Department of Chemical and Biological Engineering, Illinois Institute of Technology, Chicago, Illinois 60616, USA.
Langmuir. 2012 Nov 27;28(47):16274-84. doi: 10.1021/la302702g. Epub 2012 Nov 14.
Recent studies on the spreading phenomena of liquid dispersions of nanoparticles (nanofluids) have revealed that the self-layering and two-dimensional structuring of nanoparticles in the three-phase contact region exert structural disjoining pressure, which drives the spreading of nanofluids by forming a continuous wedge film between the liquid (e.g., oil) and solid surface. Motivated by the practical applications of the phenomenon and experimental results reported in Part I of this two-part series, we thoroughly investigated the spreading dynamics of nanofluids against an oil drop on a solid surface. With the Laplace equation as a starting point, the spreading process is modeled by Navier-Stokes equations through the lubrication approach, which considers the structural disjoining pressure, gravity, and van der Waals force. The temporal interface profile and advancing inner contact line velocity of nanofluidic films are analyzed through varying the effective nanoparticle concentration, the outer contact angle, the effective nanoparticle size, and capillary pressure. It is found that a fast and spontaneous advance of the inner contact line movement can be obtained by increasing the nanoparticle concentration, decreasing the nanoparticle size, and/or decreasing the interfacial tension. Once the nanofluidic film is formed, the advancing inner contact line movement reaches a constant velocity, which is independent of the outer contact angle if the interfacial tension is held constant.
最近对纳米颗粒(纳米流体)液体分散体的扩散现象的研究表明,纳米颗粒在三相接触区域中的自分层和二维结构化会产生结构分离压力,这种压力通过在液体(例如油)和固体表面之间形成连续的楔形膜来驱动纳米流体的扩散。受该现象的实际应用和本系列两部分的第一部分中报告的实验结果的启发,我们彻底研究了纳米流体在固体表面上对油滴的扩散动力学。从拉普拉斯方程出发,通过润滑方法利用纳维-斯托克斯方程对扩展过程进行建模,该方法考虑了结构分离压力、重力和范德华力。通过改变有效纳米颗粒浓度、外部接触角、有效纳米颗粒尺寸和毛细压力来分析纳米流体膜的时间界面轮廓和前进内部接触线速度。研究发现,通过增加纳米颗粒浓度、减小纳米颗粒尺寸和/或减小界面张力,可以获得快速而自发的内部接触线运动的推进。一旦形成纳米流体膜,前进的内部接触线运动就会达到恒定速度,如果界面张力保持不变,则与外部接触角无关。