垂直上升气液两相弹状流模型

基于等效弹单元思想,改进了预测垂直上升管中充分发展气液弹状流流动特性的模型。 模型中考虑了界面切应力对液膜运动的影响;并在液弹空隙度预测中引入临界气体夹带速度的概念,以此来描述弹状流中大气泡尾部的混合特性。本文提出的模型还考虑了管径对液弹空隙度的影响。弹状流模型的计算结果得到本文及其他作者实验数据的验证。     

垂直管内向上气液流动的分析(Ⅰ)——弹状气泡与下落液膜流动

弹状流是垂直管内气液两相上升流中的一种重要流型。本文从相对坐标系的质量与动量衡算出发,对弹状气泡与下落液膜流动进行分析,建立了相应的计算公式。本文也是完整的弹状流数学模型的一部分。     

垂直管内气液两相弹状流含气率研究

In order to investigate the influence of the entrance effect on the spatial distribution of phases, the experiments on gas-liquid two-phase slug flow in a vertical pipe of 0.03m ID were carried out by using optical probes and an EKTAPRO 1000 high speed motion analyzer. It demonstrates that the radial profile of slug flow void fraction is parabolic. Influenced by the falling liquid film, the radial profile curve of liquid slug void fraction in the wake region is also parabolic. Since fully turbulent velocity distribution is built up in the developed region,the void fraction profile in this region is the saddle type. At given superficial liquid velocity, the liquid slug void fraction increases with gas velocity. The radial profiles of liquid slug void fraction at different axial locations are all saddle curves, but void fraction is obviously high around the centerline in the entrance region. The nearer the measuring station is from the entrance, the farther the peak location is away from the wall.     

垂直上升气液弹状流中含气率分布的实验研究

彩和光导纤维探针和美国柯达公司生产的ＥＫＴＡＰＲＯ１０００型高速动态分析仪研究了生趣直上升管内气液两相弹状流中含气率分布,获得了有关弹状流入口区及充分发展区相分布的实验数据。     

垂直管内向上气液流动的分析(Ⅱ)——弹状流的压力降计算

本文采用以弹状气泡速度运动的相对坐标系,对液体段建立动量衡算关系,分析了弹状流压力降中加速压降的来源。与前人结果比较,理论根据较为充分,与实验数据也更为吻合。     

垂直管内气液两相弹状流压力降

把空隙率和气相密度沿管子高度的变化当作连续过程，并以微分单元压力降出发，然后在全管范围内积分，从而导出了气液两相在弹状流情况下的总压力降计算式：△Ｐ＝　ｌｎ（１＋　）＋Ｚｃ该计算式用于计算弹状流压力降时，简便且准确度高。     

垂直管内气液两相流的探讨—气泡流压力降

本文把空隙率和气盯密度沿管子高度的变化当作连续过程，并从微分总压力降出发，然后在全管范围内积分，从而导出气液两相在气泡流情况下的总压力降模型的Ｐ１－Ｐ２＝ｄ－ｂｃ／ａｃｌｎｄ＋ａｃＰ１／ｄ＋ａｃＰ２＋Ｚｃ该模型用于求垂直管内向上流动的气泡流压力降时初值要求不高，收敛快，且准确度高。     

垂直上升弹状流中液弹长度分布

提出了计算垂直上升弹状流中尾随Taylor气泡上升速度的关系式;并基于气泡追赶合并机理,建立了预测沿管路任意位置液弹长度分布模型,提供了弹状流发展过程中弹长分布的变化情况。     

水平管气液两相弹状流液弹频率的水动力学新模型

The prediction of slug frequency has important significance on gas-liquid two-phase flow. A hydrodynamic model was put forward to evaluate slug frequency for horizontal two-phase flow, based on the dependence of slug frequency on the frequency of unstable interfacial wave. Using air and water, experimental verification of the model was carried out in a large range of flow parameters. Six electrical probes were installed at different positions of a horizontal plexiglass pipe to detect slug frequency development. The pipe is 30 m long and its inner diameter is 24 ram. It is observed experimentally that the interracial wave frequency at the inlet is about i to 3 times the frequency of stable slug. The slug frequencies predicted by the model fit well with Tronconi (1990) model and the experimental data. The combination of the hydrodynamic model and the experimental data results in a conclusion that the frequency of equilibrium liquid slug is approximately half the minimum frequency of interfacial wave.     

地形起伏管路气液两相段塞流模型研究

段塞流是气液两相流动中的一种常见流型,由于地形原因,管路多处于起伏状态,而目前国内外对起伏诱发的气液两相管路段塞流研究尚不成熟。针对实际气液两相管路中频繁出现的地形起伏段塞流,首先利用历史数据对现有段塞流模型的适用性进行了比较,建立了地形起伏状态下段塞流的液塞追踪修正模型,最后利用FLUENT软件进行了模拟,研究了管路起伏诱发状况对段塞流段塞分布、拐角处持液率、液塞长度和压降的影响,并将模拟压降与计算压降进行对比,结果表明建立的模型具有一定的精度,对于实际的地形起伏诱发段塞流管道的安全高效运行有一定的指导意义。     

