改变液相表面张力时垂直向上环形流动界面波的实验研究

Y. Rivera, J. Muñoz-Cobo, C. Berna, José-Luis Cuadros, Alberto Escrivá
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引用次数: 1

摘要

在许多工业应用中出现的一种流型是环形两相流。其主要特点是液体质量的主要部分位于管壁上形成环空,而气相则拖着小液滴流过环空核心。这些液滴主要是由流经气芯的气相与在液/气界面产生的扰动波峰的相互作用产生的。本文描述了在垂直环空膜流动装置上进行的一组实验,在液体和气体向上流动的环空流动状态下,在不同的流动条件下,通过向水中添加少量的1-丁醇来改变液体表面张力。1-丁醇的主要特性是,少量的这种物质显著地改变了表面张力,而粘度几乎保持不变。实验在一个内径44 mm、高4.5 m的垂直管内进行,用已知孔隙率系数的多孔材料制造环空流。气体体积流量的实验条件范围为2000 ~ 3500l /min,大气条件下液体体积流量的实验条件范围为4 ~ 10l /min。在中等表面张力下,1-丁醇的水表面张力从72 - 10 Nm变化到45 - 10 Nm。为了测量扰动波的高度和液膜的厚度,我们使用了电导探头——接收传感器收集到的电信号取决于液膜层的厚度。得到了扰动波幅值与膜基厚度及其他物理量的相关性,确定系数和均方根误差值都很好。
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EXPERIMENTAL STUDY OF THE INTERFACIAL WAVES PRODUCED IN UPWARD VERTICAL ANNULAR FLOWS WHEN VARYING THE LIQUID-PHASE SURFACE TENSION
A flow pattern, which appears in many industrial applications, is annular two-phase flow. Its main characteristic is that the main portion of the liquid mass is located at the walls of the tube forming an annulus, while the gas phase flows through the annulus core dragging small liquid drops. These drops are largely produced by the interactions of the gas-phase flowing through the gas core with the peaks of the disturbance waves, which are produced in the liquid/gas interface. This paper describes a set of experiments performed at the Vertical Annular Film Flow facility, in the annular flow regime, with upward liquid and gas flows, at different flow conditions varying the liquid surface tension by adding small amounts of 1-butanol to the water. The main property of 1-butanol is that small amounts of this substance significantly change the surface tension while the viscosity remains practically unchanged. The set of experiments were carried out inside a vertical tube 44 mm inner diameter, and 4.5 m high, the annular flow was created by means of a porous material with known porosity coefficient. The experimental conditions range from 2000 to 3500 l/min for the gas volumetric flow rate, and from 4 to 10 l/min for the liquid volumetric flow rate at atmospheric conditions. Several experiments have been carried out on 1-butanol varying the water surface tension from 72 10 Nm , to 45 10 Nm , at intermediate surface tensions. To measure the height of the disturbance waves and the thickness of the film we use a conductance probe – the electrical signal collected in the receiver sensor depends on the thickness of the liquid film layer. Correlations for the amplitude of the disturbance waves, the film base thickness and other physical magnitudes have been obtained with a good value for the coefficient of determination and the root mean square error.
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