单乙醇胺水溶液化学吸收CO_2的研究

有机胺水溶液化学吸收CO2在工业上广泛应用,对其传质过程的微观机理进行研究十分必要。文中以对流扩散方程为基础,考虑了界面阻力对传质的影响,建立了带有化学反应的气液吸收过程液相侧非稳态传质模型,得到了传质系数表达式。利用激光全息干涉仪对不同液相主体流速下单乙醇胺(MEA)水溶液化学吸收CO2过程进行了实验研究,测定了传质达到稳态时的液相侧近界面浓度、浓度边界层厚度和传质系数。结果表明:随着液相主体流速的增加,近界面浓度和浓度边界层厚度减小,而传质系数增大;MEA在水溶液中的质量分数由0.1%增大到0.2%时,CO2吸收过程达到稳态时的近界面浓度、浓度边界层厚度及传质系数均增大。传质系数模型计算值与实验值吻合良好。     

基于浓度/速度场测量的吸收过程液相传质系数

针对矩形流道内气、液流体的并流吸收传质过程,分别应用实时激光全息干涉术和激光多普勒速度仪对不同气、液流速下液相内近界面浓度分布与速度分布进行了实验观测.结果表明,边界层内浓度分布呈指数下降,流速越大梯度越陡,且速度边界层厚度要大于浓度边界层厚度.建立了通过物料衡算求算液相传质系数的方法.得到了不同条件下平均液相传质系数,并与Whiteman’s双膜理论的计算结果进行了比较.     

气泡传质过程近界面非稳态特性及热力学研究

利用实时显微激光全息干涉测试技术 ,对运动气泡传质过程近界面的非稳态特性及浓度分布进行了实验测定 ,讨论了近界面湍动性质、稳态性质、非平衡性质及其关系 ,考察了流速、泡径、温度等因素对气泡传质过程的影响     

单个运动气泡近界面浓度场的研究

对单个气泡传质的近界面浓度场影响因素进行了实验和理论研究．实时激光全息干涉法测量结果表明,运动气泡近界面浓度是一个定态值,受流速、泡径、温度等因素影响显著;假设该传质过程达到局部平衡,进行热力学分析,得到的结论与实验结果一致．在实验测量结果的基础上,对单个O_2气泡在乙醇中吸收时的传质近界面浓度场进行了数值模拟,取得了良好的结果．     

吸收过程的界面传质机理

以分子热力学为基础 ,对气体吸收过程进行了理论分析 ,导出了传质通量的数学表达式。根据该文分析 ,气液界面传质的源动力来自界面处气液两相的不平衡 ,即只要有传质发生 ,液相界面处的浓度就不会达到与气相呈平衡的浓度。对于气相阻力可以忽略的吸收过程 ,两相传质速率的大小主要取决于液相的溶质界面浓度和液膜厚度 ,影响溶质界面浓度和液膜厚度的主要因素是近界面液相侧的流场分布。利用近界面浓度与液膜厚度的激光测定结果 ,计算了甲醇、乙醇及正丙醇吸收CO2 气泡的传质通量 ,计算结果与实验值吻合良好     

吸收过程的界面非平衡传质机理

针对气体吸收过程,以分子热力学为基础,结合普遍化的化学势推动力通量方程,导出了传质存在时两相界面处的浓度关系,并针对不同情况进行了求解.提出了一个反映液相侧动力学状况的无因次数群Biot数Yo,Yo数越大界面处两相越偏离平衡.界面浓度是与Yo和液相主体浓度密切相关的.对于气相阻力可以忽略的吸收过程,两相传质速率的大小主要取决于液相的溶质界面浓度和液膜厚度.采用激光显微全息干涉技术对甲醇,乙醇,正丙醇静止吸收CO2时的界面浓度进行了测定,试验结果表明了本研究模型的正确性.     

