Krzan Marcel, Chattopadhyay Pradipta, Orvalho Sandra, Zednikova Maria
Jerzy Haber Institute of Catalysis and Surface Chemistry, Polish Academy of Sciences, 30-239 Krakow, Poland.
Department of Chemical Engineering, BITS-Pilani, Pilani PIN-333031, Rajasthan, India.
Materials (Basel). 2023 Mar 6;16(5):2125. doi: 10.3390/ma16052125.
The influence of n-alkanol (C2-C10) water solutions on bubble motion was studied in a wide range of concentrations. Initial bubble acceleration, as well as local, maximal and terminal velocities during motion were studied as a function of motion time. Generally, two types of velocity profiles were observed. For low surface-active alkanols (C2-C4), bubble acceleration and terminal velocities diminished with the increase in solution concentration and adsorption coverage. No maximum velocities were distinguished. The situation is much more complicated for higher surface-active alkanols (C5-C10). In low and medium solution concentrations, bubbles detached from the capillary with acceleration comparable to gravitational acceleration, and profiles of the local velocities showed maxima. The terminal velocity of bubbles decreased with increasing adsorption coverage. The heights and widths of the maximum diminished with increasing solution concentration. Much lower initial acceleration values and no maxima presence were observed in the case of the highest n-alkanol concentrations (C5-C10). Nevertheless, in these solutions, the observed terminal velocities were significantly higher than in the case of bubbles moving in solutions of lower concentration (C2-C4). The observed differences were explained by different states of the adsorption layer in the studied solutions, leading to varying degrees of immobilization of the bubble interface, which generates other hydrodynamic conditions of bubble motion.
研究了正构醇(C2 - C10)水溶液在广泛浓度范围内对气泡运动的影响。研究了初始气泡加速度以及运动过程中的局部、最大和终端速度随运动时间的变化。一般来说,观察到两种类型的速度分布。对于低表面活性的烷醇(C2 - C4),气泡加速度和终端速度随着溶液浓度和吸附覆盖率的增加而减小。未区分出最大速度。对于高表面活性的烷醇(C5 - C10),情况要复杂得多。在低和中等溶液浓度下,气泡从毛细管脱离时的加速度与重力加速度相当,局部速度分布显示出最大值。气泡的终端速度随着吸附覆盖率的增加而降低。最大值的高度和宽度随着溶液浓度的增加而减小。在正构醇最高浓度(C5 - C10)的情况下,观察到初始加速度值低得多且不存在最大值。然而,在这些溶液中,观察到的终端速度明显高于在较低浓度(C2 - C4)溶液中气泡运动的情况。观察到的差异是由所研究溶液中吸附层的不同状态解释的,这导致气泡界面的固定程度不同,从而产生气泡运动的其他流体动力学条件。