自由落体聚结冲击模式下混相流体接触域边界处的细流结构

IF 1.8 Q3 MECHANICS Fluids Pub Date : 2023-09-28 DOI:10.3390/fluids8100269
Yuli D. Chashechkin, Andrey Yu. Ilinykh
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引用次数: 0

摘要

采用照片和视频记录的方法,记录了自由落体液滴在静止目标流体中,当液滴的动能(KEn)超过其有效表面势能(ASPe)时,液滴在聚并碰撞模式下的流动模式和物质分布。研究了空腔形成初期细流结构的演化过程。为了进行颜色配准,观察场由几个矩阵LED和恒定光的光纤光源照射。实验的计划和结果的解释是基于流体力学系统基本方程的完全解的性质,包括能量过程的传递和转换。方程组的完整解描述了波或漩涡以及细射流(韧带、细丝、纤维、细流)的大规模流动成分。在实验中,当合并流体的自由表面被消除时,射流被转换的有效表面势能(ASPe)加速。实验采用水、茜素油墨、高锰酸钾溶液和硫酸铜或硫酸铁滴液在深水中聚结的方法进行。在所有情况下,在初次接触时,液滴开始失去连续性,分裂成一层薄薄的面纱和射流,其速度超过液滴接触速度。随着时间的推移,小液滴的大小越来越大,它们从喷口顶部的尖峰处被抛向空气中。在液体表面,细小的射流留下彩色的痕迹,形成线性和网状结构。穿透空腔底部和壁的部分射流形成中间覆盖层。形成内层的射流被目标流体的界面分开。分子扩散过程使密度差相等,并在靶流体中形成具有明显边界的中间层。当一个淡水滴在同一自来水中等温扩散时,所有注意到的流的结构特征也被可视化。分子扩散过程逐渐使快速变化的合并流体边界变得平滑,合并流体边界在初始阶段具有复杂和不规则的形状。在所有实验中观察到相似的流动模式;然而,流动的几何特征取决于接触流体的个别热力学和动力学参数。
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Fine Flow Structure at the Miscible Fluids Contact Domain Boundary in the Impact Mode of Free-Falling Drop Coalescence
Registration of the flow pattern and the matter distribution of a free falling liquid drop in a target fluid at rest in the impact mode of coalescence when the kinetic energy (KEn) of the drop exceeds its available surface potential energy (ASPe) was carried out by photo and video recording. We studied the evolution of the fine flow structure at the initial stage of the cavity formation. To carry out color registration, the observation field was illuminated by several matrix LED and fiber-optic sources of constant light. The planning of experiments and interpretation of the results were based on the properties of the complete solutions of the fundamental equations of a fluid mechanics system, including the transfer and conversion of energy processes. Complete solutions of the system of equations describe large-scale flow components that are waves or vortices as well as thin jets (ligaments, filaments, fibers, trickles). In experiments, the jets are accelerated by the converted available surface potential energy (ASPe) when the free surfaces of merging fluids were eliminated. The experiments were performed with the coalescence of water, solutions of alizarin ink, potassium permanganate, and copper sulfate or iron sulfate drops in deep water. In all cases, at the initial contact, the drop begins to lose its continuity and breaks up into a thin veil and jets, the velocity of which exceeds the drop contact velocity. Small droplets, the size of which grows with time, are thrown into the air from spikes at the jet tops. On the surface of the liquid, the fine jets leave colored traces that form linear and reticular structures. Part of the jets penetrating through the bottom and wall of the cavity forms an intermediate covering layer. The jets forming the inside layer are separated by interfaces of the target fluid. The processes of molecular diffusion equalize the density differences and form an intermediate layer with sharp boundaries in the target fluid. All noted structural features of the flow are also visualized when a fresh water drop isothermally spreads in the same tap water. Molecular diffusion processes gradually smooth out the fast-changing boundary of merging fluids, which at the initial stage has a complex and irregular shape. Similar flow patterns were observed in all performed experiments; however, the geometric features of the flow depend on the individual thermodynamic and kinetic parameters of the contacting fluids.
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来源期刊
Fluids
Fluids Engineering-Mechanical Engineering
CiteScore
3.40
自引率
10.50%
发文量
326
审稿时长
12 weeks
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