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The glass–liquid transition, or glass transition, is the gradual and reversible transition in amorphous materials (or in amorphous regions within semicrystalline materials) from a hard and relatively brittle "glassy" state into a viscous or "rubbery" state as the temperature is increased. An amorphous solid that exhibits a glass transition is called a…
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glass temperature transition liquid tg state material polymer polymers amorphous time glasses free cooling supercooled temperatures materials thermal energy crystalline
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Glass transition | is a | matter of ongoing research | 0.90 | text |
| volume | instance of | which is a first-order phase transition in the Ehrenfest classification and involves discontinuities in thermodynamic and dynamic properties | 0.80 | text |
| energy | instance of | which is a first-order phase transition in the Ehrenfest classification and involves discontinuities in thermodynamic and dynamic properties | 0.80 | text |
| and viscosity | instance of | which is a first-order phase transition in the Ehrenfest classification and involves discontinuities in thermodynamic and dynamic properties | 0.80 | text |
| dynamic mechanical analysis can be used to measure the glass transition temperature | instance of | Techniques | 0.80 | text |
| dielectric spectroscopy | instance of | and the size of these cooperatively rearranging regions grows as the temperature decreases.Experimental evidence for dynamic heterogeneity has been obtained using techniques | 0.80 | text |
| multidimensional nuclear magnetic resonance | instance of | and the size of these cooperatively rearranging regions grows as the temperature decreases.Experimental evidence for dynamic heterogeneity has been obtained using techniques | 0.80 | text |
| and single-molecule fluorescence measurements | instance of | and the size of these cooperatively rearranging regions grows as the temperature decreases.Experimental evidence for dynamic heterogeneity has been obtained using techniques | 0.80 | text |
| all of which reveal spatial variations in relaxation dynamics near the glass transition | instance of | and the size of these cooperatively rearranging regions grows as the temperature decreases.Experimental evidence for dynamic heterogeneity has been obtained using techniques | 0.80 | text |
| B | instance of | addition of elements | 0.80 | text |
| Na | instance of | addition of elements | 0.80 | text |
| K or Ca to a silica glass | instance of | addition of elements | 0.80 | text |
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