Numerical Modeling of Liquid Jet in Non-Uniform Crossflow Using Enhanced Madabhushi Model

H. Feiz, Wei Zhao, D. Kubicki, M. Frackowiak, Vivek Kumar, H. Jadeja, Pravin M. Nakod, S. Shrivastava, Sravankumar Nallamothu, M. Lambert, J. Lee, Jinkwan Song
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Abstract

One of the most used spray configurations for gas turbines and power combustors is liquid jet in crossflow. The process of breakup of liquid jet is very complex and understanding this mechanism is of paramount importance in engine design. This has led to the commencement of several studies from leading research groups [1–6]. Several new modeling methods such as the Madabhushi breakup model or more detailed VOF and Level set methods have been used successfully to understand and describe these complex breakup processes. However, most of these studies have been restricted to liquid jet in uniform single stream crossflow. In reality, these jets could be subjected to several gaseous streams and the breakup mechanism may vary significantly. Recently there have been some studies to understand the effect of non-uniformities on the crossflow velocity distribution and the droplet diameter. In the current work, we attempt to extend the scope of the Madabhushi breakup model to jets subjected to non-uniform crossflow. Non-uniform crossflow is created by co-directional and parallel gas flow using several hollow tubes. Locally, the momentum flux ratio changes by a factor of 4 and uniformity ratio (the ratio of the velocities of the two gas streams) of 2. A modified version of the Madabhushi model as proposed by Lambert et. al is used here to simulate the jet breakup. Model tuning has been conducted using University of Cincinnati Research data specifically designed for this configuration in partnership with General Electric Company. For turbulence, realizable k-ε with scalable wall function is used. The droplets are tracked using Ansys Fluent Discrete Particle Model (DPM). A second modeling approach VOF-to-DPM is also used which uses VOF equation along with LES with Dynamic Kinetic Energy Subgrid-Scale Model. This model requires no fine tuning of parameters and is more accurate but comes with more computational expense. Various simulations are performed with pure water, pure diesel and emulsified diesel and water with uniform and non-uniform cross flows inside a chamber at a pressure of 50psi. Overall, the trends due to difference in material properties of the two liquids especially on penetration and Sauter mean diameter are well captured. The droplet characteristics such as axial velocity, Sauter mean diameter and volumetric flux are compared with experimental measurements and shows reasonable agreement. Overall, the liquid penetration is within reasonable accuracy. Discrepancies were seen in the spatial variation of the spray quantities such as Sauter mean diameter, droplet axial velocity etc. The simulation revealed a more averaged field whereas in experiments some layering was observed with bigger droplets at the edge of the spray, away from the wall.
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非均匀横流中液体射流的增强型Madabhushi模型数值模拟
横流液体射流是燃气轮机和动力燃烧器最常用的喷射形式之一。液体射流的破裂过程非常复杂,了解这一机理在发动机设计中具有至关重要的意义。这导致一些领先的研究小组开始了几项研究[1-6]。一些新的建模方法,如Madabhushi分手模型或更详细的VOF和水平集方法已经成功地用于理解和描述这些复杂的分手过程。然而,这些研究大多局限于均匀的单流交叉流中的液体射流。在现实中,这些喷流可能会受到几种气体流的影响,而破裂机制可能会有很大的不同。近年来,人们对非均匀性对横流速度分布和液滴直径的影响进行了一些研究。在当前的工作中,我们试图将Madabhushi破裂模型的范围扩展到遭受非均匀横流的射流。通过几个空心管的共向平行气体流动产生非均匀横流。局部,动量通量比变化了4倍,均匀度比(两股气流速度之比)变化了2倍。本文采用Lambert等人提出的Madabhushi模型的改进版本来模拟射流的破裂。模型调优是使用辛辛那提大学研究中心与通用电气公司合作专门为该配置设计的数据进行的。对于湍流,采用可实现的带有可伸缩壁函数的k-ε。使用Ansys Fluent离散粒子模型(DPM)跟踪液滴。第二种VOF-to- dpm建模方法是将VOF方程与动态动能亚网格尺度模型结合使用。该模型不需要对参数进行微调,更准确,但计算成本更高。在一个压力为50psi的室内,用纯水、纯柴油、乳化柴油以及均匀和不均匀交叉流动的水进行了各种模拟。总的来说,由于两种液体的材料性质不同,特别是在渗透和索氏平均直径方面的变化趋势得到了很好的捕捉。将液滴的轴向速度、萨特平均直径和体积通量等特性与实验结果进行了比较,结果与实验结果吻合较好。总体而言,液体渗透在合理的精度范围内。喷淋量的空间变化存在差异,如萨德平均直径、液滴轴向速度等。模拟显示了一个更平均的场,而在实验中,在喷雾的边缘,远离壁面,观察到一些分层,更大的液滴。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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