422b0412" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:6.916ex; height:2.843ex;" alt="{\displaystyle n(\Delta E)}"></span> as the density of states with energy gap <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \Delta E}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \Delta E}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/345f0ed5ff6ec6eddc5f908d379f032c52f119c2" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:3.711ex; height:2.176ex;" alt="{\displaystyle \Delta E}"></span>. We also assume that <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle n(\Delta E)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>n</mi> <mo stretchy="false">(</mo> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle n(\Delta E)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/af877de3f2b5041e7f8c7d73f26e1386422b0412" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:6.916ex; height:2.843ex;" alt="{\displaystyle n(\Delta E)}"></span> is positive and smooth near <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \Delta E\approx 0}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo>&#x2248;<!-- ≈ --></mo> <mn>0</mn> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \Delta E\approx 0}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/93a758108d847011c2dc63f497fc92a2a7f23df2" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:7.972ex; height:2.176ex;" alt="{\displaystyle \Delta E\approx 0}"></span>. </p><p>Then, the total energy contributed by those two-level systems is<span class="mwe-math-element"><span class="mwe-math-mathml-display mwe-math-mathml-a11y" style="display: none;"><math display="block" xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle {\bar {E}}\sim \int _{0}^{O(1/\beta )}{\frac {\beta \Delta E}{e^{\beta \Delta E}-1}}\beta ^{-1}\;n(\Delta E)d\Delta E=\beta ^{-2}\int _{0}^{O(1)}{\frac {a}{e^{a}-1}}n(a/\beta )da\propto \beta ^{-2}n(0)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mrow class="MJX-TeXAtom-ORD"> <mrow class="MJX-TeXAtom-ORD"> <mover> <mi>E</mi> <mo stretchy="false">&#x00AF;<!-- ¯ --></mo> </mover> </mrow> </mrow> <mo>&#x223C;<!-- ∼ --></mo> <msubsup> <mo>&#x222B;<!-- ∫ --></mo> <mrow class="MJX-TeXAtom-ORD"> <mn>0</mn> </mrow> <mrow class="MJX-TeXAtom-ORD"> <mi>O</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mrow class="MJX-TeXAtom-ORD"> <mo>/</mo> </mrow> <mi>&#x03B2;<!-- β --></mi> <mo stretchy="false">)</mo> </mrow> </msubsup> <mrow class="MJX-TeXAtom-ORD"> <mfrac> <mrow> <mi>&#x03B2;<!-- β --></mi> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mrow> <mrow> <msup> <mi>e</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>&#x03B2;<!-- β --></mi> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> </mrow> </msup> <mo>&#x2212;<!-- − --></mo> <mn>1</mn> </mrow> </mfrac> </mrow> <msup> <mi>&#x03B2;<!-- β --></mi> <mrow class="MJX-TeXAtom-ORD"> <mo>&#x2212;<!-- − --></mo> <mn>1</mn> </mrow> </msup> <mspace width="thickmathspace" /> <mi>n</mi> <mo stretchy="false">(</mo> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo stretchy="false">)</mo> <mi>d</mi> <mi mathvariant="normal">&#x0394;<!-- Δ --></mi> <mi>E</mi> <mo>=</mo> <msup> <mi>&#x03B2;<!-- β --></mi> <mrow class="MJX-TeXAtom-ORD"> <mo>&#x2212;<!-- − --></mo> <mn>2</mn> </mrow> </msup> <msubsup> <mo>&#x222B;<!-- ∫ --></mo> <mrow class="MJX-TeXAtom-ORD"> <mn>0</mn> </mrow> <mrow class="MJX-TeXAtom-ORD"> <mi>O</mi> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </msubsup> <mrow class="MJX-TeXAtom-ORD"> <mfrac> <mi>a</mi> <mrow> <msup> <mi>e</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>a</mi> </mrow> </msup> <mo>&#x2212;<!-- − --></mo> <mn>1</mn> </mrow> </mfrac> </mrow> <mi>n</mi> <mo stretchy="false">(</mo> <mi>a</mi> <mrow class="MJX-TeXAtom-ORD"> <mo>/</mo> </mrow> <mi>&#x03B2;<!-- β --></mi> <mo stretchy="false">)</mo> <mi>d</mi> <mi>a</mi> <mo>&#x221D;<!-- ∝ --></mo> <msup> <mi>&#x03B2;<!-- β --></mi> <mrow class="MJX-TeXAtom-ORD"> <mo>&#x2212;<!-- − --></mo> <mn>2</mn> </mrow> </msup> <mi>n</mi> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle {\bar {E}}\sim \int _{0}^{O(1/\beta )}{\frac {\beta \Delta E}{e^{\beta \Delta E}-1}}\beta ^{-1}\;n(\Delta E)d\Delta E=\beta ^{-2}\int _{0}^{O(1)}{\frac {a}{e^{a}-1}}n(a/\beta )da\propto \beta ^{-2}n(0)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/dd8f2a04e5032d4a82f5fdd13ef8614d1bb83404" class="mwe-math-fallback-image-display mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.338ex; width:80.083ex; height:6.343ex;" alt="{\displaystyle {\bar {E}}\sim \int _{0}^{O(1/\beta )}{\frac {\beta \Delta E}{e^{\beta \Delta E}-1}}\beta ^{-1}\;n(\Delta E)d\Delta E=\beta ^{-2}\int _{0}^{O(1)}{\frac {a}{e^{a}-1}}n(a/\beta )da\propto \beta ^{-2}n(0)}"></span> </p><p>The effect is that the average energy in these two-level systems is <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle {\bar {E}}\sim T^{2}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mrow class="MJX-TeXAtom-ORD"> <mrow class="MJX-TeXAtom-ORD"> <mover> <mi>E</mi> <mo stretchy="false">&#x00AF;<!-- ¯ --></mo> </mover> </mrow> </mrow> <mo>&#x223C;<!-- ∼ --></mo> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>2</mn> </mrow> </msup> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle {\bar {E}}\sim T^{2}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/6f8ed654775664d394197b2fc2d8045fdc39ab76" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:7.648ex; height:2.676ex;" alt="{\displaystyle {\bar {E}}\sim T^{2}}"></span>, leading to a <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \partial _{T}{\bar {E}}\propto T}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <msub> <mi mathvariant="normal">&#x2202;<!-- ∂ --></mi> <mrow class="MJX-TeXAtom-ORD"> <mi>T</mi> </mrow> </msub> <mrow class="MJX-TeXAtom-ORD"> <mrow class="MJX-TeXAtom-ORD"> <mover> <mi>E</mi> <mo stretchy="false">&#x00AF;<!-- ¯ --></mo> </mover> </mrow> </mrow> <mo>&#x221D;<!-- ∝ --></mo> <mi>T</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \partial _{T}{\bar {E}}\propto T}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/245c788981e511dcfa9965f347af5bf66fe67ee0" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.671ex; width:9.134ex; height:2.843ex;" alt="{\displaystyle \partial _{T}{\bar {E}}\propto T}"></span> term. </p> <div class="mw-heading mw-heading3"><h3 id="Experimental_data">Experimental data</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=7" title="Edit section: Experimental data"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p>In experimental measurements, the specific heat capacity of glass is measured at different temperatures, and a <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle (T^{2},c/T)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mo stretchy="false">(</mo> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>2</mn> </mrow> </msup> <mo>,</mo> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mo>/</mo> </mrow> <mi>T</mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle (T^{2},c/T)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/f18627fc67751795348618cbf2a5366ffa7affbf" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:9.423ex; height:3.176ex;" alt="{\displaystyle (T^{2},c/T)}"></span> graph is plotted. Assuming that <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle c\approx c_{1}T+c_{3}T^{3}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>c</mi> <mo>&#x2248;<!