Viscosity of Silica and Doped Silica Melts: Evidence for a Crossover Temperature
Autor: | John C. Mauro, Charles R. Kurkjian, Prabhat K. Gupta, Walter Kob |
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Přispěvatelé: | Laboratoire Charles Coulomb (L2C), Université de Montpellier (UM)-Centre National de la Recherche Scientifique (CNRS) |
Rok vydání: | 2021 |
Předmět: |
Materials science
Crossover supercooled liquids Thermodynamics FOS: Physical sciences 02 engineering and technology Activation energy 01 natural sciences Condensed Matter::Disordered Systems and Neural Networks Viscosity symbols.namesake Impurity 0103 physical sciences Materials Chemistry [PHYS.COND.CM-DS-NN]Physics [physics]/Condensed Matter [cond-mat]/Disordered Systems and Neural Networks [cond-mat.dis-nn] [PHYS.COND.CM-SM]Physics [physics]/Condensed Matter [cond-mat]/Statistical Mechanics [cond-mat.stat-mech] ComputingMilieux_MISCELLANEOUS glass 010302 applied physics Arrhenius equation Condensed Matter - Materials Science Dopant Doping Materials Science (cond-mat.mtrl-sci) Disordered Systems and Neural Networks (cond-mat.dis-nn) Condensed Matter - Disordered Systems and Neural Networks 021001 nanoscience & nanotechnology Condensed Matter::Soft Condensed Matter silica viscosity Ceramics and Composites symbols 0210 nano-technology Glass transition |
Zdroj: | Journal of the American Ceramic Society Journal of the American Ceramic Society, Wiley, 2021, pp.0. ⟨10.1111/jace.18090⟩ |
ISSN: | 0002-7820 1551-2916 |
DOI: | 10.48550/arxiv.2108.09487 |
Popis: | Silica is known as the archetypal strong liquid, exhibiting an Arrhenius viscosity curve with a high glass transition temperature and constant activation energy. However, given the ideally isostatic nature of the silica network, the presence of even a small concentration of defects can lead to a significant decrease in both the glass transition temperature and activation energy for viscous flow. To understand the impact of trace level dopants on the viscosity of silica, we measure the viscosity-temperature curves for seven silica glass samples having different impurities, including four natural and three synthetic samples. Depending on the type of dopant, the glass transition temperature can vary by nearly 300 K. A common crossover is found for all viscosity curves around ~2200-2500 K, which we attribute to a change of the transport mechanism in the melt from being dominated by intrinsic defects at high temperature to dopant-induced defects at low temperatures. |
Databáze: | OpenAIRE |
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