气液并流吸收近界面浓度分布不稳定性实时观测

气液自由界面附近的瞬时浓度分布信息对于理解相际传质动力学很重要。利用激光全息干涉测量系统分别对乙醇、甲醇并流吸收CO2过程中液相内近界面的摩尔分数分布进行了实时观测。研究表明,水平槽道内气液流动传质过程中液相内的不稳定性现象是普遍存在的。它主要包括界面湍动和周期性脉冲爆发2种形式。当传质达到稳态时近界面CO2摩尔分数的分布结果表明,流场内存在着微弱的摩尔分数波动。吸收体系的性质和流速直接影响传质推动力的大小,从而决定摩尔分数波动的强度及深度。     

气液界面传质机理

提出了气液相际传质的推动力来源于界面不平衡的概念.针对气体吸收过程, 以普遍化的化学势推动力方程为基础, 导出了在有传质通量存在下的两相界面处的浓度关系,并针对不同情况进行了求解.提出了一个反映液相侧动力学状况的量纲1数Yo ,Yo越大界面处两相越偏离平衡.界面浓度是与Yo和液相主体浓度密切相关的.为验证本文模型, 作者采用显微激光全息干涉技术对甲醇、乙醇、正丙醇静止吸收CO₂时的界面浓度进行了测定, 实验结果表明了本文模型的正确性.     

加入第二液相强化气液传质

以水吸收二氧化碳为研究体系,考察了第二液相(有机相)的加入对气液传质的增强作用.运用经验关联式,对气泡平均直径进行了预测,应用渗透模型计算并讨论了第二液相的加入对气液接触界面积、体积传质系数的影响.实验结果表明:不同搅拌速度对气泡大小影响不同,适宜的搅拌速度有利于传质;少量的第二液相的加入减少了气泡聚并现象,增大了气液接触界面积.气液传质增强效果用增强因子表示.     

液液界面传质过程的激光干涉法研究

为了研究液液传质过程的界面现象及传质特征,采用实时激光全息干涉技术,根据不同初始浓度时乙醇通过油水界面传质过程的全息干涉图,得到了传质过程水相侧的浓度分布,据此求出了近界面浓度和基于浓度的传质系数,并关联了近界面浓度与主体相溶质浓度的关系。建立了界面能随溶质浓度改变的函数关系,计算结果与实验值吻合良好。研究结果表明,液液静止界面传质过程基本符合双膜理论,溶质的加入能改变界面性能,传质过程界面处于非平衡状态。     

Utilization of the pressure differential records from gas fluidized beds with internals for bubble parameters determination

Simulated pressure gradient records, based on the theoretical pressure field around a bubble in fluidized bed derived by Davidson, are analysed by statistical methods to determine significant bubble parameters. It is shown that from two records measured by two pairs of pressure differential probes located on common vertical axis the following can be computed: bubble velocity, bubble depth (diameter), vertical spacing of bubbles, bubbling frequency, distributions of bubble sizes and spacings, and local bubble phase fraction. Simulated and actual records of the passage of non-interacting single bubbles over four pairs of probes located in a fluidized bed with internals show good agreement.     

Local hydrodynamic properties of gas phase in an internal-loop airlift reactor

The local hydrodynamic properties of the gas phase in an internal-loop airlift reactor were investigated in this study. The hydrodynamic properties including gas holdup, bubble velocity and bubble chord length were measured by dual electrical resistivity probes. The chord length distribution was then transformed to the bubble size distribution by modeling the bubbles as ellipsoids. It was found that the gas holdup increased with decreasing bubble velocity. In addition, most bubbles tended to rise along the riser central axis. Thus, the gas holdup in the axis was higher. The bubble size, bubble velocity and gas holdup were relatively constant in the axial direction of the riser except in the zones near the gas sparger and the gas–liquid separator. The bubble velocity became slower when the bubbles approached the gas–liquid separator. Moreover, the bubble size and bubble velocity for the three-phase system were relatively insensitive to the radial direction compared to those for the two-phase system. It was also found in this study that the bubble rise velocity and bubble size for the three-phase system were lower than that for the two-phase system. However, the gas holdup for the three-phase system were higher than that for the two-phase system due to bubble breakage caused by the solid particles.     