-- ≈ --></mo> <msub> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>1</mn> </mrow> </msub> <mi>T</mi> <mo>+</mo> <msub> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>3</mn> </mrow> </msub> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>3</mn> </mrow> </msup> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle c\approx c_{1}T+c_{3}T^{3}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/64083590772dc2c49588709f6a5e77bc0a2fce78" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.671ex; width:15.478ex; height:3.009ex;" alt="{\displaystyle c\approx c_{1}T+c_{3}T^{3}}"></span>, the graph should show <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle c/T\approx c_{1}+c_{3}T^{2}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mo>/</mo> </mrow> <mi>T</mi> <mo>&#x2248;<!-- ≈ --></mo> <msub> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>1</mn> </mrow> </msub> <mo>+</mo> <msub> <mi>c</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>3</mn> </mrow> </msub> <msup> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>2</mn> </mrow> </msup> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle c/T\approx c_{1}+c_{3}T^{2}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/dab25795c40dc3c8e5e26ee262bcfd493d9c6e59" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:16.641ex; height:3.176ex;" alt="{\displaystyle c/T\approx c_{1}+c_{3}T^{2}}"></span>, that is, a straight line with slope showing the typical Debye-like heat capacity, and a vertical intercept showing the anomalous linear component.<sup id="cite_ref-:2_41-1" class="reference"><a href="#cite_note-:2-41"><span class="cite-bracket">&#91;</span>41<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading2"><h2 id="Kauzmann's_paradox"><span id="Kauzmann.27s_paradox"></span>Kauzmann's paradox</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=8" title="Edit section: Kauzmann&#039;s paradox"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <figure class="mw-default-size mw-halign-right" typeof="mw:File/Thumb"><a href="/wiki/File:KauzmannParadox.png" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/8/8f/KauzmannParadox.png/220px-KauzmannParadox.png" decoding="async" width="220" height="189" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/8/8f/KauzmannParadox.png/330px-KauzmannParadox.png 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/8/8f/KauzmannParadox.png/440px-KauzmannParadox.png 2x" data-file-width="485" data-file-height="417" /></a><figcaption>Entropy difference between crystal and undercooled melt</figcaption></figure> <p>As a liquid is supercooled, the difference in entropy between the liquid and solid phase decreases. By <a href="/wiki/Extrapolating" class="mw-redirect" title="Extrapolating">extrapolating</a> the <a href="/wiki/Heat_capacity" title="Heat capacity">heat capacity</a> of the supercooled liquid below its <a href="/wiki/Glass_transition_temperature" class="mw-redirect" title="Glass transition temperature">glass transition temperature</a>, it is possible to calculate the temperature at which the difference in entropies becomes zero. This temperature has been named the <b><a href="/wiki/Walter_Kauzmann" title="Walter Kauzmann">Kauzmann</a> temperature</b>. </p><p>If a liquid could be supercooled below its Kauzmann temperature, and it did indeed display a lower entropy than the crystal phase, this would be paradoxical, as the liquid phase should have the same vibrational entropy, but much higher positional entropy, as the crystal phase. This is the <b>Kauzmann paradox</b>, still not definitively resolved.<sup id="cite_ref-44" class="reference"><a href="#cite_note-44"><span class="cite-bracket">&#91;</span>44<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-:0_45-0" class="reference"><a href="#cite_note-:0-45"><span class="cite-bracket">&#91;</span>45<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading3"><h3 id="Possible_resolutions">Possible resolutions</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=9" title="Edit section: Possible resolutions"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p>There are many possible resolutions to the Kauzmann paradox. </p><p>Kauzmann himself resolved the entropy paradox by postulating that all supercooled liquids must crystallize before the Kauzmann temperature is reached. </p><p>Perhaps at the Kauzmann temperature, glass reaches an ideal glass <i>phase</i>, which is still amorphous, but has a long-range amorphous order which decreases its overall entropy to that of the crystal. The ideal glass would be a true phase of matter.<sup id="cite_ref-:0_45-1" class="reference"><a href="#cite_note-:0-45"><span class="cite-bracket">&#91;</span>45<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-46" class="reference"><a href="#cite_note-46"><span class="cite-bracket">&#91;</span>46<span class="cite-bracket">&#93;</span></a></sup> The ideal glass is hypothesized, but cannot be observed naturally, as it would take too long to form. Something approaching an ideal glass has been observed as "ultrastable glass" formed by <a href="/wiki/Vacuum_deposition" title="Vacuum deposition">vapor deposition</a>,<sup id="cite_ref-47" class="reference"><a href="#cite_note-47"><span class="cite-bracket">&#91;</span>47<span class="cite-bracket">&#93;</span></a></sup> </p><p>Perhaps there must be a <a href="/wiki/Phase_transition" title="Phase transition">phase transition</a> before the entropy of the liquid decreases. In this scenario, the transition temperature is known as the <i>calorimetric ideal glass transition temperature</i> <i>T</i><sub>0c</sub>. In this view, the glass transition is not merely a <a href="/wiki/Chemical_kinetics" title="Chemical kinetics">kinetic</a> effect, i.e. merely the result of fast cooling of a melt, but there is an underlying <a href="/wiki/Thermodynamic" class="mw-redirect" title="Thermodynamic">thermodynamic</a> basis for glass formation. The glass transition temperature: </p> <dl><dd><span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle T_{g}\to T_{0c}{\text{ as }}{\frac {dT}{dt}}\to 0.}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <msub> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>g</mi> </mrow> </msub> <mo stretchy="false">&#x2192;<!-- → --></mo> <msub> <mi>T</mi> <mrow class="MJX-TeXAtom-ORD"> <mn>0</mn> <mi>c</mi> </mrow> </msub> <mrow class="MJX-TeXAtom-ORD"> <mtext>&#xA0;as&#xA0;</mtext> </mrow> <mrow class="MJX-TeXAtom-ORD"> <mfrac> <mrow> <mi>d</mi> <mi>T</mi> </mrow> <mrow> <mi>d</mi> <mi>t</mi> </mrow> </mfrac> </mrow> <mo stretchy="false">&#x2192;<!-- → --></mo> <mn>0.</mn> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle T_{g}\to T_{0c}{\text{ as }}{\frac {dT}{dt}}\to 0.}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/fd0f258ca0caa5470e4103121a4050e0f2c62ee4" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.005ex; width:21.468ex; height:5.509ex;" alt="{\displaystyle T_{g}\to T_{0c}{\text{ as }}{\frac {dT}{dt}}\to 0.