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剪切堵塞的致密悬浮液中两种不同应力松弛机制的起源。

Origin of Two Distinct Stress Relaxation Regimes in Shear Jammed Dense Suspensions.

作者信息

Barik Sachidananda, Majumdar Sayantan

机构信息

Soft Condensed Matter Group, Raman Research Institute, Bangalore 560080, Karnataka, India.

出版信息

Phys Rev Lett. 2022 Jun 24;128(25):258002. doi: 10.1103/PhysRevLett.128.258002.

Abstract

Many dense particulate suspensions show a stress induced transformation from a liquidlike state to a solidlike shear jammed (SJ) state. However, the underlying particle-scale dynamics leading to such striking, reversible transition of the bulk remains unknown. Here, we study transient stress relaxation behaviour of SJ states formed by a well-characterized dense suspension under a step strain perturbation. We observe a strongly nonexponential relaxation that develops a sharp discontinuous stress drop at short time for high enough peak-stress values. High resolution boundary imaging and normal stress measurements confirm that such stress discontinuity originates from the localized plastic events, whereas system spanning dilation controls the slower relaxation process. We also find an intriguing correlation between the nature of transient relaxation and the steady-state shear jamming phase diagram obtained from the Wyart-Cates model.

摘要

许多致密颗粒悬浮液表现出一种由应力诱导的从类液态到类固态剪切堵塞(SJ)状态的转变。然而,导致这种显著的、可逆的整体转变的潜在颗粒尺度动力学仍然未知。在这里,我们研究了在阶跃应变扰动下由特征明确的致密悬浮液形成的SJ状态的瞬态应力松弛行为。我们观察到一种强烈的非指数松弛,对于足够高的峰值应力值,在短时间内会出现急剧的不连续应力下降。高分辨率边界成像和法向应力测量证实,这种应力不连续性源于局部塑性事件,而系统范围的膨胀控制着较慢的松弛过程。我们还发现了瞬态松弛的性质与从怀亚特 - 凯茨模型获得的稳态剪切堵塞相图之间的有趣关联。

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