Laboratoire de Génie Chimique, Université de Toulouse, CNRS, INPT, UPS, Toulouse, France.
LISBP, Université de Toulouse, CNRS, INRA, INSA, Toulouse, France.
J Colloid Interface Sci. 2017 Apr 1;491:167-178. doi: 10.1016/j.jcis.2016.12.042. Epub 2016 Dec 21.
This paper concerns experimental investigation of the sequenced flocculation of latex particles in a Taylor-Couette reactor. The aim of this work was to investigate the evolution of both the size and the shape of aggregates under sequenced hydrodynamics. A number of studies have focused on the evolution of the aggregate size or size distribution during steps of growth-breakage-regrowth, but aggregates generally experience steps of breakage-regrowth on repeated occasions in real operating conditions (passages near the impeller or during the transfer processes, for example). The experiments conducted in this work consisted thus of an alternation of six steps with alternately low and high shear rates under turbulent conditions. The particle size distributions were monitored throughout the sequencing, and the circularity and convexity (shape parameters) distributions were measured, enabling a more precise description of the entire floc population, rather than a fractal dimension. While the aggregate size distribution was clearly controlled by hydrodynamics, the shape distributions continuously evolved during the sequencing. The main new finding of our work notes the independence between the aggregate shape and hydrodynamics. Indeed, after multiples steps of breakage-regrowth, regardless of the aggregate size distribution and hydrodynamics, the aggregate shape seemed to reach a unique steady-state morphological distribution.
本文关注于在泰勒-库埃特反应器中对胶乳颗粒的序贯絮凝进行实验研究。本工作的目的是研究在序贯流场下,聚集物的尺寸和形状的演变。已有大量研究关注于在生长-破碎-再生长阶段,聚集物尺寸或尺寸分布的演变,但在实际操作条件下,聚集物通常会多次经历破碎-再生长阶段(例如在叶轮附近或在传递过程中)。因此,这项工作中的实验由在湍流条件下交替进行的六个具有交替低剪切率和高剪切率的步骤组成。在整个序列中监测颗粒尺寸分布,并测量了圆度和凸度(形状参数)分布,从而可以更精确地描述整个絮体群体,而不是分形维数。虽然聚集物尺寸分布明显受到流场控制,但形状分布在序列过程中不断演变。我们工作的主要新发现指出了聚集物形状与流场之间的独立性。事实上,经过多次破碎-再生长步骤后,无论聚集物尺寸分布和流场如何,聚集物的形状似乎都达到了独特的稳态形态分布。