}"></span></dd></dl> <p>Perhaps the heat capacity of the supercooled liquid near the Kauzmann temperature smoothly decreases to a smaller value. </p><p>Perhaps first order phase transition to another liquid state occurs before the Kauzmann temperature with the heat capacity of this new state being less than that obtained by extrapolation from higher temperature. </p> <div class="mw-heading mw-heading2"><h2 id="In_specific_materials">In specific materials</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=10" title="Edit section: In specific materials"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <div class="mw-heading mw-heading3"><h3 id="Silica,_SiO2"><span id="Silica.2C_SiO2"></span>Silica, SiO<sub>2</sub></h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=11" title="Edit section: Silica, SiO2"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p><a href="/wiki/Silica" class="mw-redirect" title="Silica">Silica</a> (the chemical compound SiO<sub>2</sub>) has a number of distinct <a href="/wiki/Crystal" title="Crystal">crystalline</a> forms in addition to the quartz structure. Nearly all of the crystalline forms involve <a href="/wiki/Tetrahedral" class="mw-redirect" title="Tetrahedral">tetrahedral</a> SiO<sub>4</sub> units linked together by <i>shared vertices</i> in different arrangements (<a href="/wiki/Stishovite" title="Stishovite">stishovite</a>, composed of linked SiO<sub>6</sub> <a href="/wiki/Octahedron" title="Octahedron">octahedra</a>, is the main exception). Si-O bond lengths vary between the different crystal forms. For example, in α-quartz the bond length is 161 picometres (6.3<span style="margin:0 .15em 0 .25em">×</span>10<sup>−9</sup>&#160;in), whereas in α-tridymite it ranges from 154–171&#160;pm (6.1<span style="margin:0 .15em 0 .25em">×</span>10<sup>−9</sup>–6.7<span style="margin:0 .15em 0 .25em">×</span>10<sup>−9</sup>&#160;in). The Si-O-Si bond angle also varies from 140° in α-tridymite to 144° in α-quartz to 180° in β-tridymite. Any deviations from these standard parameters constitute microstructural differences or variations that represent an approach to an <a href="/wiki/Amorphous_solid" title="Amorphous solid">amorphous</a>, vitreous or <a href="/wiki/Amorphous_solid" title="Amorphous solid">glassy solid</a>. The transition temperature <i>T</i><sub>g</sub> in silicates is related to the energy required to break and re-form covalent bonds in an amorphous (or random network) lattice of <a href="/wiki/Covalent_bond" title="Covalent bond">covalent bonds</a>. The <i>T</i><sub>g</sub> is clearly influenced by the chemistry of the glass. For example, addition of elements such as <a href="/wiki/Boron" title="Boron">B</a>, <a href="/wiki/Sodium" title="Sodium">Na</a>, <a href="/wiki/Potassium" title="Potassium">K</a> or <a href="/wiki/Calcium" title="Calcium">Ca</a> to a <a href="/wiki/Silica_glass" class="mw-redirect" title="Silica glass">silica glass</a>, which have a <a href="/wiki/Valency_(chemistry)" class="mw-redirect" title="Valency (chemistry)">valency</a> less than 4, helps in breaking up the network structure, thus reducing the <i>T</i><sub>g</sub>. Alternatively, <a href="/wiki/Phosphorus" title="Phosphorus">P</a>, which has a valency of 5, helps to reinforce an ordered lattice, and thus increases the <i>T</i><sub>g</sub>.<sup id="cite_ref-48" class="reference"><a href="#cite_note-48"><span class="cite-bracket">&#91;</span>48<span class="cite-bracket">&#93;</span></a></sup> <i>T</i><sub>g</sub> is directly proportional to bond strength, e.g. it depends on quasi-equilibrium thermodynamic parameters of the bonds e.g. on the enthalpy <i>H</i><sub>d</sub> and entropy <i>S</i><sub>d</sub> of configurons – broken bonds: <i>T</i><sub>g</sub> = <i>H</i><sub>d</sub>&#160;/&#160;[<i>S</i><sub>d</sub>&#160;+&#160;R&#160;ln[(1&#160;−&#160;<i>f</i><sub>c</sub>)/&#160;<i>f</i><sub>c</sub>] where R is the gas constant and <i>f</i><sub>c</sub> is the percolation threshold. For strong melts such as Si<i>O</i><sub>2</sub> the percolation threshold in the above equation is the universal Scher–Zallen critical density in the 3-D space e.g. <i>f</i><sub>c</sub> = 0.15, however for fragile materials the percolation thresholds are material-dependent and <i>f</i><sub>c</sub>&#160;≪&#160;1.<sup id="cite_ref-49" class="reference"><a href="#cite_note-49"><span class="cite-bracket">&#91;</span>49<span class="cite-bracket">&#93;</span></a></sup> The enthalpy <i>H</i><sub>d</sub> and the entropy <i>S</i><sub>d</sub> of configurons – broken bonds can be found from available experimental data on viscosity.<sup id="cite_ref-50" class="reference"><a href="#cite_note-50"><span class="cite-bracket">&#91;</span>50<span class="cite-bracket">&#93;</span></a></sup> On the surface of SiO<sub>2</sub> films, scanning tunneling microscopy has resolved clusters of ca. 5 SiO<sub>2</sub> in diameter that move in a two-state fashion on a time scale of minutes. This is much faster than dynamics in the bulk, but in agreement with models that compare bulk and surface dynamics.<sup id="cite_ref-51" class="reference"><a href="#cite_note-51"><span class="cite-bracket">&#91;</span>51<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-52" class="reference"><a href="#cite_note-52"><span class="cite-bracket">&#91;</span>52<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading3"><h3 id="Polymers_2">Polymers</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=12" title="Edit section: Polymers"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p>In <a href="/wiki/Polymer" title="Polymer">polymers</a> the glass transition temperature, <i>T</i><sub>g</sub>, is often expressed as the temperature at which the <a href="/wiki/Gibbs_free_energy" title="Gibbs free energy">Gibbs free energy</a> is such that the <a href="/wiki/Activation_energy" title="Activation energy">activation energy</a> for the cooperative movement of 50 or so elements of the polymer is exceeded <sup class="noprint Inline-Template Template-Fact" style="white-space:nowrap;">&#91;<i><a href="/wiki/Wikipedia:Citation_needed" title="Wikipedia:Citation needed"><span title="This claim needs references to reliable sources. (September 2010)">citation needed</span></a></i>&#93;</sup>. This allows molecular chains to slide past each other when a force is applied. From this definition, we can see that the introduction of relatively stiff chemical groups (such as <a href="/wiki/Benzene" title="Benzene">benzene</a> rings) will interfere with the flowing process and hence increase <i>T</i><sub>g</sub>.<sup id="cite_ref-53" class="reference"><a href="#cite_note-53"><span class="cite-bracket">&#91;</span>53<span class="cite-bracket">&#93;</span></a></sup> The stiffness of thermoplastics decreases due to this effect (see figure.) When the glass temperature has been reached, the stiffness stays the same for a while, i.e., at or near <i>E</i><sub>2</sub>, until the temperature exceeds <i>T</i><sub>m</sub>, and the material melts. This region is called the rubber plateau. </p> <figure class="mw-default-size mw-halign-right" typeof="mw:File/Thumb"><a href="/wiki/File:Ironing.jpg" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/6/64/Ironing.jpg/220px-Ironing.jpg" decoding="async" width="220" height="184" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/6/64/Ironing.jpg/330px-Ironing.jpg 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/6/64/Ironing.jpg/440px-Ironing.jpg 2x" data-file-width="7513" data-file-height="6292" /></a><figcaption>In ironing, a fabric is heated through the glass-rubber transition.