Slug flow in curved microreactors: Hydrodynamic study

The need for eco-friendly and energy saving processes which are substantially compact and give higher efficiency has led to the concept of process intensification (PI). Curved microchannel is such innovative device, which has potential for the intensification of processes currently carried out in conventional straight or T-type microchannels. Curved microchannels utilize the benefits of centrifugal force to its advantage. The present study deals with the numerical simulation of the Taylor flow in curved microchannels, particularly on gas and liquid slugs with varying curvature ratios (i.e., coil to tube diameter=5, 10, 20 and 30). The three-dimensional, unsteady slug flow development in the curved microchannel was carried out using control volume finite difference method (CVFDM). The gas and liquid slug lengths at various operating and fluid conditions were obtained. The slug flow development for different inlet conditions and geometries (premixed feed, T-type and Y-type inlets) was also studied in the curved microchannels. It was found that for low curvature ratio (D/d=3), the phenomenon of flow reversal and slug freezing takes place due to centrifugal and buoyancy forces. For the similar process conditions, with an increase in curvature ratio to 5 and 10, the phenomenon of flow reversal and slug freezing observed was very minor. The non-uniformity in the slug formation was observed for low curvature ratio as compared to the higher curvature ratios. Further the influence of surface tension, viscosity and wall adhesion was studied on slug flow development in the curved microchannels. From the results it was observed that the surface tension, viscosity and wall adhesion have significant influence on slug flow development in curved microchannels.     

Modeling of Slug Velocity and Pressure Drop in Gas‐Liquid‐Liquid Slug Flow

Gas‐liquid‐liquid slug flow in a capillary reactor is a promising new concept that allows one to incorporate gas‐liquid reaction, liquid‐liquid extraction, and facile catalyst separation in a single unit. In order to assess the performance of a gas‐liquid‐liquid slug flow reactor, it is necessary to predict the slug velocity and pressure drop to ascertain residence times and reaction rates. New empirical models for velocity and pressure drop were developed based on existing models for two‐phase gas‐liquid and liquid‐liquid slug flows, and these were validated experimentally.     

低渗透油田油气混输管路中段塞流特征参数的计算

根据已有的油气混输管路中段塞流特征参数的计算理论,找出适合低渗透油田实际生产特征的计算模型,对低渗透油田控制实际生产中混输管路的段塞流提供参考.     

Coaxial Flow Contactors as Alternative to Double T-Contactors for Triphasic Slug Flow Generation

Triphasic gas-liquid-liquid slug flow systems have great application potential in flow chemistry and are normally generated with a double T-junction where the continuous phase and one disperse phase form a two-phase flow and the second disperse phase is added at the second junction. This design is limited to high disperse phase ratios when a regular and uniform flow is desired. The use of coaxial contactors allows overcoming most of these restrictions. The slug generation, stability, and regularity of the generated triphasic flow were experimentally characterized.     

A Hydrodynamic Modei for Slug Frequency in Horizontal Gas-Liquid Two-Phase Flow

The prediction of slug frequency has important significance on gas-liquid two-phase flow. A hydrody-namic modei was put forward to evaluate slug frequency for horizontal two-phase flow, based on the dependence of slug frequency on the frequency of unstable interfacial wave. Using air and water, experimental verification of the modei was carried out in a large range of flow parameters. Six electrical probes were installed at different positions of a horizontal plexiglass pipe to detect slug frequency development. The pipe is 30m long and its inner diameter is 24 mm. It is observed experimentally that the interfacial wave frequency at the inlet is about l to 3 times the frequency of stable slug. The slug frequencies predicted by the modei fit well with Tronconi (1990) modei and the experimental data. The combination of the hydrodynamic modei and the experimental data results in a conclusion that the frequency of equilibrium liquid slug is approximately half the miniraum frequency of interfacial wave.     

水平管道段塞流特征参数试验研究

通过对差压波动信号的详细分析 ,明确了液塞头和液塞尾到达和离开传感器测压点的时刻与差压信号特征点之间的物理关系 ,提出了采用差压波动信号分析技术获得液塞速度、液塞长度和液塞频率的计算公式。采用该方法 ,在室内长 2 4m、内径 0 .0 5 4m试验架上以空气 水、空气 柴油和空气 6 8# 机械油为介质进行了实际测试 ,经过和文献中数据以及经验公式对比 ,验证了该测试方法的正确性     

垂直同心环空管内上升弹状流向团状流的转换

对垂直同心环形管内上升气液弹状流向团状流的转换进行了一定的研究。根据弹状流及团状流的流动特性 ,并考虑同心环形管的结构特征 ,建立了垂直同心环形管上升气液团状流向环状流转换的新的理论模型。通过文中的实验数据及其他研究者的实验数据对该模型的预测性能进行了检验 ,并与其他研究者的模型进行了比较 ,最后还对环形管结构参数对转换的影响进行了一定的分析。     

水平管段塞流持液率的波动特性

气液两相段塞流是液塞和长气泡在空间和时间上的交替,在流动过程中表现出间歇性和不稳定性.今对水平管中段塞流持液率的波动特性进行了分析.结果表明:在同一折算液速下,随着折算气速的增加,段塞单元的平均持液率和液膜持液率先快速下降再缓慢下降,而液塞持液率先缓慢下降再快速下降.段塞流持液率的概率密度分布为双峰分布,高持液率峰对应于液塞区,低持液率峰对应于液膜区;概率密度函数中较完好的峰所对应的持液率与光滑分层液膜区和液塞区的平均持液率相一致.