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非胶体水凝胶颗粒悬浮液在液-固转变时的粘弹性

Viscoelasticity of non-colloidal hydrogel particle suspensions at the liquid-solid transition.

作者信息

Shewan Heather M, Yakubov Gleb E, Bonilla Mauricio R, Stokes Jason R

机构信息

School of Chemical Engineering, The University of Queensland, Brisbane, QLD 4072, Australia.

出版信息

Soft Matter. 2021 May 19;17(19):5073-5083. doi: 10.1039/d0sm01624a.

Abstract

Suspensions of soft particles transition from a viscous fluid to a soft material upon increases in phase volume. The criteria defining the transition to this jammed state are difficult to define due to the porous and deformable nature of soft particles. Here, we characterise the rheology of aqueous suspensions of industrially relevant non-colloidal, polydisperse, frictional agarose microgels and evaluate shear and viscoelastic behaviour across a range of phase volumes from the dilute regime to the highly concentrated regime. In order to model the viscoelastic response of suspensions without free fitting parameters, the random close packing volume fraction (φrcp) and the particle modulus are determined, respectively, from particle size distribution measurements and direct measurements of reduced elastic modulus of individual particles (Erp) using Atomic Force Microscopy. It is found that at φrcp, previously shown to correspond to divergence of the viscosity, also corresponds to the suspension transition from a viscous to viscoelastic fluid. However, the transition to a jammed solid-like state (φj) occurs at phase volumes exceeding this value (i.e. φj > φrcp). The suspension modulus and its sudden growth at φj are well-predicted by the Evans and Lips model that incorporates the Erp of the hydrogel particles. This rheological behaviour showing a dual transition is reminiscent of two families of systems: (i) colloidal suspensions and (ii) frictional-adhesive non-colloidal suspensions. However, it does not strictly follow either case. We propose that the width of the transition region is dictated by frictional contact, particle size distribution and particle modulus, and plan to further probe this in future work.

摘要

随着相体积的增加,软颗粒悬浮液会从粘性流体转变为软材料。由于软颗粒具有多孔和可变形的特性,定义向这种堵塞状态转变的标准很难确定。在这里,我们对工业上相关的非胶体、多分散、有摩擦的琼脂糖微凝胶的水悬浮液的流变学进行了表征,并评估了从稀溶液状态到高浓度状态范围内一系列相体积下的剪切和粘弹性行为。为了在没有自由拟合参数的情况下对悬浮液的粘弹性响应进行建模,分别从粒度分布测量以及使用原子力显微镜对单个颗粒的折合弹性模量(Erp)进行直接测量来确定随机密堆积体积分数(φrcp)和颗粒模量。研究发现,在φrcp处,先前已表明其对应于粘度的发散,同时也对应于悬浮液从粘性流体向粘弹性流体的转变。然而,向类似堵塞固体状态(φj)的转变发生在超过该值的相体积处(即φj > φrcp)。包含水凝胶颗粒Erp的Evans和Lips模型能够很好地预测悬浮模量及其在φj处的突然增长。这种呈现双重转变的流变行为让人联想到两类系统:(i)胶体悬浮液和(ii)有摩擦 - 粘附性的非胶体悬浮液。然而,它并不严格遵循这两种情况中的任何一种。我们提出转变区域的宽度由摩擦接触、粒度分布和颗粒模量决定,并计划在未来的工作中进一步探究这一点。

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