Hayami Mii Fukuda, Menju Takashi, Ide Takeshi, Uchida Tatsuro, Adachi Yasuhisa
Infrastructure Systems Research and Development Center, Toshiba Infrastructure Systems & Solutions Corporation, 1, Toshiba, Fuchu 183-8511, Tokyo, Japan.
Energy Systems Research and Development Center, Toshiba Energy Systems & Solutions Corporation, 1-20, Kansei, Tsurumi, Yokohama 230-0034, Kanagawa, Japan.
Gels. 2024 Jan 10;10(1):49. doi: 10.3390/gels10010049.
We have constructed an outer-cylinder-rotating Couette device for high-speed shear flow in laminar flow conditions and visualized the structure formation and subsequent rearrangement of PACl (flocculant made of aluminum hydroxide gel) and kaolinite flocs by visible light imaging. In a previous report, we analyzed the case of relatively low shear rate (-value = 29 1/s) and confirmed that the flocculation process could be separated into two stages: a floc growth stage and a breakup/rearrangement stage. Once the large bulky flocs that reached the maximum size appeared, they rearranged and densified through structural fracture and rearrangement. In this report, this process was further investigated by conducting experiments under two different high shear rates (58 and 78 1/s) at which breakup and rearrangement became more pronounced, and three different aluminum kaolinite ratios (ALT ratios) that were over and under the optimum dosage (neutralization point by Zeta potential). Visualization results confirmed that, during the growth stage, the flocculation rate could be approximated by a scaling relationship between floc size and elapsed time, which depended on the ALT ratio. After reaching the maximum size, the floc rapidly became compact and dense following adsorption of the gel, incorporating fine fragments from erosion breakup. The over and under dosages created a lot of fragments of erosion breakup, but less so in the optimum dosage. In the optimum ALT ratio, fragments did not remain because they were incorporated into the flocs and densified, and the floc size was thought to be maintained. The floc circularity distribution peaked at around 0.6 and 1, suggesting that the flocs were spherical in shape due to erosion breakup.
我们构建了一种用于层流条件下高速剪切流的外筒旋转库埃特装置,并通过可见光成像观察了聚合氯化铝(由氢氧化铝凝胶制成的絮凝剂)和高岭土絮体的结构形成及随后的重排过程。在之前的一份报告中,我们分析了相对较低剪切速率(值 = 29 1/s)的情况,并证实絮凝过程可分为两个阶段:絮凝生长阶段和破碎/重排阶段。一旦达到最大尺寸的大而松散的絮体出现,它们就会通过结构断裂和重排进行重新排列并致密化。在本报告中,通过在两种不同的高剪切速率(58 和 78 1/s,此时破碎和重排更为明显)以及三种不同的铝高岭土比例(ALT 比例,高于和低于最佳剂量(由 Zeta 电位确定的中和点))下进行实验,对这一过程进行了进一步研究。可视化结果证实,在生长阶段,絮凝速率可以通过絮体尺寸与经过时间之间的标度关系来近似,这取决于 ALT 比例。达到最大尺寸后,絮体在凝胶吸附后迅速变得紧凑和致密,并入了侵蚀破碎产生的细小碎片。过量和不足剂量会产生大量侵蚀破碎的碎片,但在最佳剂量下则较少。在最佳 ALT 比例下,碎片不会残留,因为它们被并入絮体并致密化,并且絮体尺寸被认为得以维持。絮体的圆形度分布在约 0.6 和 1 处达到峰值,表明由于侵蚀破碎,絮体呈球形。