不同类型鼓泡塔气液并流时液相轴向扩散系数

在相同尺寸的鼓泡塔、筛板鼓泡塔、振动筛板鼓泡塔中采用脉冲示踪法对空气-水体系进行轴向返混实验研究,考察了水和空气流速对鼓泡塔、鼓泡筛板塔液相轴向扩散系数(EZ)和水、气体流率、筛板振动强度对振动筛板鼓泡塔液相轴向扩散系数的影响.结果表明,鼓泡塔EZ与uL0.696～1.158成正比(uL为液速);筛板鼓泡塔EZ与uL和气速(uG)关系式为EZ=0.798uG0.77uL1.252;振动筛板鼓泡塔的EZ与uL0.8354～1.2740成正比.     

鼓泡塔内气液两相湍流实验研究

介绍了研究鼓泡塔气液两相流的实验装置、实验方法。液相用激光多普勒测速技术(LDV)测量,气相用粒子示踪测速技术(PIV)测量。实验表明,轴向液相速度的径向分布呈塔中心峰值、壁面附近倒流形式,且与气相表观速度大小有关,当液相表观速度一定时,随气相表观速度增大而愈加陡峭,返混也剧烈。当表观液速与表观气速之比小于19．6时,返混区总是存在,且返混区大小与高度有关：当表观液遣与表观气速之比大于19．6时,返混消失,含气率分布由塔中心峰值转向壁面峰值。径向液相速度既与气相表现速度有关又与位置高度有关,在塔底部呈现负值,这意味着向塔轴心方向流动。随着塔高增加。流动方向逐渐转变为向塔壁方向,且又有明显的峰值。     

气液鼓泡塔液体流动状态的声发射检测

提出一种基于声发射气液鼓泡塔液相流动状态检测方法,将多通道声发射传感器等距地置于鼓泡塔轴向壁面,提取不同表观气速下的各通道声发射信号,对其做经验模态分解(EMD),根据每个imf的Hurst指数值,提取和重构相应的imf,求其每个信号的平均能量。实验结果表明:鼓泡塔壁处液体轴向流速随着表观气速的增加而增大,当表观气速为14 m/min时,塔壁处液体轴向环流速度最大,当表观气速大于18 m/min时,液体轴向完全变为湍流,出现严重返混。声发射检测法能够有效检测出液体流动状态。     

气液两相鼓泡塔流区及其过渡的混沌分析

应用确定性混饨分析技术,以气液两相鼓泡塔内的压力波动时间序列为分析对象,系统研究了鼓泡塔系统的混饨特性．结果表明,鼓泡塔内气液两相流动系统为混饨动力学系统,混饨特征参数最大Ｌｙａｐｕｎｏｖ指数、Ｋｏｌｍｏｇｏｒｏｖ熵和关联维数Ｄ２等可以有效地表征鼓泡塔的流区及其过渡．混沌分析为定量判别鼓泡塔的流区及其过渡提供了新途径．操作条件对鼓泡塔内气液两相流动的混沌特性影响显著,表现为混沌特征参数值随表观气速增加而增加,随表观液速增加而减小,但是,混沌特性随空间位置的变化不显著．     

多级鼓泡塔中液相返混系数与交换速度的研究

采用示踪方法对高2 000 mm,内径282 mm多级筛板鼓泡塔内液相返混系数进行测量研究,并通过扩散-返混模型以及RTD曲线给出鼓泡塔内筛板上下二侧液体交换速度,同时考查了表观气速、开孔率等因素对轴向扩散系数与液体交换速度的影响.根据实验得出鼓泡塔内轴向返混系数以及液体交换速度与表观气速、开孔率有很大关系,均随表观气...     

气液鼓泡床内的液体流速分布

引言 鼓泡床是一种重要的气液或气液固多相反应器.液体循环流动是鼓泡床的一个重要流体力学特征,从20世纪50年代人们就开始对此进行了比较系统的实验研究[1-6].这个特征对鼓泡床的流体返混行为、气含率、气液界面积以及传热传质系数都有很大影响,特别是液体返混行为可以由液体循环特性直接决定.如何准确地描述和预测鼓泡床中的液体流速沿径向的分布,关系到鼓泡床反应器的设计、放大和优化.因此,许多年来它一直是人们致力探讨的重要课题之一[7-8].     

