The iso-structural viscosity, configurational entropy and fragility of oxide liquids

被引:73
|
作者
Yue, Yuanzheng [1 ]
机构
[1] Univ Aalborg, Sect Chem, DK-9000 Aalborg, Denmark
关键词
Oxide glasses; Clorimetry; Viscosity; Configurational entropy; Fragility; CALCIUM ALUMINOSILICATE MELTS; GLASS-FORMING LIQUIDS; TEMPERATURE-DEPENDENCE; RHEOLOGICAL PROPERTIES; FICTIVE TEMPERATURE; BOROSILICATE MELTS; HEAT-CAPACITY; RELAXATION; TRANSITION; SILICATES;
D O I
10.1016/j.jnoncrysol.2009.01.032
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
This paper describes how the fragility of a liquid is linked to the ratio between the energy barrier (E-eq) for the equilibrium Viscous behavior and that (E-iso) for the non-equilibrium iso-structural viscous behavior. Using the concept of iso-structural Viscosity, two functions describing the variation of the configurational entropy (S-c) with temperature (T) are obtained from the Avramov-Milchev (AM) and the Vogel-Fulcher-Tammann (VFT) viscosity equations, respectively. The two S-c(T) functions exhibit different relations to the liquid fragility. The AM S-c(T) function is a power function with the exponent of F - 1, where F is the AM fragility index. In this case, S-c vanishes at T = 0 K. For the VFT function, S-c vanishes as T is lowered to a finite temperature T-0, whereas it reaches the maximum Value S-c,S-max at infinitively high T. S-c.max is proportional to the VFT fragility index. Thus, the VFT equation is not only a dynamical, but also a thermodynamic model. It is proved that for oxide liquids, the VFT equation describes viscosity data better than the AM equation, provided the pre-exponential factor eta(0) is fixed to a generally accepted value, e.g., 10(-3.5) Pa s. (C) 2009 Elsevier B.V. All rights reserved.
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页码:737 / 744
页数:8
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