Moghimi Esmaeel, Schofield Andrew B, Petekidis George
FORTH/IESL and Department of Materials Science and Technology, University of Crete, 71110 Heraklion, Greece.
School of Physics and Astronomy, The University of Edinburgh, EH9 3FD, Scotland, United Kingdom.
J Phys Condens Matter. 2021 Jun 3;33(28). doi: 10.1088/1361-648X/abfb8d.
We examine the macroscopic deformation of a colloidal depletion gel subjected to a step shear stress. Three regimes are identified depending on the magnitude of the applied stress: (i) for stresses below yield stress, the gel undergoes a weak creep in which the bulk deformation grows sublinearly with time similar to crystalline and amorphous solids. For stresses above yield stress, when the bulk deformation exceeds approximately the attraction range, the sublinear increase of deformation turns into a superlinear growth which signals the onset of non-linear rearrangements and yielding of the gel. However, the long-time creep after such superlinear growth shows two distinct behaviors: (ii) under strong stresses, a viscous flow is reached in which the strain increases linearly with time. This indicates a complete yielding and flow of the gel. In stark contrast, (iii) for weak stresses, the gel after yielding starts to resolidify. More homogenous gels that are produced through enhancement of either interparticle attraction strength or strain amplitude of the oscillatory preshear, resolidify gradually. In contrast, in gels that are more heterogeneous resolidification occurs abruptly. We also find that heterogenous gels produced by oscillatory preshear at intermediate strain amplitude yield in a two-step process. Finally, the characteristic time for the onset of delayed yielding is found to follow a two-step decrease with increasing stress. This is comprised of an exponential decrease at low stresses, during which bond reformation is decisive and resolidification is detected, and a power law decrease at higher stresses where bond breaking and particle rearrangements dominate.
我们研究了受到阶跃剪切应力作用的胶体耗尽凝胶的宏观变形。根据所施加应力的大小可识别出三种状态:(i) 对于低于屈服应力的应力,凝胶经历弱蠕变,其中整体变形随时间呈亚线性增长,类似于晶体和非晶态固体。对于高于屈服应力的应力,当整体变形超过大约吸引力范围时,变形的亚线性增加转变为超线性增长,这标志着凝胶开始出现非线性重排和屈服。然而,这种超线性增长后的长时间蠕变表现出两种不同的行为:(ii) 在强应力下,达到粘性流动状态,应变随时间线性增加。这表明凝胶完全屈服并流动。与之形成鲜明对比的是,(iii) 对于弱应力,屈服后的凝胶开始重新固化。通过增强颗粒间吸引力强度或振荡预剪切的应变幅度而产生的更均匀的凝胶会逐渐重新固化。相比之下,在更不均匀的凝胶中,重新固化会突然发生。我们还发现,在中等应变幅度下通过振荡预剪切产生的不均匀凝胶在两步过程中屈服。最后,发现延迟屈服开始的特征时间随着应力增加呈两步下降。这包括在低应力下的指数下降,在此期间键的重新形成起决定性作用且可检测到重新固化,以及在高应力下的幂律下降,此时键的断裂和颗粒重排起主导作用。