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Dynamics of dewetting and bubble attachment to rough hydrophobic surfaces - Measurements and modelling

机译:粗疏水表面脱模和泡沫附着的动态 - 测量和造型

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The influence of solid surface roughness (hydrophobic Teflon (R)) on the timescale of the ascending air bubble (R-b = 0.74 mm) attachment and the kinetics of the spreading of the three-phase contact (TPC - gas/liquid/solid) line was studied. The moment of the rising bubble collision with a horizontal Teflon (R) plate immersed in ultrapure water was monitored using fast video recordings (4000 fps). It was shown that, depending on the solid surface roughness, the time of the TPC formation was significantly different. Similarly to our previous studies, it was shorter for higher roughnesses. Using high-frequency video acquisition, an additional factor, kinetics of the spreading of the TPC line associated with various bubble shape changes during TPC formation, could be determined. The registered attachment kinetics and bubble shape variations were very reproducible for smooth and very rough Teflon (R) surfaces, whereas for Teflon (R) of intermediate roughness, up to five different attachment scenarios were observed, with a relatively large standard deviation of time of TPC formation. Numerical calculations used for simulation of the bubble collisions with a horizontal solid wall With precisely controlled hydrodynamic boundary conditions revealed that the experimentally observed timescales of the bubble attachment and spectacular bubble shape variations can be accurately (qualitatively) reproduced for each roughness of the Teflon (R) plate studied. Good agreement between experimental and numerical data is, in our opinion, rather strong evidence for air-induced rupture of the liquid film formed between the colliding bubble and the hydrophobic solid plate. This supports the hypothesis that depending on the solid surface roughness, different amounts of air entrapped in solid surface irregularities could drastically change the solid surface hydrodynamic boundary conditions and, consequently, the kinetics of spreading and formation of the TPC. (C) 2015 Elsevier Ltd. All rights reserved.
机译:固体表面粗糙度(疏水性Teflon(R))对三相触点的次脉冲泡(RB = 0.74mm)附着的时间尺度(TPC - 气/液/固体)管线的动力学研究过。使用快速录像(4000 FPS)监测与浸入超纯水中的水平Teflon板的上升气泡碰撞的时刻。结果表明,取决于固体表面粗糙度,TPC形成的时间显着不同。与我们以前的研究同样,较高的粗糙度较短。可以确定使用高频视频采集,可以确定与TPC形成期间与各种气泡形状改变相关的TPC线的额外因素,传播的动力学。注册的附件动力学和气泡形状变化对于光滑且非常粗糙的Teflon(R)表面非常可再现,而对于中间粗糙度的Teflon(R),观察到多达五种不同的附着方案,具有相对较大的标准偏差TPC形成。用于模拟与水平实心壁的气泡碰撞模拟具有精确控制的流体动力边界条件的泡沫碰撞的数值揭示了可以准确地(定性地)对泡泡附着和壮观的气泡形状变化的实验观察到的时间尺度(R)(R )板材研究。在我们看来,实验和数值数据之间的良好一致性是在碰撞泡沫和疏水固体板之间形成的液体膜的空气诱导破裂的良好证据。这支持假设,取决于固体表面粗糙度,在固体表面不规则中捕获的不同空气可能会大大改变固体表面流体动力边界条件,因此,TPC的扩散和形成动力学。 (c)2015 Elsevier Ltd.保留所有权利。

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