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A surface renewal model for unsteady-state mass transfer using the generalized Danckwerts age distribution function

机译:使用广义Danckwerts年龄分布函数的非稳态传质表面更新模型

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摘要

The recently derived steady-state generalized Danckwerts age distribution is extended to unsteady-state conditions. For three different wind speeds used by researchers on air–water heat exchange on the Heidelberg Aeolotron, calculations reveal that the distribution has a sharp peak during the initial moments, but flattens out and acquires a bell-shaped character with process time, with the time taken to attain a steady-state profile being a strong and inverse function of wind speed. With increasing wind speed, the age distribution narrows significantly, its skewness decreases and its peak becomes larger. The mean eddy renewal time increases linearly with process time initially but approaches a final steady-state value asymptotically, which decreases dramatically with increased wind speed. Using the distribution to analyse the transient absorption of a gas into a large body of liquid, assuming negligible gas-side mass-transfer resistance, estimates are made of the gas-absorption and dissolved-gas transfer coefficients for oxygen absorption in water at 25°C for the three different wind speeds. Under unsteady-state conditions, these two coefficients show an inverse behaviour, indicating a heightened accumulation of dissolved gas in the surface elements, especially during the initial moments of absorption. However, the two mass-transfer coefficients start merging together as the steady state is approached. Theoretical predictions of the steady-state mass-transfer coefficient or transfer velocity are in fair agreement (average absolute error of prediction = 18.1%) with some experimental measurements of the same for the nitrous oxide–water system at 20°C that were made in the Heidelberg Aeolotron.
机译:最近导出的稳态广义Danckwerts年龄分布扩展到非稳态条件。对于研究人员在海德堡Aeolotron上的空气-水热交换中使用的三种不同风速,计算表明,该分布在初始时刻具有尖锐的峰值,但随着时间的推移,分布逐渐变平并呈现出钟形特征,随时间变化用来获得稳态曲线是风速的强而反函数。随着风速的增加,年龄分布明显变窄,偏度减小,峰值变大。平均涡流更新时间最初随着处理时间线性增加,但逐渐接近最终稳态值,随着风速的增加,平均稳态值逐渐减小。假设气体侧传质阻力可忽略不计,使用分布分析气体在大块液体中的瞬态吸收,可以估算出在25°C时水中的氧气吸收率和气体吸收率C为三种不同的风速。在非稳态条件下,这两个系数表现出相反的行为,表明表面元素中溶解气体的积累增加,尤其是在吸收的初始时刻。但是,随着接近稳态,两个传质系数开始合并在一起。稳态传质系数或传质速度的理论预测值是一致的(预测值的平均绝对误差= 18.1%),并且在20℃下对一氧化二氮-水系统进行了一些相同的实验测量。海德堡电子风云。

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