米叶微结构表面薄液膜上的液滴冲击动力学

Yongze An, Yiyao Hao, Chaoxi Wang, Jinlin Xue, Wei Qiu, Yunfu Chen
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引用次数: 0

摘要

虽然向茎叶喷洒杀虫剂是预防植物病虫害的最有效方法,但液滴在撞击叶片表面时的飞溅是施药过程中药液流失的主要途径之一。此外,由于叶片表面存在微观结构,流动液滴与液膜的碰撞和冲击非常复杂。因此,了解液滴撞击动力学对于改进农药施用过程至关重要。本文建立了一个具有微结构表面的模拟水稻叶片,并采用数值方法研究了液滴对该表面薄液膜的冲击动力学。具体来说,分析了不同液滴直径、液滴速度、液膜厚度和叶片表面微结构尺寸对冲击动力学的影响。结果表明,当液滴撞击具有薄液膜的模拟水稻叶片表面时,会出现扩散、喷射、反弹和飞溅等行为。此外,液滴直径越大、速度越快,形成的树冠的最大高度和直径也越大。此外,液膜越厚,形成的叶冠基部半径越小。当喷射角增大时,液冠高度增加,而基底半径减小。随着微结构肋间距的增大,冠的最大高度先增大后减小,而冠的基底半径则减小。然而,肋深对树冠的基底半径没有明显影响。根据雷诺数、奥恩索尔格数和韦伯数以及无量纲液膜厚度,建立了定量表达沉积、喷射和飞溅现象之间过渡关系的方程。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Droplet impacting dynamics on a thin liquid film on the rice-leaf microstructured surface
Although spraying pesticides onto stems and leaves is the most effective method to prevent plant pests and diseases, the splashing of the droplets upon impact with the leaf surface is one of the main ways that the liquid agent is lost during the application process. Moreover, the collision and impact of flowing droplets with the liquid film are complex owing to the presence of microstructures on the leaf surface. Therefore, understanding the droplet impact dynamics is crucial for improving the pesticide application process. In this paper, a simulated rice leaf with a microstructured surface was established, and the impacting dynamics of a liquid droplet on this surface with thin liquid film were investigated using numerical methods. Specifically, the influences of different droplet diameters, droplet velocities, liquid film thicknesses, and leaf surface microstructure dimensions on the impacting dynamics were analyzed. The results showed that the behavior of spreading, jetting, rebound, and splashing occurred upon when droplets impact the simulated surface of rice leaves with thin liquid film. Moreover, a larger droplet diameter and a higher velocity lead to an increase in both the maximum height and diameter of the formed crown. Additionally, the thicker liquid films result in crowns with a smaller base radius. When the jetting angle increases, the crown height increases while its base radius decreases. With the increase in the rib spacing of microstructure, the maximum crown height initially increases and then decreases, while the crown base radius decreases. However, the rib depth has no significant influence on the base radius of the crown. Equations for the quantitative expression of the transition relationships between the deposition, jetting, and splashing phenomena were established on the basis of the Reynolds number, Ohnesorge number, and Weber number as well as the dimensionless liquid film thickness.
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