</figcaption></figure> <p>In <a href="/wiki/Ironing" title="Ironing">ironing</a>, a fabric is heated through this transition so that the polymer chains become mobile. The weight of the iron then imposes a preferred orientation. <i>T</i><sub>g</sub> can be significantly decreased by addition of <a href="/wiki/Plasticizer" title="Plasticizer">plasticizers</a> into the polymer matrix. Smaller molecules of plasticizer embed themselves between the polymer chains, increasing the spacing and free volume, and allowing them to move past one another even at lower temperatures. Addition of plasticizer can effectively take control over polymer chain dynamics and dominate the amounts of the associated free volume so that the increased mobility of polymer ends is not apparent.<sup id="cite_ref-54" class="reference"><a href="#cite_note-54"><span class="cite-bracket">&#91;</span>54<span class="cite-bracket">&#93;</span></a></sup> The addition of nonreactive <a href="/wiki/Side_chain" title="Side chain">side groups</a> to a polymer can also make the chains stand off from one another, reducing <i>T</i><sub>g</sub>. If a plastic with some desirable properties has a <i>T</i><sub>g</sub> that is too high, it can sometimes be combined with another in a <a href="/wiki/Copolymer" title="Copolymer">copolymer</a> or <a href="/wiki/Composite_material" title="Composite material">composite material</a> with a <i>T</i><sub>g</sub> below the temperature of intended use. Note that some plastics are used at high temperatures, e.g., in automobile engines, and others at low temperatures.<sup id="cite_ref-PVC_32-11" class="reference"><a href="#cite_note-PVC-32"><span class="cite-bracket">&#91;</span>32<span class="cite-bracket">&#93;</span></a></sup> </p> <figure class="mw-default-size mw-halign-left" typeof="mw:File/Thumb"><a href="/wiki/File:Rubber_plateau.svg" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/8/85/Rubber_plateau.svg/220px-Rubber_plateau.svg.png" decoding="async" width="220" height="138" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/8/85/Rubber_plateau.svg/330px-Rubber_plateau.svg.png 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/8/85/Rubber_plateau.svg/440px-Rubber_plateau.svg.png 2x" data-file-width="400" data-file-height="250" /></a><figcaption>Stiffness versus temperature</figcaption></figure><p>In <a href="/wiki/Viscoelasticity" title="Viscoelasticity">viscoelastic</a> materials, the presence of liquid-like behavior depends on the properties of and so varies with rate of applied load, i.e., how quickly a force is applied. The <a href="/wiki/Silicone" title="Silicone">silicone</a> toy <a href="/wiki/Silly_Putty" title="Silly Putty">Silly Putty</a> behaves quite differently depending on the time rate of applying a force: pull slowly and it flows, acting as a heavily viscous liquid; hit it with a hammer and it shatters, acting as a glass. </p><p>On cooling, <a href="/wiki/Rubber" class="mw-redirect" title="Rubber">rubber</a> undergoes a <i>liquid-glass transition</i>, which has also been called a <i>rubber-glass transition</i>. </p> <div class="mw-heading mw-heading2"><h2 id="Mechanics_of_vitrification">Mechanics of vitrification</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=13" title="Edit section: Mechanics of vitrification"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <style data-mw-deduplicate="TemplateStyles:r1236090951">.mw-parser-output .hatnote{font-style:italic}.mw-parser-output div.hatnote{padding-left:1.6em;margin-bottom:0.5em}.mw-parser-output .hatnote i{font-style:normal}.mw-parser-output .hatnote+link+.hatnote{margin-top:-0.5em}@media print{body.ns-0 .mw-parser-output .hatnote{display:none!important}}</style><div role="note" class="hatnote navigation-not-searchable">Main article: <a href="/wiki/Vitrification" title="Vitrification">Vitrification</a></div> <p>Molecular motion in condensed matter can be represented by a <a href="/wiki/Fourier_series" title="Fourier series">Fourier series</a> whose physical interpretation consists of a <a href="/wiki/Superposition_principle" title="Superposition principle">superposition</a> of <a href="/wiki/Longitudinal_wave" title="Longitudinal wave">longitudinal</a> and <a href="/wiki/Transverse_wave" title="Transverse wave">transverse</a> <a href="/wiki/Wave" title="Wave">waves</a> of atomic displacement with varying directions and wavelengths. In monatomic systems, these waves are called <i><a href="/wiki/Density" title="Density">density</a> <a href="https://en.wiktionary.org/wiki/fluctuation" class="extiw" title="wikt:fluctuation">fluctuations</a></i>. (In polyatomic systems, they may also include <a href="https://en.wiktionary.org/wiki/composition" class="extiw" title="wikt:composition">compositional</a> fluctuations.)<sup id="cite_ref-55" class="reference"><a href="#cite_note-55"><span class="cite-bracket">&#91;</span>55<span class="cite-bracket">&#93;</span></a></sup> </p><p>Thus, <a href="/wiki/Thermal_motion" class="mw-redirect" title="Thermal motion">thermal motion</a> in liquids can be decomposed into elementary <a href="/wiki/Longitudinal_wave" title="Longitudinal wave">longitudinal vibrations</a> (or acoustic <a href="/wiki/Phonon" title="Phonon">phonons</a>) while <a href="/wiki/Transverse_wave" title="Transverse wave">transverse vibrations</a> (or shear waves) were originally described only in <a href="/wiki/Elasticity_(physics)" title="Elasticity (physics)">elastic</a> solids exhibiting the highly ordered crystalline state of matter. In other words, simple liquids cannot support an applied force in the form of a <a href="/wiki/Shearing_stress" class="mw-redirect" title="Shearing stress">shearing stress</a>, and will yield mechanically via macroscopic <a href="/wiki/Plastic_deformation" class="mw-redirect" title="Plastic deformation">plastic deformation</a> (or viscous flow). Furthermore, the fact that a <a href="/wiki/Solid" title="Solid">solid</a> deforms locally while retaining its <a href="/wiki/Stiffness" title="Stiffness">rigidity</a> – while a <a href="/wiki/Liquid" title="Liquid">liquid</a> yields to macroscopic <a href="/wiki/Viscous_flow" class="mw-redirect" title="Viscous flow">viscous flow</a> in response to the application of an applied <a href="/wiki/Shearing_force" class="mw-redirect" title="Shearing force">shearing force</a> – is accepted by many as the mechanical distinction between the two.<sup id="cite_ref-56" class="reference"><a href="#cite_note-56"><span class="cite-bracket">&#91;</span>56<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-57" class="reference"><a href="#cite_note-57"><span class="cite-bracket">&#91;</span>57<span class="cite-bracket">&#93;</span></a></sup> </p><p>The inadequacies of this conclusion, however, were pointed out by Frenkel in his revision of the <a href="/wiki/Kinetic_theory_of_solids" class="mw-redirect" title="Kinetic theory of solids">kinetic theory of solids</a> and the <a href="/wiki/Theory_of_elasticity" class="mw-redirect" title="Theory of elasticity">theory of elasticity</a> in <a href="/wiki/Liquid" title="Liquid">liquids</a>. This revision follows directly from the continuous characteristic of the <a href="/wiki/Viscoelastic" class="mw-redirect" title="Viscoelastic">viscoelastic</a> crossover from the liquid state into the solid one when the transition is not accompanied by crystallization—ergo the supercooled <a href="/wiki/Viscous_liquid" title="Viscous liquid">viscous liquid</a>. Thus we see the intimate correlation between transverse acoustic phonons (or shear waves) and the onset of rigidity upon <a href="/wiki/Vitrification" title="Vitrification">vitrification</a>, as described by Bartenev in his mechanical description of the vitrification process.