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International Journal of Multiphase Flow最新文献

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Subgrid scale modeling of droplet bag breakup in VOF simulations VOF 模拟中液滴袋破裂的子网格尺度建模
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-14 DOI: 10.1016/j.ijmultiphaseflow.2024.104958
Austin Han, Olivier Desjardins

The mesh-dependency of the breakup of liquid films, including their breakup length scales and resulting drop size distributions, has long been an obstacle inhibiting the computational modeling of large-scale spray systems. With the aim of overcoming this barrier, this work presents a framework for the prediction and modeling of subgrid-thickness liquid film formation and breakup within two-phase simulations using the volume of fluid method. A two-plane interface reconstruction is used to capture the development of liquid films as their thickness decreases below the mesh size. The breakup of the film is predicted with a semi-analytical model that incorporates the film geometry captured through the two-plane reconstruction. The framework is validated against experiments of the bag breakup of a liquid drop at We=13.8 through the comparison of the resulting drop size and velocity distributions. The generated distributions show good agreement with experimental results for drop resolutions as low as 25.6 cells across the initial diameter. The presented framework enables these drop breakup simulations to be performed at a computational cost three orders of magnitude lower than the cost of simulations utilizing adaptive mesh refinement.

长期以来,液膜破裂(包括破裂长度尺度和由此产生的液滴大小分布)与网格的关系一直是阻碍大规模喷雾系统计算建模的障碍。为了克服这一障碍,本研究提出了一个框架,利用流体体积法在两相模拟中对亚网格厚度液膜的形成和破裂进行预测和建模。双平面界面重构用于捕捉液膜在厚度减小到网格尺寸以下时的发展过程。利用半解析模型预测薄膜的破裂,该模型结合了通过双平面重构捕捉到的薄膜几何形状。通过比较产生的液滴大小和速度分布,在 We=13.8 条件下对液滴的破袋实验验证了该框架。生成的分布与实验结果非常吻合,液滴分辨率低至初始直径的 25.6 个单元。所提出的框架使液滴破裂模拟的计算成本比利用自适应网格细化的模拟成本低三个数量级。
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引用次数: 0
Thermodynamically consistent phase field model for liquid-gas phase transition with soluble surfactant 具有可溶性表面活性剂的液气相变热力学一致相场模型
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-14 DOI: 10.1016/j.ijmultiphaseflow.2024.104957
Xiao-Yu Zhang , Xin-Yue Duan , Chuan-Yong Zhu , Ming-Hai Xu , Shuyu Sun , Liang Gong , John C. Chai

Despite the enormous potential in facilitating natural development and migration of interfaces during multiphase simulation, the phase-field method remains restricted to low-density ratios, owing to inherent thermodynamic inconsistency, especially for multiphase flow systems with surfactants. The present paper first constructs a liquid-vapor phase transition phase-field model with soluble surfactants using the second law of thermodynamics as the original model. Then, a simplified liquid-vapor phase transition model with soluble surfactants that satisfies thermodynamic consistency is proposed to simulate pool boiling at higher-density ratio. A novel numerical algorithm for the simplified model that satisfies semi-discrete thermodynamic consistency is also developed. Compared with the original model, the thermodynamically consistent characteristics of the simplified numerical model proposed in this paper can significantly reduce the spurious velocity on the interface of a static droplet and thus enable the numerical model to simulate liquid-vapor transition at higher liquid/vapor density ratios. Vapor-liquid coexistence, Laplace's law, and multiple bubble coalescence are used to validate the accuracies and effectiveness of the mathematical model and numerical algorithm. The liquid/vapor density ratio can reach 6776:1 under saturation temperature 0.3Tc (Tc is the critical temperature). The approach is then used to model pool boiling at a low saturation temperature (0.5Tc) with and without soluble surfactants, significantly lower than reported in comparable literature. The results demonstrate that surfactants significantly influence the dynamics of bubbles, and a critical concentration can be identified. In addition, soluble surfactants can also suppress coalescence between adjacent bubbles and prevent the formation of larger bubbles during pool boiling.

