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Drop-size effects on coalescence of two equal-sized drops in a head-on collision

机译:液滴大小对正面碰撞中两个相等大小的液滴合并的影响

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When two equal-sized drops collide in a two-dimensional extensional flow of a second immiscible fluid, the time required to drain the thin film between the drops prior to coalescence is referred to as the drainage time. In a previously proposed scaling theory [H. Yang , Phys. Fluids 13, 1087-1106 (2001)] we found that in the low Ca regime, the dimensionless product of the film drainage time (t(d)) and the applied shear rate (G) should scale as Ca-1/2. Yet, recent numerical simulations contradict this result and show that the dimensionless drainage time (t(d)G) in this regime scales as Ca. Furthermore, the existing experiments suggest that the drainage time may become independent of Ca in the limit Ca < 1. In this paper, we attempt to address these apparent contradictions. First, we carry out coalescence experiments in a four-roll mill for significantly smaller drops than have heretofore been studied. Our results show that as R is decreased for a fixed Ca range, the scaling exponent m in the correlation t(d)G similar to Ca-m falls in the range 1 <= m <= 4/3, but never exhibits a value smaller than 1. Thus, we corroborate the numerically predicted scaling of t(d)G with Ca in the low Ca regime. We then reexamine the scaling theory. We find that the disagreement between scaling theories and the numerical simulations (as well as the present experiments) ultimately emanates from a fundamental limitation in the definition of the drainage time. Finally, our experiments show that the scaling exponent unexpectedly increases when the viscosity ratio is increased from lambda=0.19 to lambda=6.8 for a drop radius smaller than 27 mu m. We show that one must evidently account for interfacial "slip" between the drops and the surrounding film to account for this observed increase in m. We define a slip parameter that gives an a priori estimate of the importance of slip in the experimental data.
机译:当两个相等大小的液滴在第二种不互溶的流体的二维扩展流中发生碰撞时,在聚结之前排出液滴之间的薄膜所需的时间称为排出时间。在先前提出的缩放理论[H。杨物理流体13,1087-1106(2001)]我们发现,在低Ca条件下,薄膜排水时间(t(d))和施加的剪切速率(G)的无量纲乘积应按Ca-1 / 2缩放。然而,最近的数值模拟与该结果相矛盾,并且表明在这种情况下无因次排水时间(t(d)G)与Ca成比例。此外,现有的实验表明,排水时间可能在Ca <1的极限范围内与Ca无关。在本文中,我们试图解决这些明显的矛盾。首先,我们在四辊磨机中进行聚结实验,所得到的液滴比以前研究的要小得多。我们的结果表明,当在固定的Ca范围内R减小时,与Ca-m相似的相关性t(d)G中的缩放指数m落在1 <= m <= 4/3的范围内,但从不显示值小于1。因此,我们证实了在低Ca条件下,t(d)G与Ca的数值预测比例。然后,我们重新审查缩放理论。我们发现,定标理论与数值模拟(以及本实验)之间的分歧最终源于排水时间定义的基本局限。最后,我们的实验表明,当液滴半径小于27μm时,粘度比从λ= 0.19增大到λ= 6.8时,结垢指数会意外增加。我们表明,一个人显然必须考虑到液滴与周围膜之间的界面“滑移”,以解决这一观察到的m增大。我们定义了一个转差参数,可以对实验数据中转差的重要性进行先验估计。

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