On the glass transition temperature T against molar volume V plotting in arsenoselenide glasses

Autor: V. Balitska, Catherine Boussard-Plédel, Bruno Bureau, J. Szlęzak, V. Boyko, Oleh Shpotyuk, Ya. Shpotyuk, M. Shpotyuk
Přispěvatelé: National Polytechnic University of Lviv (LPNU), Rzeszow University of Technology, Ivan Franko National University of Lviv, Institut des Sciences Chimiques de Rennes (ISCR), Université de Rennes (UR)-Institut National des Sciences Appliquées - Rennes (INSA Rennes), Institut National des Sciences Appliquées (INSA)-Institut National des Sciences Appliquées (INSA)-Ecole Nationale Supérieure de Chimie de Rennes (ENSCR)-Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS), Jan Dlugosz University in Czestochowa, Ministry of Education and Science of Ukraine, MESU, Centre National de la Recherche Scientifique (CNRS)-Institut de Chimie du CNRS (INC)-Université de Rennes 1 (UR1), Université de Rennes (UNIV-RENNES)-Université de Rennes (UNIV-RENNES)-Ecole Nationale Supérieure de Chimie de Rennes (ENSCR)-Institut National des Sciences Appliquées - Rennes (INSA Rennes), Institut National des Sciences Appliquées (INSA)-Université de Rennes (UNIV-RENNES)-Institut National des Sciences Appliquées (INSA)
Rok vydání: 2020
Předmět:
Zdroj: Journal of Non-Crystalline Solids
Journal of Non-Crystalline Solids, 2020, 528, pp.119758. ⟨10.1016/j.jnoncrysol.2019.119758⟩
Journal of Non-Crystalline Solids, Elsevier, 2020, 528, pp.119758. ⟨10.1016/j.jnoncrysol.2019.119758⟩
ISSN: 0022-3093
DOI: 10.1016/j.jnoncrysol.2019.119758
Popis: International audience; Dependence of glass transition temperature Tg (K) on overall mean bonding energy E (kJ/mol) in arsenoselenide glass reexamined under per-atom calculations is shown to obey linearized master equation Tg ≅ 418⋅(E–1.13). Compositional variations in Tg against molar volume Vm are plotted for g-AsxSe100- x taken within (0 ≤ x ≤ 65) domain assuming preferential cohesive Van der Waals (VDW) bonding between network-constituting entities. The Tg values are found to vary as inverse-αth power of Vm, attaining distinct values for different networks, in part, 0D-molecular (α=6/3= 2), 1D-chained (α=5/3), 2D-layered (α=4/3), and 3D-spatial (α=3/3=1). These variations originated from macroscopic geometry of VDW interaction are linearized in log-log presentation for networks dominated with chain-like 1D-entities (0 ≤ x
Databáze: OpenAIRE