顶部浸没竖直向下平口管口气泡膨胀脱离特性

利用高速摄像机拍摄顶部浸没竖直向下管口气泡膨胀及脱离演变过程,对比分析管径、平均气速对气泡尺寸、形成时间的影响规律。引入泡龄k表征管口气泡位置特性,用椭球形气泡长短轴比L表征气泡形状特征。研究发现,气泡生成机理有间歇生成气泡、含抽吸间歇生成气泡和连续生成气泡3种;气泡脱离直径随平均气速变化过程明显存在气泡脱离形态转变点;气泡膨胀脱离模式随平均气速变化分为单个气泡形成、气泡聚并形成两种。平均气速为3.1 m·s^-1时管口处存在抽吸现象,此时最大泡龄k_max最小;脱离阶段气泡长短轴比L随脱离时间变化过程明显存在时间分界点。在分界点前,L值在2.0附近波动,气泡主要以椭球形存在。分界点后,L值明显增加,气泡形状向扁椭球体发展。     

CREEPING MOTION OF A BUBBLE WITH FIXED SURFACE CHARGE IN A UNIFORM ELECTRIC FIELD

Approximate solutions of the shape function and the electrophoretic movement of a bubble in an aqueous medium with ionized detergent and a small number of electrolytes under the influence of uniform electric field are derived. Specifically, a bubble that has the interface saturated and densely packed with detergent molecules is considered, and the charges were deemed to be fixed provided the position change among the detergent molecules is hindered relative to the free molecule. The surface tension at the interface is weakened with the addition of the detergent, and the deformation can be significant. The variation of the shape of the bubble was represented by the Legendre polynomial and the perturbed velocity profile was used to derive the drag force for the deformed bubble. The speed and size of the bubble was assumed to be very small so that the flow around it is in the creeping flow regime. The shape of the bubble with fixed surface charge undergoes a prolate deformation with axial symmetry around the axis parallel to the direction of the electric field and exhibits asymmetry with respect to the plane that goes through the center of the bubble and is perpendicular to the axis. But this asymmetry is not significant unless the surface charge density and the electric field are very large. Only symmetric deformation governs the movement, and, consequently, the drag force is not dependent on the sign of surface charge. As the bubble becomes more slender with deformation, the movement is enhanced.     

CREEPING MOTION OF A BUBBLE WITH FIXED SURFACE CHARGE IN A UNIFORM ELECTRIC FIELD

Approximate solutions of the shape function and the electrophoretic movement of a bubble in an aqueous medium with ionized detergent and a small number of electrolytes under the influence of uniform electric field are derived. Specifically, a bubble that has the interface saturated and densely packed with detergent molecules is considered, and the charges were deemed to be fixed provided the position change among the detergent molecules is hindered relative to the free molecule. The surface tension at the interface is weakened with the addition of the detergent, and the deformation can be significant. The variation of the shape of the bubble was represented by the Legendre polynomial and the perturbed velocity profile was used to derive the drag force for the deformed bubble. The speed and size of the bubble was assumed to be very small so that the flow around it is in the creeping flow regime. The shape of the bubble with fixed surface charge undergoes a prolate deformation with axial symmetry around the axis parallel to the direction of the electric field and exhibits asymmetry with respect to the plane that goes through the center of the bubble and is perpendicular to the axis. But this asymmetry is not significant unless the surface charge density and the electric field are very large. Only symmetric deformation governs the movement, and, consequently, the drag force is not dependent on the sign of surface charge. As the bubble becomes more slender with deformation, the movement is enhanced.     