尽管相场方法在促进多相模拟过程中界面的自然发展和迁移方面具有巨大潜力,但由于其固有的热力学不一致性,相场方法仍然局限于低密度比,尤其是对于含有表面活性剂的多相流系统。本文首先以热力学第二定律为原始模型,构建了可溶性表面活性剂的液气相变相场模型。然后,提出了满足热力学一致性的可溶性表面活性剂的简化液气相变模型,以模拟高密度比下的池沸腾。此外,还为满足半离散热力学一致性的简化模型开发了一种新的数值算法。与原始模型相比,本文提出的简化数值模型的热力学一致性特征可显著降低静态液滴界面上的虚假速度,从而使数值模型能够模拟较高液体/蒸汽密度比下的液体-蒸汽转变。气液共存、拉普拉斯定律和多气泡凝聚被用来验证数学模型和数值算法的准确性和有效性。在饱和温度 0.3Tc(Tc 为临界温度)下,液体/蒸汽密度比可达 6776:1。然后,使用该方法模拟了有无可溶性表面活性剂在较低饱和温度(0.5Tc)下的池沸腾,其温度明显低于同类文献报道的温度。结果表明,表面活性剂对气泡的动力学有显著影响,并且可以确定临界浓度。此外,可溶性表面活性剂还能抑制相邻气泡之间的凝聚,防止在池沸腾过程中形成更大的气泡。
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引用次数: 0
On charging and breakup of paints using a high-speed rotary bell atomizer with internal charging system 使用带内部装料系统的高速旋转钟罩式雾化器装料和分解涂料
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-10 DOI: 10.1016/j.ijmultiphaseflow.2024.104955
Q. Ye , B. Shen , O. Tiedje , P. Knee , J. Domnick

Experimental and numerical studies on charge transport and liquid atomization with the consideration of electrohydrodynamics (EHD) have been performed for a high-speed rotary bell atomizer with internal charging system. The VOF-to-DPM hybrid model in the commercial CFD code ANSYS Fluent is used to investigate and analyse the liquid breakup. Furthermore, the charge conservation equation is solved not only considering flow convection but also the significant ion drift convection due to the presence of the strong electric field. We introduce the so-called apparent ion mobility coefficient that depends on the permittivity and conductivity of liquid, the film thickness on the bell surface and the electric field strength. With this model we can calculate the charge migration from the electrode, in this case the bell surface, to the liquid film and the droplets. Simulation results show an inhomogeneous charge distribution perpendicular to the bell surface, namely charge accumulating mainly on the film surface. Breakup simulations are carried out using a Newtonian liquid and a real paint. The electric body forces have been included in the Navier-Stokes equations. Effects of EHD on the liquid breakup are analysed. The relationship of droplet charge to droplet diameter is obtained, from which the total current is predicted that compared well with experiments. Simulation results deliver useful information for an improved understanding of the relevant physical processes.

在考虑电流体力学(EHD)的情况下,对带有内部装料系统的高速旋转钟罩式雾化器的电荷传输和液体雾化进行了实验和数值研究。商用 CFD 代码 ANSYS Fluent 中的 VOF 到 DPM 混合模型用于研究和分析液体破裂。此外,电荷守恒方程的求解不仅考虑了流动对流,还考虑了由于强电场的存在而产生的显著离子漂移对流。我们引入了所谓的表观离子迁移系数,它取决于液体的导电率和电导率、钟面上的薄膜厚度以及电场强度。利用这一模型,我们可以计算电荷从电极(此处为喇叭口表面)向液膜和液滴的迁移。模拟结果显示,垂直于喇叭口表面的电荷分布不均匀,即电荷主要积聚在薄膜表面。破裂模拟使用牛顿液体和真实涂料进行。纳维-斯托克斯方程中包含了电体力。分析了 EHD 对液体破裂的影响。得出了液滴电荷与液滴直径的关系,并由此预测了总电流,结果与实验结果对比良好。模拟结果为更好地理解相关物理过程提供了有用信息。
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引用次数: 0
Numerical and experimental investigation of the axis-switching behavior of a rectangular jet 矩形射流轴切换行为的数值和实验研究
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-08 DOI: 10.1016/j.ijmultiphaseflow.2024.104951
C. García Llamas , V.V. Swami , V.P. Petrova , K.A. Buist , J.A.M. Kuipers , M.W. Baltussen