填料特性对鼓泡填料萃取塔性能影响

填料的结构与表面性能对鼓泡填料萃取塔性能有直接影响。利用空气 煤油 (苯甲酸 ) 水体系 ,测定了未装填料和分别装填板波填料、丝网填料、压延孔环填料的鼓泡萃取塔水力学性能和传质性能。实验表明 ,对未装填料和装有填料的萃取塔 ,气相搅拌都可以显著提高液液两相的接触与传质性能 ;液泛速度随表观气速的增大而下降 ;流道设计合理的规整填料传质性能明显高于散装填料 ;表面光滑的填料分散相滞存率低 ,因而液泛速度较高 ;填料的作用有利于降低轴向返混 ,明显提高萃取塔传质性能。     

气液两相单孔鼓泡过程的混沌分析

运用确定性混沌分析技术 ,研究了气液两相单孔鼓泡过程的混沌机理 .结果表明 ,单孔鼓泡过程是由周期及拟周期鼓泡通向混沌的 .鼓泡过程随气体流量增加可分为 3个动力学流区 :周期鼓泡区、混沌鼓泡区及喷射区 .     

不同分布器对鼓泡塔气液两相流影响的CFD模拟

对不同分布器的鼓泡塔反应器内的气液两相流体动力学行为进行了三维瞬态数值模拟.模型采用欧拉-欧拉双流体模型以及RNG κ-ε湍流模型,研究了不同分布器设计对鼓泡塔反应器气液两相流的影响.模拟得到了鼓泡塔内整体气含率、液相速度矢量分布、时均气含率以及时均轴向液速的径向分布等结果,并对部分模拟结果与文献实验结果进行了比较,其结果吻合得较好,证实了随着分布器开孔越均匀则有利于加强流形的非对称性,从而加剧了气液两相径向混合,但对整体气含率的影响不大.     

非牛顿型浆液鼓泡塔内气含率轴向分布实验研究

通过实验研究，得到了非牛顿型浆液鼓泡塔内压力的轴向分布关联式，进而得到了塔内气含率的轴向分布式。为进一步研究非牛顿型浆液鼓泡塔流体力学行为打下基础。     

鼓泡床中的气泡尺寸分布

根据气泡聚并和破裂速率模型,提出一个描述鼓泡床中气泡尺寸分布的总体平衡(Population Balance)模型。该模型可预计鼓泡床中气泡尺寸分布随床高的变化。对空气-水体系的模拟结果与实测结果吻合较好。     

鼓泡床反应器中液体循环的模拟

应用分离流概念对气液鼓泡床反应器中的两相流体动力学进行了理论分析,从而建立了一个基于机理的液体循环的数学模型。根据这个模型,对影响液体循环的诸因素及部分实例进行了模拟计算,其结果与实验结果吻合很好。     

鼓泡塔中浮力驱动环流特征及反应器放大

针对鼓泡塔一维流动模型,应用新分析方法首次给出环流特征参数（如速度转折点、最大Reynolds剪应力及其位置以及最大回流速度点）的具有明确物理含义的理论表达式,并比较了该关系式与既有结果的异同,分析了气含率分布与Reynolds剪应力的相互关系,提出一种基于流体动力学相似的鼓泡塔放大准则,即以所导出的最大Reynolds剪应力作为特征量,若几何尺寸不同的两个塔满足流体动力学相似,则该剪应力近似相等或具有相同的量级,对比分析表明,该准则对直径介于0.14～5.5m的鼓泡塔近似成立。     

鼓泡塔中的有效涡扩散系数及湍流特性

依据湍流模式理论提出新的有效涡扩散系数关系式,讨论其与既有关系式的异同并与湍流实测数据比较,结果表明,本文关系式给出与实测值更为一致的结果,而既有的一些关系式的计算值偏高．由此讨论了涡扩散系数与鼓泡塔流动模型的关系,指出了数据偏差产生的原因．     

A SIMPLE EXPERIMENTAL TECHNIQUE TO MEASURE GAS PHASE DISPERSION IN BUBBLE COLUMNS

A new technique to measure gas phase dispersion in bubble columns is presented. This technique is fairly simple to implement, accurate and inexpensive as compared to conventional methods used in the literature. Nitrogen is used as a tracer and a step change is effected by switching from air to the tracer, nitrogen. The gas phase concentration of oxygen is monitored by means of a polarographic oxygen sensor. The system studied is air-water and the experimental results compare well with the literature data. The technique presents a simple way to measure gas phase axial dispersion in bubble columns and can also be applied to other types of reactors     