<sup id="cite_ref-D_58-0" class="reference"><a href="#cite_note-D-58"><span class="cite-bracket">&#91;</span>58<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-59" class="reference"><a href="#cite_note-59"><span class="cite-bracket">&#91;</span>59<span class="cite-bracket">&#93;</span></a></sup> </p><p>The velocities of longitudinal acoustic phonons in condensed matter are directly responsible for the <a href="/wiki/Thermal_conductivity" class="mw-redirect" title="Thermal conductivity">thermal conductivity</a> that levels out temperature differentials between <a href="/wiki/Compressibility" title="Compressibility">compressed</a> and <a href="/wiki/Thermal_expansion" title="Thermal expansion">expanded</a> volume elements. Kittel proposed that the behavior of glasses is interpreted in terms of an approximately constant "<a href="/wiki/Mean_free_path" title="Mean free path">mean free path</a>" for lattice phonons, and that the value of the mean free path is of the <a href="/wiki/Order_of_magnitude" title="Order of magnitude">order of magnitude</a> of the scale of disorder in the molecular structure of a liquid or solid. The thermal phonon mean free paths or relaxation lengths of a number of glass formers have been plotted versus the glass transition temperature, indicating a linear relationship between the two. This has suggested a new criterion for glass formation based on the value of the phonon mean free path.<sup id="cite_ref-60" class="reference"><a href="#cite_note-60"><span class="cite-bracket">&#91;</span>60<span class="cite-bracket">&#93;</span></a></sup> </p><p>It has often been suggested that <a href="/wiki/Heat_conduction" class="mw-redirect" title="Heat conduction">heat transport</a> in <a href="/wiki/Dielectric" title="Dielectric">dielectric</a> solids occurs through elastic vibrations of the lattice, and that this transport is limited by elastic <a href="/wiki/Scattering" title="Scattering">scattering</a> of acoustic phonons by lattice defects (e.g. randomly spaced vacancies).<sup id="cite_ref-61" class="reference"><a href="#cite_note-61"><span class="cite-bracket">&#91;</span>61<span class="cite-bracket">&#93;</span></a></sup> These predictions were confirmed by experiments on commercial <a href="/wiki/Glasses" title="Glasses">glasses</a> and glass <a href="/wiki/Ceramic_engineering" title="Ceramic engineering">ceramics</a>, where mean free paths were apparently limited by "internal boundary scattering" to length scales of 10–100 micrometres (0.00039–0.00394&#160;in).<sup id="cite_ref-62" class="reference"><a href="#cite_note-62"><span class="cite-bracket">&#91;</span>62<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-63" class="reference"><a href="#cite_note-63"><span class="cite-bracket">&#91;</span>63<span class="cite-bracket">&#93;</span></a></sup> The relationship between these transverse waves and the mechanism of vitrification has been described by several authors who proposed that the onset of correlations between such phonons results in an orientational ordering or "freezing" of local <a href="/wiki/Shear_stress" title="Shear stress">shear stresses</a> in glass-forming liquids, thus yielding the glass transition.<sup id="cite_ref-64" class="reference"><a href="#cite_note-64"><span class="cite-bracket">&#91;</span>64<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading3"><h3 id="Electronic_structure">Electronic structure</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=14" title="Edit section: Electronic structure"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <p>The influence of <a href="/wiki/Heat" title="Heat">thermal</a> <a href="/wiki/Phonon" title="Phonon">phonons</a> and their interaction with <a href="/wiki/Electron" title="Electron">electronic</a> structure is a topic that was appropriately introduced in a discussion of the <a href="/wiki/Electrical_resistance" class="mw-redirect" title="Electrical resistance">resistance</a> of liquid metals. Lindemann's theory of melting is referenced,<sup id="cite_ref-65" class="reference"><a href="#cite_note-65"><span class="cite-bracket">&#91;</span>65<span class="cite-bracket">&#93;</span></a></sup> and it is suggested that the drop in <a href="/wiki/Electrical_resistivity_and_conductivity" title="Electrical resistivity and conductivity">conductivity</a> in going from the <a href="/wiki/Crystal" title="Crystal">crystalline</a> to the liquid state is due to the increased <a href="/wiki/Scattering" title="Scattering">scattering</a> of conduction electrons as a result of the increased <a href="/wiki/Amplitude" title="Amplitude">amplitude</a> of atomic <a href="/wiki/Vibration" title="Vibration">vibration</a>. Such theories of localization have been applied to transport in <a href="/wiki/Metallic_glass" class="mw-redirect" title="Metallic glass">metallic glasses</a>, where the <a href="/wiki/Mean_free_path" title="Mean free path">mean free path</a> of the electrons is very small (on the order of the interatomic spacing).<sup id="cite_ref-66" class="reference"><a href="#cite_note-66"><span class="cite-bracket">&#91;</span>66<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-67" class="reference"><a href="#cite_note-67"><span class="cite-bracket">&#91;</span>67<span class="cite-bracket">&#93;</span></a></sup> </p><p>The formation of a non-crystalline form of a gold-silicon alloy by the method of <a href="/wiki/Splat_quenching" title="Splat quenching">splat quenching</a> from the melt led to further considerations of the influence of electronic structure on glass forming ability, based on the properties of the <a href="/wiki/Metallic_bond" class="mw-redirect" title="Metallic bond">metallic bond</a>.<sup id="cite_ref-68" class="reference"><a href="#cite_note-68"><span class="cite-bracket">&#91;</span>68<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-69" class="reference"><a href="#cite_note-69"><span class="cite-bracket">&#91;</span>69<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-70" class="reference"><a href="#cite_note-70"><span class="cite-bracket">&#91;</span>70<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-71" class="reference"><a href="#cite_note-71"><span class="cite-bracket">&#91;</span>71<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-72" class="reference"><a href="#cite_note-72"><span class="cite-bracket">&#91;</span>72<span class="cite-bracket">&#93;</span></a></sup> </p><p>Other work indicates that the <a href="/wiki/Electron_mobility" title="Electron mobility">mobility</a> of localized <a href="/wiki/Electron" title="Electron">electrons</a> is enhanced by the presence of dynamic phonon modes. One claim against such a model is that if <a href="/wiki/Chemical_bonds" class="mw-redirect" title="Chemical bonds">chemical bonds</a> are important, the <a href="/wiki/Nearly_free_electron_model" title="Nearly free electron model">nearly free electron models</a> should not be applicable. However, if the model includes the buildup of a <a href="/wiki/Charge_distribution" class="mw-redirect" title="Charge distribution">charge distribution</a> between all pairs of atoms just like a chemical bond (e.g., silicon, when a band is just filled with electrons) then it should apply to <a href="/wiki/Solid" title="Solid">solids</a>.