Rectangular jets exhibit axis-switching behavior which results in enhanced flow entrainment compared to round jets. This feature allows for their potential industrial use as passive flow controllers in mixing applications. However, rectangular jets have received limited attention compared to round jets. To operate rectangular jets optimally, a better understanding on the underlying phenomena influencing the axis-switching of the jet is required. In this paper, Direct Numerical Simulations of rectangular jets are performed at different injection velocities using the Local Front Reconstruction Method (LFRM) to track the liquid–gas interface. The simulations are validated using experiments in a similar range of Weber and Reynolds numbers. The obtained results showed that LFRM can accurately capture the jet oscillations, break-up lengths and droplet sizes observed experimentally. Additionally, a fully developed velocity profile at the nozzle outlet enhances the jet stability resulting in larger break-up length values compared to a uniform velocity profile.

与圆形喷射器相比,矩形喷射器表现出轴切换行为,从而增强了流动夹带。这一特性使其有可能在混合应用中用作被动流量控制器。然而,与圆形喷射器相比,矩形喷射器受到的关注有限。要优化矩形射流的运行,需要更好地了解影响射流轴向切换的基本现象。本文采用局部前沿重构法(LFRM)跟踪液气界面,在不同喷射速度下对矩形喷流进行了直接数值模拟。在类似的韦伯和雷诺数范围内,使用实验对模拟进行了验证。结果表明,局部前沿重构法能够准确捕捉实验中观察到的射流振荡、破裂长度和液滴大小。此外,与均匀的速度曲线相比,喷嘴出口处充分发展的速度曲线会增强射流的稳定性,从而产生更大的破裂长度值。
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引用次数: 0
Development of a new computational solver for multiphase flows in heterogeneous porous media at different scales 为不同尺度异质多孔介质中的多相流开发新的计算求解器
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-06 DOI: 10.1016/j.ijmultiphaseflow.2024.104954
Roberto Lange , Gabriel M. Magalhães , Franciane F. Rocha , Pedro V.S. Coimbra , Jovani L. Favero , Rodrigo A.C. Dias , Antonio O.S. Moraes , Mateus P. Schwalbert

This work presents the development of a novel solver tailored for simulating multiphase flows within heterogeneous porous media. Leveraging the Eulerian multi-fluid model coupled with Darcy’s law, the solver demonstrates adaptability across diverse scales, effectively handling heterogeneous porosity and permeability fields. The proposed solver, called upstreamFoam, extends the capabilities of OpenFOAM framework, specifically the multiphaseEulerFoam, by incorporating models for porous media simulations. This integration introduces new features and formulations, allowing for the simulation of compressible multiphase flows in porous media with intricate properties. The approach presented here provides a robust framework for characterizing reservoirs and treating heterogeneous porous systems at different scales. A successful validation of the introduced solver for classical problems with analytical, semi-analytical, and reference solutions is presented. Then, applications on a wide range of multiphase flows in heterogeneous porous media at different scales have been studied, demonstrating the potential of the solver to simulate complex multiphase problems.

本研究介绍了一种专为模拟异质多孔介质中的多相流而开发的新型求解器。利用欧拉多流体模型和达西定律,该求解器展示了不同尺度的适应性,可有效处理异质孔隙度和渗透性场。所提出的求解器名为 upstreamFoam,它扩展了 OpenFOAM 框架的功能,特别是多相 EulerFoam,纳入了多孔介质模拟模型。这种集成引入了新的功能和公式,允许模拟具有复杂性质的多孔介质中的可压缩多相流。本文介绍的方法为描述储层特征和处理不同尺度的异质多孔系统提供了一个强大的框架。本文介绍了引入的求解器对经典问题的分析、半分析和参考解的成功验证。然后,研究了在不同尺度异质多孔介质中多相流的广泛应用,展示了求解器模拟复杂多相问题的潜力。
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引用次数: 0
Enhancing experimental image quality in two-phase bubbly systems with super-resolution using generative adversarial networks 利用生成式对抗网络的超分辨率提高两相气泡系统的实验图像质量
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-05 DOI: 10.1016/j.ijmultiphaseflow.2024.104952
M.C. Neves , J. Filgueiras , Z. Kokkinogenis , M.C.F. Silva , J.B.L.M. Campos , L.P. Reis

