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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Activated Hopping,Barrier Fluctuations,and Heterogeneity in Glassy Suspensions and Liquids
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Activated Hopping,Barrier Fluctuations,and Heterogeneity in Glassy Suspensions and Liquids

机译:悬浮液和液体中的活化跳变,壁垒波动和非均质性

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Our entropic barrier hopping theory of glassy hard sphere colloidal suspensions is extended to include heterogeneity within a simple trap model framework.The origin of local domains,their size,and the corresponding static barrier fluctuations are attributed to mesoscopic density fluctuations of an amplitude controlled by the bulk compressibility.Based on typical values of the density fluctuation correlation length in dense liquids,the domain size on which correlated hopping occurs is estimated to be 3-4 particle or molecular diameters.Consequences of barrier fluctuations include an increased average relaxation time,faster diffusion,stretched exponential relaxation,diffusion-viscosity decoupling,and a fractional Stokes-Einstein relation.The common origin of the fluctuation effects is the heterogeneity-induced component of the barrier.For colloidal suspensions in the typically studied volume fraction regime the barrier fluctuations have modest consequences,but significantly larger effects are predicted in the putative glassy regime.A statistical dynamical analysis of domain lifetime suggests that for suspensions the relaxation time of mesoscopic collective density fluctuations is at least as long as the single particle hopping time.A general,model-independent analysis of the single molecule incoherent dynamic structure factor for suspensions and thermal liquids has also been performed in the long time and intermediate wavevector regime.The coupling of single particle density and longitudinal stress fluctuations results in a wavevector-dependent apparent diffusion constant and a dynamic correlation length scale which is strongly temperature dependent and directly related to the translation-rotation decoupling factor.This dynamic length is estimated to be 10 times larger than a molecular diameter for tris-naphthyl benzene near the glass transition temperature but shrinks to a molecular size above the crossover temperature that signals the emergence of collective barriers.
机译:我们将玻璃态硬球体胶体悬浮液的熵垒跳跃理论扩展到包括简单陷阱模型框架中的异质性。局部域的起源,它们的大小以及相应的静态势垒波动归因于介电体密度波动,该波动由电磁场控制。体积可压缩性。基于稠密液体中密度波动相关长度的典型值,估计发生相关跳跃的域大小为3-4个粒子或分子直径。势垒波动的后果包括平均弛豫时间增加,扩散更快,伸展的指数松弛,扩散-粘度解耦和分数斯托克斯-爱因斯坦关系。波动效应的共同起因是屏障的异质性诱导成分。对于通常研究的体积分数状态下的胶体悬浮液,屏障波动适度后果,但影响更大s是在假定的玻璃态下预测的。对畴寿命的统计动力学分析表明,对于悬浮液,介观集合密度波动的弛豫时间至少与单个粒子的跳跃时间一样长。对模型的一般独立于模型的分析悬浮液和热液体的分子非相干动态结构因子也已在长时间和中间波矢范围内进行了研究。单粒子密度和纵向应力波动的耦合导致了波矢依赖的表观扩散常数和动态相关长度标度强烈地取决于温度并且与平移-旋转解耦因子直接相关。此动态长度估计是三萘基苯在玻璃化转变温度附近的分子直径的10倍大,但会缩窄到高于信号传递温度的分子大小集体障碍的出现s。

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