<sup id="cite_ref-73" class="reference"><a href="#cite_note-73"><span class="cite-bracket">&#91;</span>73<span class="cite-bracket">&#93;</span></a></sup> </p><p>Thus, if the <a href="/wiki/Electrical_conductivity" class="mw-redirect" title="Electrical conductivity">electrical conductivity</a> is low, the <a href="/wiki/Mean_free_path" title="Mean free path">mean free path</a> of the electrons is very short. The electrons will only be sensitive to the <a href="/wiki/Short-range_order" class="mw-redirect" title="Short-range order">short-range order</a> in the glass since they do not get a chance to scatter from atoms spaced at large distances. Since the short-range order is similar in glasses and crystals, the electronic energies should be similar in these two states. For alloys with lower resistivity and longer electronic mean free paths, the electrons could begin to sense <sup class="noprint Inline-Template" style="white-space:nowrap;">&#91;<i><a href="/wiki/Wikipedia:Accuracy_dispute#Disputed_statement" title="Wikipedia:Accuracy dispute"><span title="The material near this tag is possibly inaccurate or nonfactual. (July 2019)">dubious</span></a>&#32;&#8211; <a href="/wiki/Talk:Glass_transition#Dubious" title="Talk:Glass transition">discuss</a></i>&#93;</sup> that there is <a href="/wiki/Order_and_disorder_(physics)" class="mw-redirect" title="Order and disorder (physics)">disorder</a> in the glass, and this would raise their energies and destabilize the glass with respect to crystallization. Thus, the glass formation tendencies of certain alloys may therefore be due in part to the fact that the electron mean free paths are very short, so that only the short-range order is ever important for the energy of the electrons. </p><p>It has also been argued that glass formation in metallic systems is related to the "softness" of the interaction potential between unlike atoms. Some authors, emphasizing the strong similarities between the local structure of the glass and the corresponding crystal, suggest that chemical bonding helps to stabilize the amorphous structure.<sup id="cite_ref-74" class="reference"><a href="#cite_note-74"><span class="cite-bracket">&#91;</span>74<span class="cite-bracket">&#93;</span></a></sup><sup id="cite_ref-75" class="reference"><a href="#cite_note-75"><span class="cite-bracket">&#91;</span>75<span class="cite-bracket">&#93;</span></a></sup> </p><p>Other authors have suggested that the electronic structure yields its influence on glass formation through the directional properties of bonds. Non-crystallinity is thus favored in elements with a large number of <a href="/wiki/Polymorphism_(materials_science)" class="mw-redirect" title="Polymorphism (materials science)">polymorphic</a> forms and a high degree of <a href="/wiki/Chemical_bond" title="Chemical bond">bonding</a> <a href="/wiki/Anisotropy" title="Anisotropy">anisotropy</a>. Crystallization becomes more unlikely as bonding anisotropy is increased from <a href="/wiki/Isotropic" class="mw-redirect" title="Isotropic">isotropic</a> <a href="/wiki/Metal" title="Metal">metallic</a> to <a href="/wiki/Anisotropic" class="mw-redirect" title="Anisotropic">anisotropic</a> <a href="/wiki/Metal" title="Metal">metallic</a> to <a href="/wiki/Covalent" class="mw-redirect" title="Covalent">covalent</a> bonding, thus suggesting a relationship between the <a href="/wiki/Chemical_family" class="mw-redirect" title="Chemical family">group number</a> in the <a href="/wiki/Periodic_table" title="Periodic table">periodic table</a> and the glass forming ability in <a href="/wiki/Chemical_element" title="Chemical element">elemental</a> <a href="/wiki/Solid" title="Solid">solids</a>.<sup id="cite_ref-76" class="reference"><a href="#cite_note-76"><span class="cite-bracket">&#91;</span>76<span class="cite-bracket">&#93;</span></a></sup> </p> <div class="mw-heading mw-heading2"><h2 id="See_also">See also</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=15" title="Edit section: See also"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <ul><li><a href="/wiki/Gardner_transition" title="Gardner transition">Gardner transition</a></li> <li><a href="/wiki/Glass_formation" title="Glass formation">Glass formation</a></li></ul> <div class="mw-heading mw-heading2"><h2 id="References">References</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Glass_transition&amp;action=edit&amp;section=16" title="Edit section: References"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <style data-mw-deduplicate="TemplateStyles:r1239543626">.mw-parser-output .reflist{margin-bottom:0.5em;list-style-type:decimal}@media screen{.mw-parser-output .reflist{font-size:90%}}.mw-parser-output .reflist .references{font-size:100%;margin-bottom:0;list-style-type:inherit}.mw-parser-output .reflist-columns-2{column-width:30em}.mw-parser-output .reflist-columns-3{column-width:25em}.mw-parser-output .reflist-columns{margin-top:0.3em}.mw-parser-output .reflist-columns ol{margin-top:0}.mw-parser-output .reflist-columns li{page-break-inside:avoid;break-inside:avoid-column}.mw-parser-output .reflist-upper-alpha{list-style-type:upper-alpha}.mw-parser-output .reflist-upper-roman{list-style-type:upper-roman}.mw-parser-output .reflist-lower-alpha{list-style-type:lower-alpha}.mw-parser-output .reflist-lower-greek{list-style-type:lower-greek}.mw-parser-output .reflist-lower-roman{list-style-type:lower-roman}</style><div class="reflist reflist-columns references-column-width" style="column-width: 30em;"> <ol class="references"> <li id="cite_note-1"><span class="mw-cite-backlink"><b><a href="#cite_ref-1">^</a></b></span> <span class="reference-text"><style data-mw-deduplicate="TemplateStyles:r1238218222">.mw-parser-output cite.citation{font-style:inherit;word-wrap:break-word}.mw-parser-output .citation q{quotes:"\"""\"""'""'"}.mw-parser-output .citation:target{background-color:rgba(0,127,255,0.133)}.mw-parser-output .id-lock-free.id-lock-free a{background:url("//upload.wikimedia.org/wikipedia/commons/6/65/Lock-green.svg")right 0.1em center/9px no-repeat}.mw-parser-output .id-lock-limited.id-lock-limited a,.mw-parser-output .id-lock-registration.id-lock-registration a{background:url("//upload.wikimedia.org/wikipedia/commons/d/d6/Lock-gray-alt-2.svg")right 0.1em center/9px no-repeat}.mw-parser-output .id-lock-subscription.id-lock-subscription a{background:url("//upload.wikimedia.org/wikipedia/commons/a/aa/Lock-red-alt-2.svg")right 0.1em center/9px no-repeat}.mw-parser-output .cs1-ws-icon a{background:url("//upload.wikimedia.org/wikipedia/commons/4/4c/Wikisource-logo.svg")right 0.1em center/12px 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Polymer Science Learning Center. Archived from <a rel="nofollow" class="external text" href="http://pslc.ws/macrog/tg.htm">the original</a> on 2019-01-15<span class="reference-accessdate">. Retrieved <span class="nowrap">2009-10-15</span></span>.</cite><span title="ctx_ver=Z39.88-2004&amp;rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Abook&amp;rft.genre=unknown&amp;rft.btitle=The+Glass+Transition&amp;rft.pub=Polymer+Science+Learning+Center&amp;rft_id=http%3A%2F%2Fpslc.ws%2Fmacrog%2Ftg.htm&amp;rfr_id=info%3Asid%2Fen.wikipedia.org%3AGlass+transition" class="Z3988"></span></span> </li> <li id="cite_note-Debenedetti-4"><span class="mw-cite-backlink">^ <a href="#cite_ref-Debenedetti_4-0"><sup><i><b>a</b></i></sup></a> <a href="#cite_ref-Debenedetti_4-1"><sup><i><b>b</b></i></sup></a></span> <span class="reference-text"><link rel="mw-deduplicated-inline-style" href="mw-data:TemplateStyles:r1238218222"><cite id="CITEREFDebenedettiStillinger2001" class="citation journal cs1">Debenedetti, P. 