Fluid Dynamics is a key scientific field to multitudes of engineering applications. Experimental work in this field requires careful set-up and expensive image-capturing equipment, particularly when considering the finer details of complex phenomena. In this work, we study the application of super-resolution Generative Adversarial Networks (GANs) to achieve high-resolution results by upscaling lower-resolution experimental images.

We train GANs proposed for natural images on a bubbly flow experimental Fluid Dynamics dataset and compare common super-resolution evaluation metrics to domain expert assessments of the upscaled images. We find that these models achieve promising results, as evaluated by experts, and transfer learning from natural images translates to better performance overall. Attention mechanisms are found to be particularly useful in recreating sharper details. On the other hand, traditional super-resolution evaluation metrics are found to align poorly with expert perception of quality, signaling the need for better systematic evaluation methodologies in this domain.

流体动力学是众多工程应用的关键科学领域。该领域的实验工作需要精心的设置和昂贵的图像捕捉设备,尤其是在考虑复杂现象的细节时。在这项工作中,我们研究了超分辨率生成对抗网络(GANs)的应用,通过提升低分辨率实验图像的分辨率来获得高分辨率结果。
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引用次数: 0
Theoretical study on sequential splitting of droplets flowing through fractal tree-shaped microchannel networks 关于流经分形树状微通道网络的液滴顺序分裂的理论研究
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-05 DOI: 10.1016/j.ijmultiphaseflow.2024.104953
Zilong Deng, Suchen Wu, Yongping Chen

A theoretical model for describing the sequential splitting of droplets flowing through the fractal tree-shaped microchannel network with arbitrary branch level is developed to explore the mechanisms underlying the hydraulic imbalance on the high-throughput droplets production. Accordingly, detailed droplet splitting characteristics are presented, including the droplet velocities in branches, droplet distribution coefficient, and monodispersity of droplets production. It is found that the uniformity of droplet mainly depends on two key dimensionless parameters, namely Λ1 and Λ2, where Λ1 is determined by the initial working condition involving the initial lengths and viscosity of the continuous and discrete phases, the width of the 0th level channel, and the initial capillary number, and Λ2 is concerned with the outlet pressure pout, [2n-1] and the pressure drops of the continuous and discrete phases at the 0th level channel. The monodispersity of droplets goes down with the decreasing Λ1 and the increasing Λ2. Based on the Λ1 and Λ2, the optimal design strategies contributing to enhancing the droplet generation uniformity are recommended, including increasing Ca, enlarging the length of continuous phase flow at the main channel, and increasing the lengths of each level channels. Furthermore, the tree-shaped microchannel networks with higher branch level (n) have stronger ability to resist asymmetric disturbances. In particular, in our work, the width fractal dimension Δ = 2 is adopted as a proper key structure parameter, so as to ensure sequential breakup of droplet at each T-junction under symmetric condition.

