Vassileva Nikolina D, van den Ende Dirk, Mugele Frieder, Mellema Jorrit
Physics of Complex Fluids, Department of Science and Technology, Institute of Mechanics, Processes and Control-Twente, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands.
Langmuir. 2007 Feb 27;23(5):2352-61. doi: 10.1021/la0625087.
We consider single two-dimensional aggregates containing glass particles trapped at a water/oil or water/air interface. Two modes for aggregate break-up are observed: break-up by fragmentation into a few parts and break-up by erosion of single particles. We have studied the critical shear rate for these modes as a function of the aggregate size. Two different particle sizes were used. The smaller particles, with a radius of 65 microm, form aggregates that break up predominantly by erosion at a shear rate between 0.5 and 0.7 s(-1). This value hardly depends on the size of the aggregates. The larger particles, with a radius of 115 microm, form aggregates that break by erosion or by fragmentation. In both modes, the critical shear rate again depends only weakly on the size of the aggregates and ranges between 1.6 and 2.2 s(-1). Also the structural changes inside the aggregate before break-up were studied. The aggregate behavior at the water/air and water/oil interfaces is quite similar. The critical shear rate for break up was also modeled. The model shows in both modes a weak dependence of the critical shear rate on the aggregate size, which is consistent with the experimental observations. The kinetics of the erosion process was also modeled and compared with the experimentally obtained time dependence of the aggregate size. The differences in the large and small particle systems can be attributed to the occurrence of friction forces between the particles, which one expects to be much larger for the large particle system, due to the stronger two-particle interaction.
我们考虑含有被困在水/油或水/气界面处玻璃颗粒的单个二维聚集体。观察到聚集体破裂的两种模式:破碎成几个部分的破裂和单个颗粒侵蚀导致的破裂。我们研究了这些模式的临界剪切速率与聚集体尺寸的函数关系。使用了两种不同粒径的颗粒。半径为65微米的较小颗粒形成的聚集体主要在0.5至0.7 s⁻¹的剪切速率下通过侵蚀而破裂。该值几乎不依赖于聚集体的尺寸。半径为115微米的较大颗粒形成的聚集体通过侵蚀或破碎而破裂。在这两种模式下,临界剪切速率同样仅微弱地依赖于聚集体的尺寸,范围在1.6至2.2 s⁻¹之间。还研究了聚集体在破裂前内部的结构变化。聚集体在水/气和水/油界面处的行为非常相似。还对破裂的临界剪切速率进行了建模。该模型在两种模式下均显示临界剪切速率对聚集体尺寸的依赖性较弱,这与实验观察结果一致。还对侵蚀过程的动力学进行了建模,并与实验获得的聚集体尺寸的时间依赖性进行了比较。大颗粒和小颗粒系统中的差异可归因于颗粒之间摩擦力的出现,由于更强的双颗粒相互作用,预计大颗粒系统中的摩擦力要大得多。