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Liquid flow measurement using phase isolation and an imaging method in horizontal gas-liquid two-phase flow

机译:使用相位隔离和水平气液两相流的成像方法的液体流量测量

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摘要

A new imaging method based on phase isolation for the liquid flow measurement of gas-liquid two-phase flow is proposed in this study. A swirler is arranged upstream to isolate two-phase fluids. As the two-phase mixture passes through it, a strong swirl flow is generated. The gas is concentrated into the center of the tube and forms a gas core while the liquid phase is pushed to the tube wall and forms a uniform liquid film, which is where the swirl core-annular flow occurs. After phase isolation, many microbubbles, which are small enough to neglect their body force, appear in the liquid film. These phase-isolation-induced microbubbles are used as tracers to represent the local velocity of the liquid flow. A CCD camera is employed to track the motion of the bubbles at the focal plane and determines the velocity at this position. Then this measured local velocity is converted to the mean velocity of the liquid film by a velocity coefficient based on the similitude principle of the velocity profile. After the flow area of the liquid film is derived from the void fraction measurement by another CCD camera, the flowrate of liquid film is determined. The velocity coefficients which express the relation between local velocity and mean velocity of liquid film are obtained by a calibration experiment. Two conventional industry CCD cameras and corresponding individual LED illuminations constitute the imaging system. The image-processing algorithm was developed using the MATLAB image toolbox. AAir and tap water are used and their superficial velocity are in the range of 3.41 m s(-1)similar to 45.15 m s(-1)and 0.022 m s(-1)similar to 0.265 m s(-1), respectively. The thickness of liquid film ranges from 72.75 mu m to 423.11 mu m and the diameter of microbubbles ranges from 11 mu m to 35 mu m.
机译:本研究提出了一种基于气液两相流液体流量测量的相位隔离的新成像方法。旋流器布置在上游以隔离两相液体。随着两相混合物通过它,产生强旋流。将气体集中到管的中心,并形成气体芯,同时将液相推向管壁并形成均匀的液体膜,这是旋流芯环流动的均匀液体膜。在相隔离后,许多微泡足够小以忽视其体力,出现在液体膜中。这些相位隔离诱导的微泡用作示踪剂,以表示液体流动的局部速度。使用CCD摄像机来跟踪焦平面在焦平面上的气泡的运动,并确定该位置的速度。然后,该测量的局部速度通过基于速度曲线的类似速度系数转换为液体膜的平均速度。在通过另一种CCD相机通过另一CCD相机衍生自液体膜的流量面积之后,确定液体膜的流量。表达局部速度与液体膜的平均速度之间关系的速度系数是通过校准实验获得的。两个传统的行业CCD相机和相应的单独LED照明构成了成像系统。使用MATLAB图像工具箱开发了图像处理算法。使用轴承和自来水,其表面速度在3.41m S(-1)的范围内,类似于45.15 m S(-1)和0.022 m s(-1),分别类似于0.265 m s(-1)。液体膜的厚度范围为72.75μm至423.11μm,微泡的直径范围为11μm至35μm。

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