本文建立了一个理论模型,用于描述流经具有任意分支层级的分形树状微通道网络的液滴的顺序分裂,以探索水力失衡对高通量液滴产生的影响机制。因此,研究给出了详细的液滴分裂特征,包括分支中的液滴速度、液滴分布系数和液滴产生的单分散性。研究发现,液滴的均匀性主要取决于两个关键的无量纲参数,即Λ1 和Λ2,其中Λ1 由初始工况决定,涉及连续相和离散相的初始长度和粘度、第 0 层通道的宽度以及初始毛细管数;而Λ2 则与出口压力 pout [2n-1] 以及连续相和离散相在第 0 层通道的压降有关。液滴的单分散性随着Λ1 的减小和Λ2 的增大而减小。根据Λ1和Λ2,推荐了有助于提高液滴生成均匀性的最佳设计策略,包括增加 Ca、扩大主通道连续相流长度和增加各级通道长度。此外,分支级别(n)较高的树形微通道网络具有更强的抗非对称干扰能力。在我们的工作中,特别采用了宽度分形维数 Δ = 2 作为适当的关键结构参数,以确保在对称条件下,液滴在每个 T 型交界处依次破碎。
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引用次数: 0
Machine learning and physics-driven modelling and simulation of multiphase systems 多相系统的机器学习和物理驱动建模与仿真
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-08-01 DOI: 10.1016/j.ijmultiphaseflow.2024.104936
Nausheen Basha , Rossella Arcucci , Panagiota Angeli , Charitos Anastasiou , Thomas Abadie , César Quilodrán Casas , Jianhua Chen , Sibo Cheng , Loïc Chagot , Federico Galvanin , Claire E. Heaney , Fria Hossein , Jinwei Hu , Nina Kovalchuk , Maria Kalli , Lyes Kahouadji , Morgan Kerhouant , Alessio Lavino , Fuyue Liang , Konstantia Nathanael , Omar K Matar

We highlight the work of a multi-university collaborative programme, PREMIERE (PREdictive Modelling with QuantIfication of UncERtainty for MultiphasE Systems), which is at the intersection of multi-physics and machine learning, aiming to enhance predictive capabilities in complex multiphase flow systems across diverse length and time scales. Our contributions encompass a variety of approaches, including the Design of Experiments for nanoparticle synthesis optimisation, Generalised Latent Assimilation models for drop coalescence prediction, Bayesian regularised artificial neural networks, eXtreme Gradient Boosting for microdroplet formation prediction, and a sub-sampling based adversarial neural network for predicting slug flow behaviour in two-phase pipe flows. Additionally, we introduce a generalised latent assimilation technique, Long Short-Term Memory networks for sequence forecasting mixing performance in stirred and static mixers, active learning via Bayesian optimisation to recover coalescence model parameters for high current density electrolysers, Gaussian process regression for drop size distribution predictions for sprays, and acoustic emission signal inversion using gradient boosting machines to characterise particle size distribution in fluidised beds. We also offer perspectives on the development of a shape optimisation framework that leverages the use of a multi-fidelity multiphase emulator. The results presented have applications in chemical synthesis, microfluidics, product manufacturing, and green hydrogen generation.

我们重点介绍一项多所大学合作计划 PREMIERE(多相流系统不确定性量化预测建模)的工作,该计划处于多物理场和机器学习的交叉点,旨在提高不同长度和时间尺度的复杂多相流系统的预测能力。我们的研究成果涵盖多种方法,包括用于纳米粒子合成优化的实验设计(Design of Experiments)、用于液滴凝聚预测的广义同化模型(Generalised Latent Assimilation models)、贝叶斯正则化人工神经网络(Bayesian regularised artificial neural networks)、用于微液滴形成预测的梯度提升(eXtreme Gradient Boosting),以及用于预测两相管道流中蛞蝓流动行为的基于子采样的对抗神经网络(adversarial neural network)。此外,我们还介绍了广义潜势同化技术、用于序列预测搅拌式和静态混合器混合性能的长短期记忆网络、通过贝叶斯优化恢复高电流密度电解槽凝聚模型参数的主动学习、用于预测喷雾液滴粒度分布的高斯过程回归,以及使用梯度提升机反演声发射信号以描述流化床中的粒度分布特征。我们还对利用多保真度多相模拟器开发形状优化框架提出了展望。所展示的成果可应用于化学合成、微流体、产品制造和绿色制氢。
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引用次数: 0
Effect of incoming flow conditions on air lubrication regimes 入流条件对空气润滑状态的影响
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-07-31 DOI: 10.1016/j.ijmultiphaseflow.2024.104948
Lina Nikolaidou , Angeliki Laskari , Tom van Terwisga , Christian Poelma

