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变形和静态硬球胶体玻璃中的局部剪切转变

Local shear transformations in deformed and quiescent hard-sphere colloidal glasses.

作者信息

Jensen K E, Weitz D A, Spaepen F

机构信息

Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA.

Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA and School of Engineering and Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2014 Oct;90(4):042305. doi: 10.1103/PhysRevE.90.042305. Epub 2014 Oct 10.

Abstract

We perform a series of deformation experiments on a monodisperse, hard-sphere colloidal glass while simultaneously following the three-dimensional trajectories of roughly 50,000 individual particles with a confocal microscope. In each experiment, we deform the glass in pure shear at a constant strain rate [(1-5)×10(-5) s(-1)] to maximum macroscopic strains (5%-10%) and then reverse the deformation at the same rate to return to zero macroscopic strain. We also measure three-dimensional particle trajectories in an identically prepared quiescent glass in which the macroscopic strain is always zero. We find that shear transformation zones exist and are active in both sheared and quiescent colloidal glasses, revealed by a distinctive fourfold signature in spatial autocorrelations of the local shear strain. With increasing shear, the population of local shear transformations develops more quickly than in a quiescent glass and many of these transformations are irreversible. When the macroscopic strain is reversed, we observe partial elastic recovery, followed by plastic deformation of the opposite sign, required to compensate for the irreversibly transformed regions. The average diameter of the shear transformation zones in both strained and quiescent glasses is slightly more than two particle diameters.

摘要

我们对单分散硬球胶体玻璃进行了一系列变形实验,同时用共聚焦显微镜跟踪大约50000个单个粒子的三维轨迹。在每个实验中,我们以恒定应变率[(1 - 5)×10^(-5)s^(-1)]在纯剪切状态下使玻璃变形至最大宏观应变(5% - 10%),然后以相同速率反向变形以使宏观应变恢复到零。我们还在一个同样制备的静态玻璃中测量三维粒子轨迹,该静态玻璃中的宏观应变始终为零。我们发现剪切转变区存在且在剪切和静态胶体玻璃中均处于活跃状态,这通过局部剪切应变的空间自相关中独特的四重特征得以揭示。随着剪切的增加,局部剪切转变的数量比在静态玻璃中发展得更快,并且其中许多转变是不可逆的。当宏观应变反向时,我们观察到部分弹性恢复,随后是相反符号的塑性变形,以补偿不可逆转变的区域。应变和静态玻璃中剪切转变区的平均直径略大于两个粒子直径。

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