Department of Engineering and Applied Sciences, University of Bergamo , Viale Marconi 5, 24044 Dalmine (BG), Italy.
ISTEC CNR - Institute of Science and Technology for Ceramics , Via Granarolo 64, 48018 Faenza (RA), Italy.
Langmuir. 2016 Jun 28;32(25):6255-62. doi: 10.1021/acs.langmuir.6b01117. Epub 2016 Jun 13.
It is well known that a superhydrophobic surface may not be able to repel impacting droplets because of the so-called Cassie-to-Wenzel transition. It has been proven that a critical value of the receding contact angle (θR) exists for the complete rebound of water, recently experimentally measured to be 100° for a large range of impact velocities. On the contrary, in the present work, no rebound was observed when low-surface-tension liquids such as hexadecane (σ = 27.5 mN/m at 25 °C) are concerned, even for very low impact velocities and very high values of θR and low contact angle hysteresis. Therefore, the critical threshold of θR ≈ 100° does not sound acceptable for all liquids and for all hydrophobic surfaces. For the same Weber numbers, a Cassie-to-Wenzel state transition occurs after the impact as a result of the easier penetration of low-surface-tension fluids in the surface structure. Hence, a criterion for the drop rebound of low-surface-tension liquids must consider not only the contact angle values with surfaces but also their surface tension and viscosity. This suggests that, even if it is possible to produce surfaces with enhanced static repellence against oils and organics, generally the realization of synthetic materials with self-cleaning and antisticking abilities in dynamic phenomena, such as spray impact, remains an unsolved task. Moreover, it is demonstrated that the chemistry of the surface, the physicochemical interactions with the liquid drops, and the possible wettability gradient of the surface asperity also play important roles in determining the critical Weber number above which impalement occurs. Therefore, the classical numerical simulations of drop impact on dry surfaces are definitively not able to capture the final outcomes of the impact for all possible fluids if the surface topology and chemistry and/or the wettability gradient in the surface structure are not properly reflected.
众所周知,由于所谓的 Cassie-to-Wenzel 转变,超疏水表面可能无法排斥撞击液滴。已经证明,对于水的完全回弹,存在一个后退接触角(θR)的临界值,最近在很大的冲击速度范围内实验测量到为 100°。相反,在目前的工作中,当涉及低表面张力液体(如十六烷(σ=27.5 mN/m 在 25°C))时,即使对于非常低的冲击速度和非常高的θR 值和低接触角滞后,也观察不到回弹。因此,临界阈值θR ≈ 100°对于所有液体和所有疏水性表面似乎都不可接受。对于相同的韦伯数,由于低表面张力液体更容易渗透到表面结构中,因此在撞击后会发生 Cassie-to-Wenzel 状态转变。因此,低表面张力液体回弹的标准不仅必须考虑与表面的接触角值,还必须考虑其表面张力和粘度。这表明,即使有可能生产出对油和有机物具有增强静态排斥性的表面,但在喷雾冲击等动态现象中实现具有自清洁和抗粘性能力的合成材料仍然是一个未解决的任务。此外,还表明表面化学、与液滴的物理化学相互作用以及表面粗糙度的可能润湿性梯度在确定发生刺穿的临界韦伯数方面也起着重要作用。因此,如果表面拓扑和化学性质以及/或表面结构中的润湿性梯度没有得到适当反映,那么经典的液滴冲击干表面的数值模拟肯定无法捕获所有可能流体的最终冲击结果。