Сapillatry在抽干蒸发成气体横流的液体膜的过程中表现出的效应

Y. Kostiuchenko, Vitalii Butar, S. Romanko, V. Lukashov
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引用次数: 0

摘要

本文的目的是确定热毛细效应和浓度毛细效应(马兰戈尼效应)对蒸发成气体横流的液膜宽度变化的规律。这项研究是通过实验进行的,使用一个加热(工作)表面的装置,在其上流动液体膜(水或含水甘油溶液)。一股气流被送入工作面和距离它一定距离的围墙之间的空间,高度均匀,垂直于薄膜运动。沿工作面的高度测量了膜宽,并以不同流动过程参数的依赖关系图表示。在所有的实验中,图形都有一个初始截面,薄膜宽度急剧减小,在这一截面以下,薄膜宽度的变化是平稳的。膜宽随流动过程参数的减小程度可达80%。在层流模式下,膜宽度的减小比湍流模式下更均匀,当曲线在初始截面之外出现一些上升时,可以用液体的强烈混合来解释。随着初始液体流量的增大,膜宽的减小程度减小。在水流过程中,工作表面的温度对膜宽的变化有显著影响,随着温度的升高,膜宽减小。当该温度高于100℃时,可以观察到曲线的上升,这可能与向体积蒸发的转变有关。当甘油溶液流动时,工作表面温度对膜宽变化的影响较小,但其沿工作表面高度的减小幅度大于水。初始液体温度、初始溶液浓度、速度和空气温度等工艺参数对膜宽变化的影响相对较小。为了校正经工艺计算确定的薄膜蒸发面面积,引入毛细效应下的平均蒸发面宽度。其值随着初始液体流量的增大而增大。对于水,这种依赖的特征是在从层流到湍流模式的过渡中膜宽度呈跳变减小。对甘油溶液的依赖性没有这种影响,这可以用它的高粘度来解释。随着工作表面温度的升高,膜的平均蒸发面宽度减小,随着空气速度的增大,膜的平均蒸发面宽度也减小。得到了校正系数估计的经验方程。在这种情况下,毛细效应表现为在其径流高度时膜的宽度减小,这导致需要修正由技术计算确定的膜蒸发面面积。
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Сapillatry effects manifested in the process of draining a liquid film that evaporated into a gas cross flow
The aim of the work is to determine the regularities of changes in the width of the flowing liquid film evaporating into a gas cross flow resulting from thermocapillary and concentration-capillary effects (Marangoni effect). The research was carried out experimentally employing an installation with a heated (working) surface, on which a liquid film (water or aqueous glycerol solution) was flowing. A flow of air was fed into the space between the working surface and the enclosing wall located at a distance from it, evenly in height and perpendicularly to the film movement. The film width was measured along the height of the working surface and the obtained dependencies were presented as graphs for different parameters of the flowing process. In all experiments, the graphs have an initial section with a sharp decrease in the film width, below which its change occurs smoothly. The degree of reduction in the film width depending on the parameters of the flowing process can reach 80%. In laminar mode, the reduction of the film width is more uniform than in turbulent mode, when some rise of the curves beyond the initial section is observed and can be explained by intensive mixing of the liquid. As the initial liquid flow increases, the degree of reduction in the film width decreases. Significant influence on the change in the film width is exerted by the temperature of the working surface during the flow of water: with increasing temperature, the film width decreases. At values of this temperature greater than 100℃, the rise of the curves is observed, possibly associated with the transition to volumetric evaporation. When the glycerol solution is flowing, the temperature of the working surface less influences the change in film width, although its decrease along the height of the working surface is greater than for water. The process parameters such as initial liquid temperature, initial solution concentration, and velocity and air temperature have relatively little effect on the change in film width. To correct the area of the film evaporation surface, determined by technological calculation, the width of the average evaporation surface is introduced under capillary effects. Its value increases with the initial liquid flow. For water, this dependence is characterized by a jump-like decrease in the film width in the transition from laminar to turbulent flow mode. This effect is absent on the dependence for glycerol solution, which can be explained by its higher viscosity. As the temperature of the working surface increases, the width of the average evaporation surface of the film decreases, some decrease being also observed with an increase in air velocity. Empirical equations for estimation of the correction factor were obtained. Capillary effects in this case are expressed by decrease in the width of the film at the height of its runoff, which leads to the need to correct the area of the film evaporation surface determined by technological calculation.
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