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arXiv 2103.16230physics.flu-dyn
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基于显式体积扩散概念的界面流模型

Modelling of Interfacial Flows Based on An Explicit Volume Diffusion Concept

B. Wang, M. J. Cleary, A. R. Masri

摘要:

提出了一种新的流体体积模型(VoF),即显式体积扩散(EVD)模型,用于模拟包括湍流和初级喷雾雾化在内的界面流动。EVD模型是通过在物理定义的长度尺度上对VoF方程进行体积平均而得出的。这引入了未闭合的子体积通量、子体积应力和体积平均表面张力力。由于湍流运动和其他界面动力学,通常可以发生在层流和湍流中,从而产生子体积波动。这两种类型的波动都被体积平均过程衰减。子体积通量由梯度扩散模型封闭,并且涉及与物理长度尺度相关的显式体积扩散系数。子体积应力封闭引入了一个明确的体积粘度增加的湍流粘度在湍流。体积平均表面张力力闭合是基于褶皱子体积界面的分形性质。这些封闭通过一系列的二维层流和三维湍流界面剪切流的解析流模拟的先验分析进行评估。随后,充分EVD模拟验证这些剪切流和实验室气流喷射。数值收敛表明,保持物理长度尺度不变,同时减少数值网格的大小,使数值扩散减少,并成为压倒显式体积扩散。还进行了灵敏度分析的物理长度尺度的变化,这是比较的边界层厚度的轻流体侧的接口。

英文摘要:

A novel volume of fluid model (VoF) called explicit volume diffusion (EVD) is developed for the simulation of interfacial flows, including those with turbulence and primary spray atomisation. The EVD model is derived by volume averaging the VoF equations over a physically-defined length scale. This introduces unclosed sub-volume flux, sub-volume stress and volume averaged surface tension force. Sub-volume fluctuations arise due to both turbulent motions and other interface dynamics which can, in general, occur in both laminar and turbulent flows. Both of these types of fluctuations are attenuated by the volume averaging process. The sub-volume flux is closed by a gradient diffusion model and involves an explicit volume diffusion coefficient that is linked to the physical length scale. The sub-volume stress closure introduces an explicit volume viscosity augmented by turbulent viscosity in turbulent flows. The volume averaged surface tension force closure is based on fractal properties of wrinkled sub-volume interfaces. These closures are evaluated through a priori analysis of resolved flow simulations for a series of two-dimensional laminar and three-dimensional turbulent interfacial shear flows. Subsequently, full EVD simulations are validated for these shear flows and for a laboratory airblast spray jet. Numerical convergence is demonstrated by keeping the physical length scale constant while reducing the numerical grid size so that numerical diffusion diminishes and becomes overwhelmed by the explicit volume diffusion. A sensitivity analysis is also conducted for variations in the physical length scale, which is compared to the boundary layer thickness on the light fluid side of the interface.

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