Zhdanov S A, Starov V M, Sobolev V D, Velarde M G
Department of Chemical Engineering, Loughborough University, Loughborough, Leicestershire LE11 3TU, UK.
J Colloid Interface Sci. 2003 Aug 15;264(2):481-9. doi: 10.1016/S0021-9797(03)00520-4.
Experimental investigations were carried out on the spreading of small drops of aqueous SDS solutions over dry thin porous substrates (nitrocellulose membranes) in the case of partial wetting. The time evolution was monitored of the radii of both the drop base and the wetted area inside the porous substrate. The total duration of the spreading process was subdivided into three stages: the first stage: the drop base expands until the maximum value of the drop base is reached, the contact angle rapidly decreases during this stage; the second stage: the radius of the drop base remains constant and the contact angle decreases linearly with time; the third stage: the drop base shrinks and the contact angle remains constant. The wetted area inside the porous substrate expends during the whole spreading process. Appropriate scales were used with a plot of the dimensionless radii of the drop base, of the wetted area inside the porous substrate and the dynamic contact angle on the dimensionless time. Our experimental data show: the overall time of the spreading of drops of SDS solution over dry thin porous substrates decreases with the increase of surfactant concentration; the difference between advancing and hydrodynamic receding contact angles decreases with the surfactant concentration increase; the constancy of the contact angle during the third stage of spreading has nothing to do with the hysteresis of contact angle, but determined by the hydrodynamic reasons. It is shown using independent spreading experiments of the same drops on nonporous nitrocellulose substrate that the static receding contact angle is equal to zero, which supports our conclusion on the hydrodynamic nature of the hydrodynamic receding contact angle on porous substrates.
在部分润湿的情况下,对SDS水溶液小液滴在干燥的薄多孔基底(硝酸纤维素膜)上的铺展进行了实验研究。监测了液滴底部半径和多孔基底内部润湿区域半径随时间的变化。铺展过程的总持续时间分为三个阶段:第一阶段:液滴底部扩展直至达到最大值,在此阶段接触角迅速减小;第二阶段:液滴底部半径保持不变,接触角随时间线性减小;第三阶段:液滴底部收缩,接触角保持不变。多孔基底内部的润湿区域在整个铺展过程中不断扩大。使用适当的标度绘制了液滴底部的无量纲半径、多孔基底内部润湿区域的无量纲半径以及动态接触角随无量纲时间的变化曲线。我们的实验数据表明:SDS溶液液滴在干燥薄多孔基底上的铺展总时间随表面活性剂浓度的增加而减少;前进接触角与流体动力学后退接触角之间的差值随表面活性剂浓度的增加而减小;铺展第三阶段接触角的恒定与接触角滞后无关,而是由流体动力学原因决定的。通过在无孔硝酸纤维素基底上对相同液滴进行独立铺展实验表明,静态后退接触角等于零,这支持了我们关于多孔基底上流体动力学后退接触角的流体动力学性质的结论。