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(2011). <span class="id-lock-registration" title="Free registration required"><a rel="nofollow" class="external text" href="https://www.degruyter.com/downloadpdf/j/pac.2011.83.issue-10/pac-rec-10-11-13/pac-rec-10-11-13.pdf">"Definitions of terms relating to crystalline polymers (IUPAC Recommendations 2011)"</a></span> <span class="cs1-format">(PDF)</span>. <i><a href="/wiki/Pure_and_Applied_Chemistry" title="Pure and Applied Chemistry">Pure and Applied Chemistry</a></i>. <b>83</b> (10): 1831. <a href="/wiki/Doi_(identifier)" class="mw-redirect" title="Doi (identifier)">doi</a>:<a rel="nofollow" class="external text" href="https://doi.org/10.1351%2FPAC-REC-10-11-13">10.1351/PAC-REC-10-11-13</a>. <a href="/wiki/S2CID_(identifier)" class="mw-redirect" title="S2CID (identifier)">S2CID</a>&#160;<a rel="nofollow" class="external text" href="https://api.semanticscholar.org/CorpusID:98823962">98823962</a>. <a rel="nofollow" class="external text" href="https://web.archive.org/web/20180625161113/https://www.degruyter.com/downloadpdf/j/pac.2011.83.issue-10/pac-rec-10-11-13/pac-rec-10-11-13.pdf">Archived</a> <span class="cs1-format">(PDF)</span> from the original on 2018-06-25<span class="reference-accessdate">. Retrieved <span class="nowrap">2018-06-25</span></span>.</cite><span title="ctx_ver=Z39.88-2004&amp;rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Ajournal&amp;rft.genre=article&amp;rft.jtitle=Pure+and+Applied+Chemistry&amp;rft.atitle=Definitions+of+terms+relating+to+crystalline+polymers+%28IUPAC+Recommendations+2011%29&amp;rft.volume=83&amp;rft.issue=10&amp;rft.pages=1831&amp;rft.date=2011&amp;rft_id=info%3Adoi%2F10.1351%2FPAC-REC-10-11-13&amp;rft_id=https%3A%2F%2Fapi.semanticscholar.org%2FCorpusID%3A98823962%23id-name%3DS2CID&amp;rft.au=Meille+Stefano%2C+V.&amp;rft.au=Allegra%2C+G.&amp;rft.au=Geil+Phillip%2C+H.&amp;rft.au=He%2C+J.&amp;rft.au=Hess%2C+M.&amp;rft.au=Jin%2C+J.-I.&amp;rft.au=Kratochv%C3%ADl%2C+P.&amp;rft.au=Mormann%2C+W.&amp;rft.au=Stepto%2C+R.&amp;rft_id=https%3A%2F%2Fwww.degruyter.com%2Fdownloadpdf%2Fj%2Fpac.2011.83.issue-10%2Fpac-rec-10-11-13%2Fpac-rec-10-11-13.pdf&amp;rfr_id=info%3Asid%2Fen.wikipedia.org%3AGlass+transition" class="Z3988"></span></span> </li> <li id="cite_note-9"><span class="mw-cite-backlink"><b><a href="#cite_ref-9">^</a></b></span> <span class="reference-text"><a href="/wiki/International_Union_of_Pure_and_Applied_Chemistry" title="International Union of Pure and Applied Chemistry">IUPAC</a>, <i><a href="/wiki/IUPAC_books#Gold_Book" class="mw-redirect" title="IUPAC books">Compendium of Chemical Terminology</a></i>, 2nd ed. (the "Gold Book") (1997). Online corrected version: (2006&#8211;) "<a rel="nofollow" class="external text" href="https://goldbook.iupac.org/terms/view/G02640.html">glass transition</a>". <link rel="mw-deduplicated-inline-style" href="mw-data:TemplateStyles:r1238218222"><a href="/wiki/Doi_(identifier)" class="mw-redirect" title="Doi (identifier)">doi</a>:<a rel="nofollow" class="external text" href="https://doi.org/10.1351%2Fgoldbook.G02640">10.1351/goldbook.G02640</a></span> </li> <li id="cite_note-Hansen&amp;McDonald-10"><span class="mw-cite-backlink"><b><a href="#cite_ref-Hansen&amp;McDonald_10-0">^</a></b></span> <span class="reference-text"><link rel="mw-deduplicated-inline-style" href="mw-data:TemplateStyles:r1238218222"><cite id="CITEREFHansenMcDonald,_I._R.2007" class="citation book cs1">Hansen, J.-P.; McDonald, I. R. (2007). <a rel="nofollow" class="external text" href="https://books.google.com/books?id=Uhm87WZBnxEC"><i>Theory of Simple Liquids</i></a>. 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class="navbox-title" colspan="2"><link rel="mw-deduplicated-inline-style" href="mw-data:TemplateStyles:r1129693374"><style data-mw-deduplicate="TemplateStyles:r1239400231">.mw-parser-output .navbar{display:inline;font-size:88%;font-weight:normal}.mw-parser-output .navbar-collapse{float:left;text-align:left}.mw-parser-output .navbar-boxtext{word-spacing:0}.mw-parser-output .navbar ul{display:inline-block;white-space:nowrap;line-height:inherit}.mw-parser-output .navbar-brackets::before{margin-right:-0.125em;content:"[ "}.mw-parser-output .navbar-brackets::after{margin-left:-0.125em;content:" ]"}.mw-parser-output .navbar li{word-spacing:-0.125em}.mw-parser-output .navbar a>span,.mw-parser-output .navbar a>abbr{text-decoration:inherit}.mw-parser-output .navbar-mini abbr{font-variant:small-caps;border-bottom:none;text-decoration:none;cursor:inherit}.mw-parser-output .navbar-ct-full{font-size:114%;margin:0 7em}.mw-parser-output .navbar-ct-mini{font-size:114%;margin:0 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scope="row" class="navbox-group" style="width:1%">Basics</th><td class="navbox-list-with-group navbox-list navbox-odd hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/Glass" title="Glass">Glass</a></li> <li><a class="mw-selflink selflink">Glass transition</a></li> <li><a href="/wiki/Supercooling" title="Supercooling">Supercooling</a></li></ul> </div></td></tr><tr><th scope="row" class="navbox-group" style="width:1%">Formulation</th><td class="navbox-list-with-group navbox-list navbox-even hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/AgInSbTe" title="AgInSbTe">AgInSbTe</a></li> <li><a href="/wiki/Bioglass" class="mw-redirect" title="Bioglass">Bioglass</a></li> <li><a href="/wiki/Borophosphosilicate_glass" title="Borophosphosilicate glass">Borophosphosilicate glass</a></li> <li><a href="/wiki/Borosilicate_glass" title="Borosilicate glass">Borosilicate glass</a></li> <li><a href="/wiki/Ceramic_glaze" title="Ceramic glaze">Ceramic glaze</a></li> <li><a href="/wiki/Chalcogenide_glass" title="Chalcogenide glass">Chalcogenide glass</a></li> <li><a href="/wiki/Cobalt_glass" title="Cobalt glass">Cobalt glass</a></li> <li><a href="/wiki/Cranberry_glass" title="Cranberry glass">Cranberry glass</a></li> <li><a href="/wiki/Crown_glass_(optics)" title="Crown glass (optics)">Crown glass</a></li> <li><a href="/wiki/Flint_glass" title="Flint glass">Flint glass</a></li> <li><a href="/wiki/Fluorosilicate_glass" title="Fluorosilicate glass">Fluorosilicate glass</a></li> <li><a href="/wiki/Fused_quartz" title="Fused quartz">Fused quartz</a></li> <li><a href="/wiki/GeSbTe" title="GeSbTe">GeSbTe</a></li> <li><a href="/wiki/Cranberry_glass" title="Cranberry glass">Gold ruby glass</a></li> <li><a href="/wiki/Lead_glass" title="Lead glass">Lead glass</a></li> <li><a href="/wiki/Milk_glass" title="Milk glass">Milk glass</a></li> <li><a href="/wiki/Phosphosilicate_glass" title="Phosphosilicate glass">Phosphosilicate glass</a></li> <li><a href="/wiki/Photochromic_lens" title="Photochromic lens">Photochromic lens glass</a></li> <li><a href="/wiki/Glass#Silicate_glass" title="Glass">Silicate glass</a></li> <li><a href="/wiki/Soda%E2%80%93lime_glass" title="Soda–lime glass">Soda–lime glass</a></li> <li><a href="/wiki/Sodium_hexametaphosphate" title="Sodium hexametaphosphate">Sodium hexametaphosphate</a></li> <li><a href="/wiki/Sodium_silicate" title="Sodium