A SIMPLE EXPERIMENTAL TECHNIQUE TO MEASURE GAS PHASE DISPERSION IN BUBBLE COLUMNS

A new technique to measure gas phase dispersion in bubble columns is presented. This technique is fairly simple to implement, accurate and inexpensive as compared to conventional methods used in the literature. Nitrogen is used as a tracer and a step change is effected by switching from air to the tracer, nitrogen. The gas phase concentration of oxygen is monitored by means of a polarographic oxygen sensor. The system studied is air-water and the experimental results compare well with the literature data. The technique presents a simple way to measure gas phase axial dispersion in bubble columns and can also be applied to other types of reactors     

DISPERSION OF GAS AND LIQUID IN BUBBLE COLUMNS OF HOMOGENEOUS BUBBLE FLOW REGIME

Mean gas holdup, lateral distribution of gas holdup and axial mixing of gas and liquid were measured in bubble columns of 12 and 19cm i.d. The lateral distribution of gas holdup was strongly dependent on the flow regimes in the column. The axial mixing of liquid in the homogeneous bubble flow regime was much smaller than that in the heterogeneous bubble flow regime, and was not expressed by existing correlations. The axial mixing of liquid in the homogeneous bubble flow and the intermediate flow regime was simulated with a flow model based on the lateral distribution of buoyancy force and the effective viscosity. The axial mixing of gas was larger than that of liquid.     

PHASE DISTRIBUTION AND MIXING IN A JET BUBBLE COLUMN

This paper describes the results of an experimental study to evaluate phase holdups and RTD for a jet bubble column. The experimental data were obtained in a 61 cm diameter jet bubble column with a conical inlet. Air and water were used as a two-phase system. The ranges of gas and liquid velocities examined were 0 to 9 cm/sec and 0 to 0·6 cm/sec respectively, both based on the cylinder diameter. The experimental data indicate that in the conical section of the column, the gas holdup first decreases with an increase in distance away from the cone inlet, achieves a minimum and then increases until it reaches a somewhat constant value within the cylinder. Gas holdup varies radially with the maximum at the center and the minimum near the wall. Radially-averaged gas holdup increased with gas velocity and remained essentially unchanged with liquid velocity. The RTD measurements were correlated by a two-dimensional dispersion model. The axial dispersion coefficient increased linearly from the cone inlet to the cylinder. It also increased with the gas velocity. The radial dispersion coefficients were considerably smaller than the axial dispersion coefficients.     

MULTI-SCALE CHARACTERISTICS OF CHAOS BEHAVIOR IN GAS-LIQUID BUBBLE COLUMNS

The multi-value phenomenon of correlation dimension appearing in chaos analysis of time series of pressure fluctuation obtained from gas-liquid bubble columns was studied. Its relationship with multi-scale flow behavior and possible application in the identification of flow regime and regime transition in bubble columns were investigated. The results indicated that the multi-value phenomenon of correlation dimension results from the multi-scale behavior existing in the heterogeneous churn flow regime in bubble columns. When a bubble column is in the homogeneous flow regime, only one correlation dimension is found at a specified superficial gas velocity, indicating that single-scale behavior is dominant in the system. When a bubble column is in the heterogeneous churn flow regime, multi- (generally three) correlation dimensions can be obtained, showing the appearance of multi-scale behavior. Therefore, the formulation of an effective flow model depends on an appropriate multi-scale analysis for bubble columns. Flow regime and regime transition can be characterized by the structure and structure variation of the plot of the correlation integral versus radius of the hyper-sphere. On the basis of the above analysis, a complementary potential methodology called correlation integral analysis for the identification of flow regime and regime transition in gas-liquid bubble columns is recommended.     

MULTI-SCALE CHARACTERISTICS OF CHAOS BEHAVIOR IN GAS-LIQUID BUBBLE COLUMNS

The multi-value phenomenon of correlation dimension appearing in chaos analysis of time series of pressure fluctuation obtained from gas-liquid bubble columns was studied. Its relationship with multi-scale flow behavior and possible application in the identification of flow regime and regime transition in bubble columns were investigated. The results indicated that the multi-value phenomenon of correlation dimension results from the multi-scale behavior existing in the heterogeneous churn flow regime in bubble columns. When a bubble column is in the homogeneous flow regime, only one correlation dimension is found at a specified superficial gas velocity, indicating that single-scale behavior is dominant in the system. When a bubble column is in the heterogeneous churn flow regime, multi- (generally three) correlation dimensions can be obtained, showing the appearance of multi-scale behavior. Therefore, the formulation of an effective flow model depends on an appropriate multi-scale analysis for bubble columns. Flow regime and regime transition can be characterized by the structure and structure variation of the plot of the correlation integral versus radius of the hyper-sphere. On the basis of the above analysis, a complementary potential methodology called correlation integral analysis for the identification of flow regime and regime transition in gas-liquid bubble columns is recommended.