Different air phase regimes are formed by controlled air injection in a spatially developing flat plate turbulent boundary layer (TBL). The air is introduced via a slot type injector without the use of a backward-facing step or cavitator upstream of the air injection position. The effect of different incoming liquid flow characteristics on the different regimes is investigated by varying both the liquid freestream velocity and the incoming TBL thickness. The latter is realized through changing the position of the air injection along the length of the water tunnel facility. That resulted in a downstream distance based Reynolds number from 1 to 5 million. Three different air phase regimes are identified under different air flow rates and freestream velocities: the bubbly regime, the transitional, and the air layer regime. The morphological differences of each one are described and quantitative analysis is performed based on the non-wetted area in each condition. The incoming TBL as well as the flow around the air layer are measured with planar particle image velocimetry. The latter enabled the determination of the air layer thickness. In addition, the ratio of the air layer to the incoming boundary layer thickness tair/δ is also calculated ( 0.04 – 0.5). This is a significant dimensionless parameter for scaling, which indicates the extent to which the air layer is embedded within the incoming TBL. Depending on the incoming flow conditions, a two or three branch air layer is formed. The length of the air layer is found to increase with increasing liquid freestream velocities. A good agreement between the air layer length and a half gravity wave predicted by the dispersion relation is found. An increase of the air layer length is observed with a decreasing incoming TBL thickness. This is attributed to a decrease in the local mean velocity at the air–water interface due to the TBL growth. Finally, increasing the incoming TBL thickness delays the onset of the air layer regime.