silicate">Soluble glass</a></li> <li><a href="/wiki/Tellurite_glass" title="Tellurite glass">Tellurite glass</a></li> <li><a href="/wiki/Thoriated_glass" title="Thoriated glass">Thoriated glass</a></li> <li><a href="/wiki/Ultra_low_expansion_glass" title="Ultra low expansion glass">Ultra low expansion glass</a></li> <li><a href="/wiki/Uranium_glass" title="Uranium glass">Uranium glass</a></li> <li><a href="/wiki/Vitreous_enamel" title="Vitreous enamel">Vitreous enamel</a></li> <li><a href="/wiki/Wood%27s_glass" title="Wood&#39;s glass">Wood's glass</a></li> <li><a href="/wiki/ZBLAN" title="ZBLAN">ZBLAN</a></li></ul> </div></td></tr><tr><th scope="row" class="navbox-group" style="width:1%"><a href="/wiki/Glass-ceramic" title="Glass-ceramic">Glass-ceramics</a></th><td class="navbox-list-with-group navbox-list navbox-odd hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/Bioactive_glass" title="Bioactive glass">Bioactive glass</a></li> <li><a href="/wiki/CorningWare" title="CorningWare">CorningWare</a></li> <li><a href="/wiki/Glass-ceramic-to-metal_seals" title="Glass-ceramic-to-metal seals">Glass-ceramic-to-metal seals</a></li> <li><a href="/wiki/Macor" title="Macor">Macor</a></li> <li><a href="/wiki/Zerodur" title="Zerodur">Zerodur</a></li></ul> </div></td></tr><tr><th scope="row" class="navbox-group" style="width:1%">Preparation</th><td class="navbox-list-with-group navbox-list navbox-even hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/Annealing_(glass)" title="Annealing (glass)">Annealing</a></li> <li><a href="/wiki/Chemical_vapor_deposition" title="Chemical vapor deposition">Chemical vapor deposition</a></li> <li><a href="/wiki/Glass_batch_calculation" title="Glass batch calculation">Glass batch calculation</a></li> <li><a href="/wiki/Glass_production" title="Glass production">Glass forming</a></li> <li><a href="/wiki/Glass_production#Hot_end" title="Glass production">Glass melting</a></li> <li><a href="/wiki/Calculation_of_glass_properties" title="Calculation of glass properties">Glass modeling</a></li> <li><a href="/wiki/Ion_implantation" title="Ion implantation">Ion implantation</a></li> <li><a href="/wiki/Liquidus" class="mw-redirect" title="Liquidus">Liquidus temperature</a></li> <li><a href="/wiki/Sol%E2%80%93gel_process" title="Sol–gel process">sol–gel technique</a></li> <li><a href="/wiki/Viscosity#Viscosity_of_amorphous_materials" title="Viscosity">Viscosity</a></li> <li><a href="/wiki/Vitrification" title="Vitrification">Vitrification</a></li></ul> </div></td></tr><tr><th scope="row" class="navbox-group" style="width:1%"><a href="/wiki/Optics" title="Optics">Optics</a></th><td class="navbox-list-with-group navbox-list navbox-odd hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/Achromatic_lens" title="Achromatic lens">Achromat</a></li> <li><a href="/wiki/Dispersion_(optics)" title="Dispersion (optics)">Dispersion</a></li> <li><a href="/wiki/Gradient-index_optics" title="Gradient-index optics">Gradient-index optics</a></li> <li><a href="/wiki/Hydrogen_darkening" title="Hydrogen darkening">Hydrogen darkening</a></li> <li><a href="/wiki/Optical_amplifier" title="Optical amplifier">Optical amplifier</a></li> <li><a href="/wiki/Optical_fiber" title="Optical fiber">Optical fiber</a></li> <li><a href="/wiki/Optical_lens_design" title="Optical lens design">Optical lens design</a></li> <li><a href="/wiki/Photochromic_lens" title="Photochromic lens">Photochromic lens</a></li> <li><a href="/wiki/Photosensitive_glass" title="Photosensitive glass">Photosensitive glass</a></li> <li><a href="/wiki/Refraction" title="Refraction">Refraction</a></li> <li><a href="/wiki/Transparency_and_translucency" title="Transparency and translucency">Transparent materials</a></li></ul> </div></td></tr><tr><th scope="row" class="navbox-group" style="width:1%">Surface<br />modification</th><td class="navbox-list-with-group navbox-list navbox-even hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/Anti-reflective_coating" title="Anti-reflective coating">Anti-reflective coating</a></li> <li><a href="/wiki/Chemically_strengthened_glass" title="Chemically strengthened glass">Chemically strengthened glass</a></li> <li><a href="/wiki/Corrosion#Corrosion_of_glasses" title="Corrosion">Corrosion</a></li> <li><a href="/wiki/Dealkalization" title="Dealkalization">Dealkalization</a></li> <li><a href="/wiki/DNA_microarray" title="DNA microarray">DNA microarray</a></li> <li><a href="/wiki/Hydrogen_darkening" title="Hydrogen darkening">Hydrogen darkening</a></li> <li><a href="/wiki/Insulated_glazing" title="Insulated glazing">Insulated glazing</a></li> <li><a href="/wiki/Porous_glass" title="Porous glass">Porous glass</a></li> <li><a href="/wiki/Self-cleaning_glass" title="Self-cleaning glass">Self-cleaning glass</a></li> <li><a href="/wiki/Sol%E2%80%93gel_process" title="Sol–gel process">sol–gel technique</a></li> <li><a href="/wiki/Tempered_glass" title="Tempered glass">Tempered glass</a></li></ul> </div></td></tr><tr><th scope="row" class="navbox-group" style="width:1%">Diverse<br />topics</th><td class="navbox-list-with-group navbox-list navbox-odd hlist" style="width:100%;padding:0"><div style="padding:0 0.25em"> <ul><li><a href="/wiki/Conservation_and_restoration_of_glass_objects" title="Conservation and restoration of glass objects">Conservation and restoration of glass objects</a></li> <li><a href="/wiki/Glass-coated_wire" title="Glass-coated wire">Glass-coated wire</a></li> <li><a href="/wiki/Safety_glass" title="Safety glass">Safety glass</a></li> <li><a href="/wiki/Glass_databases" title="Glass databases">Glass databases</a></li> <li><a href="/wiki/Glass_electrode" title="Glass electrode">Glass electrode</a></li> <li><a href="/wiki/Glass_fiber_reinforced_concrete" title="Glass fiber reinforced concrete">Glass fiber reinforced concrete</a></li> <li><a href="/wiki/Glass_ionomer_cement" title="Glass ionomer cement">Glass ionomer cement</a></li> <li><a href="/wiki/Glass_microsphere" title="Glass microsphere">Glass microspheres</a></li> <li><a href="/wiki/Fiberglass" title="Fiberglass">Glass-reinforced plastic</a></li> <li><a href="/wiki/Glass_cloth" title="Glass cloth">Glass cloth</a></li> <li><a href="/wiki/Glass-to-metal_seal" title="Glass-to-metal seal">Glass-to-metal seal</a></li> <li><a href="/wiki/Porous_glass" title="Porous glass">Porous glass</a></li> <li><a href="/wiki/Pre-preg" title="Pre-preg">Pre-preg</a></li> <li><a href="/wiki/Prince_Rupert%27s_drop" title="Prince Rupert&#39;s drop">Prince Rupert's drops</a></li> <li><a href="/wiki/Radioactive_waste#Vitrification" title="Radioactive waste">Radioactive waste vitrification</a></li> <li><a href="/wiki/Windshield" title="Windshield">Windshield</a></li> <li><a href="/wiki/Glass_fiber" title="Glass fiber">Glass fiber</a></li></ul> </div></td></tr></tbody></table></div> <div class="navbox-styles"><link rel="mw-deduplicated-inline-style" href="mw-data:TemplateStyles:r1129693374"><link rel="mw-deduplicated-inline-style" href="mw-data:TemplateStyles:r1236075235"></div><div role="navigation" class="navbox authority-control" aria-label="Navbox" style="padding:3px"><table class="nowraplinks hlist navbox-inner" style="border-spacing:0;background:transparent;color:inherit"><tbody><tr><th scope="row" class="navbox-group" style="width:1%"><a href="/wiki/Help:Authority_control" 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