Peculiarities of fluctuations in glass-forming liquids

I. V. Blazhnov, N. P. Malomuzh
{"title":"Peculiarities of fluctuations in glass-forming liquids","authors":"I. V. Blazhnov, N. P. Malomuzh","doi":"10.1117/12.486682","DOIUrl":null,"url":null,"abstract":"The present work is devoted to the investigation of the peculiarities of fluctuations in glass-forming liquids. To justify our reasons we will anlayze the character of molecular light scattering in silicate glass, that was the object of experimental study. Our approach to the problem of fluctuations in glasses and liquids near the glassification point is based on the following general motivations. Highly-viscous and glass-like states of glass-forming liquids are in the metastable region, which correspond to the crystal state of a system in the equilibrium. The behavior of a system is determined by relations between two characteristic times: τw(T) and τe, where the former is the waiting time for the critical nucleus and τe is the time for cooling the system from the melting temperature to the spinodal temperature Ts at the same pressure. If τe <(<<) τw(Ts) the system smoothly passes to the glass-like state. Here two factors are very important. In metastable region of a system the nuclei of the new phase (crystal) appear. The fraction volume φ(T), occupied by them, depends on the cooling rate. The value of φ is the less the more quick cooling the system is. However, below the spinodal in accordance with thermodynamics the homogeneous states of a system are impossible. The existence of the lasts contradicts the stabilty conditons. From here we conclude that typical glass-like states in a system should be microinhomogeneous. Similar conclusion is confirmed by the results of experimental study of the structure. Now we should note that the strongly anisotropic interaction between nonspyherical molecules of glass-forming liquids leads to considerable coupling between the translational and orientational degrees of freedom in a system. In other words the changes of density is accompanied by the corresponding modulation of molecular orientations. Due to strong increasing the shear viscosity at approaching the glassification point some configurations of the centers of mass and the orientations of molecules froze. More exactyly, only weak thermal deviations of coordinates of molecules from their local equilibrium values are possible. The radical change of the global molecular configuration requires exponentially large time. Thus, the combination of frozen and thermal fluctuations is the distinctive feature of glass-like state of a system. It is necessary to note that different ways of cooling of a system lead to nonequivalent frozen fluctuations.","PeriodicalId":205850,"journal":{"name":"International School on Spectroscopy of Molecules and Crystals","volume":"248 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2002-12-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International School on Spectroscopy of Molecules and Crystals","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.486682","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3

Abstract

The present work is devoted to the investigation of the peculiarities of fluctuations in glass-forming liquids. To justify our reasons we will anlayze the character of molecular light scattering in silicate glass, that was the object of experimental study. Our approach to the problem of fluctuations in glasses and liquids near the glassification point is based on the following general motivations. Highly-viscous and glass-like states of glass-forming liquids are in the metastable region, which correspond to the crystal state of a system in the equilibrium. The behavior of a system is determined by relations between two characteristic times: τw(T) and τe, where the former is the waiting time for the critical nucleus and τe is the time for cooling the system from the melting temperature to the spinodal temperature Ts at the same pressure. If τe <(<<) τw(Ts) the system smoothly passes to the glass-like state. Here two factors are very important. In metastable region of a system the nuclei of the new phase (crystal) appear. The fraction volume φ(T), occupied by them, depends on the cooling rate. The value of φ is the less the more quick cooling the system is. However, below the spinodal in accordance with thermodynamics the homogeneous states of a system are impossible. The existence of the lasts contradicts the stabilty conditons. From here we conclude that typical glass-like states in a system should be microinhomogeneous. Similar conclusion is confirmed by the results of experimental study of the structure. Now we should note that the strongly anisotropic interaction between nonspyherical molecules of glass-forming liquids leads to considerable coupling between the translational and orientational degrees of freedom in a system. In other words the changes of density is accompanied by the corresponding modulation of molecular orientations. Due to strong increasing the shear viscosity at approaching the glassification point some configurations of the centers of mass and the orientations of molecules froze. More exactyly, only weak thermal deviations of coordinates of molecules from their local equilibrium values are possible. The radical change of the global molecular configuration requires exponentially large time. Thus, the combination of frozen and thermal fluctuations is the distinctive feature of glass-like state of a system. It is necessary to note that different ways of cooling of a system lead to nonequivalent frozen fluctuations.
玻璃形成液体波动的特性
本文致力于研究玻璃形成液体波动的特性。为了证明我们的理由,我们将分析作为实验研究对象的硅酸盐玻璃中的分子光散射特性。我们处理玻璃和液体在玻璃化点附近波动问题的方法是基于以下一般动机。形成玻璃的液体的高粘性和类玻璃态处于亚稳区,这对应于系统在平衡状态下的晶体状态。系统的行为由两个特征时间τw(T)和τe之间的关系决定,其中τw(T)是临界核的等待时间,τe是在相同压力下系统从熔化温度冷却到旋量温度Ts的时间。如果τe <(<<) τw(Ts),则系统平稳地过渡到类玻璃态。这里有两个因素非常重要。在系统的亚稳区出现新相(晶体)的核。它们所占的分数体积φ(T)取决于冷却速率。φ值越小,系统冷却越快。然而,根据热力学,在旋量以下,系统的齐次状态是不可能的。最后的存在与稳定条件相矛盾。由此我们得出结论,系统中典型的类玻璃态应该是微非均匀的。该结构的实验研究结果也证实了类似的结论。现在我们应该注意到,玻璃形成液体的非球形分子之间的强各向异性相互作用导致了系统中平移自由度和取向自由度之间的相当大的耦合。换句话说,密度的变化伴随着分子取向的相应调制。在接近玻璃化点时,由于剪切粘度的强烈增加,一些质心构型和分子取向冻结。更确切地说,只有分子坐标与局部平衡值的微弱热偏差是可能的。整体分子构型的根本变化需要指数级大的时间。因此,冻结波动和热波动的结合是系统类玻璃态的显著特征。有必要指出,系统的不同冷却方式会导致非等效冻结波动。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信