Non-equilibrium entropy of glasses formed by continuous cooling

被引:12
作者
Mauro, John C. [1 ]
Gupta, Prabhat K. [2 ]
Loucks, Roger J. [1 ,3 ]
Varshneya, Arun K. [4 ]
机构
[1] Corning Inc, Div Sci & Technol, Corning, NY 14831 USA
[2] Ohio State Univ, Dept Mat Sci & Engn, Columbus, OH 43210 USA
[3] Alfred Univ, Dept Phys & Astron, Alfred, NY 14802 USA
[4] Alfred Univ, New York State Coll Ceram, Alfred, NY 14802 USA
关键词
Glass transition; Modeling and simulation; Structural relaxation; ENERGY LANDSCAPE; STATISTICAL-MECHANICS; SUPERCOOLED LIQUIDS; ENTHALPY LANDSCAPES; BROKEN ERGODICITY; BOLTZMANN ENTROPY; TRANSITION; SYSTEMS; MODEL; THERMODYNAMICS;
D O I
10.1016/j.jnoncrysol.2008.09.044
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
We propose a generalized definition of entropy accounting for the continuous breakdown of ergodicity at the laboratory glass transition. Our approach is applicable through all regimes of glass forming, from the equilibrium liquid state through the glass transition range and into the glassy state at low temperatures. The continuous loss of ergodicity during the laboratory glass transition is accompanied by a loss of entropy as the system gradually becomes trapped in a subset of the configurational phase space. Using a hierarchical master equation approach, We compute the configurational entropy of selenium, a simple but realistic glass-former, for cooling rates covering 25 orders of magnitude, viz., 10(-12) to 10(12) K/s. In all cases, the entropy of glass is zero in the limit of absolute zero temperature, since here the system is necessarily confined to a single microstate. (C) 2009 Elsevier B.V. All rights reserved.
引用
收藏
页码:600 / 606
页数:7
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