在空间发展的平板湍流边界层(TBL)中,通过控制空气注入形成不同的气相机制。空气通过槽式喷射器喷入,在空气喷射位置的上游不使用后向台阶或空化器。通过改变液体自由流速度和进入的 TBL 厚度,研究了不同进入液体流动特性对不同状态的影响。后者是通过沿水洞设施长度方向改变空气注入位置来实现的。这导致基于下游距离的雷诺数从 100 万到 500 万不等。在不同的空气流速和自由流速度下,确定了三种不同的气相状态:气泡状态、过渡状态和气层状态。对每种气相的形态差异进行了描述,并根据每种情况下的非润湿面积进行了定量分析。利用平面粒子图像测速仪测量了进入的 TBL 以及空气层周围的流动情况。后者能够确定空气层的厚度。此外,还计算了空气层与进入的边界层厚度之比 tair/δ(≈ 0.04 - 0.5)。这是一个重要的缩放无量纲参数,表示空气层嵌入流入 TBL 的程度。根据入流条件,会形成两支或三支空气层。空气层的长度随着液体自由流速度的增加而增加。空气层长度与根据弥散关系预测的半重力波之间有很好的一致性。空气层长度随着进入的 TBL 厚度的减小而增加。这是因为 TBL 的增长导致空气-水界面的局部平均速度下降。最后,增加进入的 TBL 厚度会推迟空气层状态的出现。
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引用次数: 0
Benchmark DEBORA: Assessment of MCFD compared to high-pressure boiling pipe flow measurements 基准 DEBORA:与高压沸腾管流量测量相比的 MCFD 评估
IF 3.6 2区 工程技术 Q1 MECHANICS Pub Date : 2024-07-30 DOI: 10.1016/j.ijmultiphaseflow.2024.104920
G. Bois , P. Fillion , F. François , A. Burlot , A. Ben Hadj Ali , A. Khaware , J. Sanyal , M. Rehm , B. Farges , F. Vinauger , W. Ding , A. Gajšek , M. Tekavčič , B. Končar , J.-M. Le Corre , H. Li , R. Härlin , J. Jaseliūnaitė , E. Baglietto , R. Brewster , V. Hovi
<div><p>A benchmark activity on two-fluid simulations of high-pressure boiling upward flows in a pipe is performed by 12 participants using different MCFD (Multiphase Computational Fluid Dynamics) codes and closure relationships. More than 30 conditions from DEBORA experiment conducted by CEA are considered. Each case is characterised by the flow rate, inlet temperature, wall heat flux and outlet pressure. High-pressure Freon (R12) at 14<!--> <!-->bar and 26<!--> <!-->bar is boiled in a <span><math><mrow><mtext>19.2</mtext><mspace></mspace><mtext>mm</mtext></mrow></math></span> pipe heated over <span><math><mrow><mtext>3.5</mtext><mspace></mspace><mtext>m</mtext></mrow></math></span>. Flow rates range from 2000<!--> <!-->kg<!--> <!-->m<sup>−2</sup> <!-->s<sup>−1</sup> to 5000<!--> <!-->kg<!--> <!-->m<sup>−2</sup> <!-->s<sup>−1</sup> and exit quality <span><math><mi>x</mi></math></span> ranges from single-phase conditions to <span><math><mrow><mi>x</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>1</mn></mrow></math></span> which leads to a peak void fraction of <span><math><mrow><mi>α</mi><mo>=</mo><mn>70</mn><mtext>%</mtext></mrow></math></span>. In these high pressure conditions, bubbles remain small and there is no departure from the bubbly flow regime (François et al., 2011; Hösler, 1968). However, different kind of bubbly flows are observed: wall-peak, intermediate peak or core-peak, depending on the case considered. Measurements along the pipe radius near the end of the heated section are compared to code predictions. They include void fraction, bubble mean diameter, vapour velocity and liquid temperature. The benchmark covered two phases. In the first phase of the benchmark activities, experimental data were given to the participants, allowing to compare the simulation results and to develop, to select or to adjust the models in the CMFD codes. The second phase included blind cases where the participants could not compare to the measurements. In between the two phases, possible additional model adjustments or calibrations were performed.</p><p>Overall, the benchmark involved very different closures and a wide range of models’ complexity was covered. Yet, it is extremely difficult to have a robust closure for all conditions considered, even knowing experimental measurements. The wall-to-core peak transition is not captured consistently by the models. The degree of subcooling and the void fraction level are also difficult to assess. We were not capable of showing superiority of some physical closures, even for part of the model. The interaction between mechanisms and their hierarchy are extremely difficult to understand.</p><p>Although departure from nucleate boiling (DNB) was not considered in this benchmarking exercise, it is expected that DNB predictions at high-pressure conditions depend strongly on the near-wall flow, temperature, and void fraction distributions. Therefore, the suitability of the closures also limits the accuracy of DNB prediction
12 位参与者使用不同的 MCFD(多相计算流体力学)代码和闭合关系,对管道中的高压沸腾上升流进行了双流体模拟。其中考虑了由法国原子能委员会(CEA)进行的 DEBORA 试验中的 30 多种情况。每种情况的特点是流速、入口温度、壁面热通量和出口压力。14bar和26bar的高压氟利昂(R12)在一根加热至沸点的管道中沸腾。流速范围从 2000kgms 到 5000kgms,出口质量范围从单相条件到导致峰值空隙率为 . 在这些高压条件下,气泡仍然很小,不会偏离气泡流动状态(François 等人,2011 年;Hösler,1968 年)。然而,根据所考虑的情况,会观察到不同类型的气泡流:壁峰、中间峰或芯峰。沿加热段末端附近的管道半径进行的测量结果与代码预测结果进行了比较。这些数据包括空隙率、气泡平均直径、蒸汽速度和液体温度。基准测试包括两个阶段。在基准活动的第一阶段,向参与者提供实验数据,以便比较模拟结果,并开发、选择或调整 CMFD 代码中的模型。第二阶段包括盲测,参与者无法与测量结果进行比较。在这两个阶段之间,还可能进行额外的模型调整或校准。
{"title":"Benchmark DEBORA: Assessment of MCFD compared to high-pressure boiling pipe flow measurements","authors":"G. Bois ,&nbsp;P. Fillion ,&nbsp;F. François ,&nbsp;A. Burlot ,&nbsp;A. Ben Hadj Ali ,&nbsp;A. Khaware ,&nbsp;J. Sanyal ,&nbsp;M. Rehm ,&nbsp;B. Farges ,&nbsp;F. Vinauger ,&nbsp;W. Ding ,&nbsp;A. Gajšek ,&nbsp;M. Tekavčič ,&nbsp;B. Končar ,&nbsp;J.-M. Le Corre ,&nbsp;H. Li ,&nbsp;R. Härlin ,&nbsp;J. Jaseliūnaitė ,&nbsp;E. Baglietto ,&nbsp;R. Brewster ,&nbsp;V. Hovi","doi":"10.1016/j.ijmultiphaseflow.2024.104920","DOIUrl":"10.1016/j.ijmultiphaseflow.2024.104920","url":null,"abstract":"&lt;div&gt;&lt;p&gt;A benchmark activity on two-fluid simulations of high-pressure boiling upward flows in a pipe is performed by 12 participants using different MCFD (Multiphase Computational Fluid Dynamics) codes and closure relationships. More than 30 conditions from DEBORA experiment conducted by CEA are considered. Each case is characterised by the flow rate, inlet temperature, wall heat flux and outlet pressure. High-pressure Freon (R12) at 14&lt;!--&gt; &lt;!--&gt;bar and 26&lt;!--&gt; &lt;!--&gt;bar is boiled in a &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mtext&gt;19.2&lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;mm&lt;/mtext&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; pipe heated over &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mtext&gt;3.5&lt;/mtext&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mtext&gt;m&lt;/mtext&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. Flow rates range from 2000&lt;!--&gt; &lt;!--&gt;kg&lt;!--&gt; &lt;!--&gt;m&lt;sup&gt;−2&lt;/sup&gt; &lt;!--&gt;s&lt;sup&gt;−1&lt;/sup&gt; to 5000&lt;!--&gt; &lt;!--&gt;kg&lt;!--&gt; &lt;!--&gt;m&lt;sup&gt;−2&lt;/sup&gt; &lt;!--&gt;s&lt;sup&gt;−1&lt;/sup&gt; and exit quality &lt;span&gt;&lt;math&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; ranges from single-phase conditions to &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; which leads to a peak void fraction of &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;α&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;70&lt;/mn&gt;&lt;mtext&gt;%&lt;/mtext&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. In these high pressure conditions, bubbles remain small and there is no departure from the bubbly flow regime (François et al., 2011; Hösler, 1968). However, different kind of bubbly flows are observed: wall-peak, intermediate peak or core-peak, depending on the case considered. Measurements along the pipe radius near the end of the heated section are compared to code predictions. They include void fraction, bubble mean diameter, vapour velocity and liquid temperature. The benchmark covered two phases. In the first phase of the benchmark activities, experimental data were given to the participants, allowing to compare the simulation results and to develop, to select or to adjust the models in the CMFD codes. The second phase included blind cases where the participants could not compare to the measurements. In between the two phases, possible additional model adjustments or calibrations were performed.&lt;/p&gt;&lt;p&gt;Overall, the benchmark involved very different closures and a wide range of models’ complexity was covered. Yet, it is extremely difficult to have a robust closure for all conditions considered, even knowing experimental measurements. The wall-to-core peak transition is not captured consistently by the models. The degree of subcooling and the void fraction level are also difficult to assess. We were not capable of showing superiority of some physical closures, even for part of the model. The interaction between mechanisms and their hierarchy are extremely difficult to understand.&lt;/p&gt;&lt;p&gt;Although departure from nucleate boiling (DNB) was not considered in this benchmarking exercise, it is expected that DNB predictions at high-pressure conditions depend strongly on the near-wall flow, temperature, and void fraction distributions. Therefore, the suitability of the closures also limits the accuracy of DNB prediction","PeriodicalId":339,"journal":{"name":"International Journal of Multiphase Flow","volume":"179 ","pages":"Article 104920"},"PeriodicalIF":3.6,"publicationDate":"2024-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0301932224001976/pdfft?md5=468a165bf322ec7e4fc6794e0f1dadf9&pid=1-s2.0-S0301932224001976-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141933748","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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International Journal of Multiphase Flow
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