非牛顿流体中的两并行运动气泡周围流场及气泡间相互作用的PIV研究

The flow fields surrounding two parallel moving bubbles rising from two identical orifices submerged in non-Newtonian fluid of carboxymethylcellulose (CMC) solution of three different mass concentration were measured experimentally by the use of particle image velocimetry (PIV). The influences of gas flowrate, solution mass concentration, orifice interval and the angle between two bubble centers line and vertical direction on the flow field surrounding bubbles were discussed respectively by analyzing the velocity vector, velocity contours as well as individual velocity components. The results show that the liquid velocity both in front of two bubbles and behind increases with gas flowrate duo to shear-thinning effect of previous bubbles, whereas decreases with the increase of CMC concentration due to the increase of drag force acting on bubbles. The effect of the orifice interval on the flow field around two moving bubbles becomes gradually obvious as the interval becomes closer. Moreover, two adjacent side-by-side bubbles repulse each other during rising, leading to the practical interval between them increased somewhat above the orifice interval. When the distance between bubbles is less than the orifice interval l0 mm, the interaction between two neighboring bubbles changed from mutual repellence to attraction with the decrease of the angle of the line of linking two bubble centers to the vertical direction.     

电场作用下氮气泡行为的数值模拟和实验研究

为了探讨电水动力学强化沸腾传热机理,以水为实验工质,通过数值计算和实验观察相结合的方法,系统研究了冷态氮气泡在电场作用下的行为特性;并计算了直流电压10 kV工况下,气泡周围电场强度分布、气泡脱离周期和气泡脱离时刻瞬时速度场。结果表明:场强越大,气泡伸长变形越明显,脱离周期越短;电场强度沿着气泡轮廓方向逐步对称减小;气泡脱离时刻的速度随着电场强度的增大而增大且速度极大值处在气泡的底部。     

Effects of probe numbers and arrangement on the measurement of charge distributions around a rising bubble in a two-dimensional fluidized bed

The charge density distribution around a rising bubble in a two-dimensional fluidized bed was measured using eight induction probes flush with the outside wall of the column and connected to charge amplifiers for recording induced charge signals as bubbles passed by. The charge distribution surrounding the bubble was reconstructed using an iterative linear back projection (LBP) algorithm by assuming that the bubble is symmetrical and the charge around the bubble remains constant as the bubble rises. The results showed that the emulsion phase far from the bubble in a two-dimensional fluidized bed of glass beads was charged negatively, and the charge density decreased gradually toward the bubble-dense phase interface, with a nearly zero charge density inside the bubble. The effects of the number of probes are also investigated. The reconstructed results using both simulated charge distribution and experimental data for different numbers of probes of the same probe diameter of 3 mm showed that increasing the number of probes can improve the reconstruction resolution. The addition of one or two more probes outside the bubble path also increased the reconstruction resolution in the region outside the bubble.     

中等Reynolds数线性剪切泡状流的液相雷诺应力

Analytical investigation of liquid Reynolds stress in shear bubbly flow with intermediate Reynolds numbers is absent. In this paper, the velocity field around a sphere bubble in linear shear liquid is assumed to be the linear superposition of the velocity field of uniform liquid passing a sphere bubble and the linear shear velocity field. The formula of shear liquid Reynolds stress was derived by averaging the velocity field in the cell-ensemble averaging method, and the formula was corrected under conditions of intermediate Reynolds number. The formula was compared with that of Sato, and the predicted results of local liquid velocity of the fully developed upward bubbly flow in pipes were compared with the experimental data. The results show that the formula is valid and accurate in prediction.     

Influence du passage d'une bulle sur le coefficient instantané de transfert de chaleur à une paroi immergée dans un lit fluidisé

This paper deals with the study of the vigorous particle mixing around an artificial bubble injected in a fluidized bed using a hot film anemometric technique.The fluctuations of the heat transfer coefficient have been studied as a function of the bubble characteristics and position with respect to the probe.In the bubble injection axis the heat transer coefficient depends very much on the bubbling frequency but only slightly on the bubble diameter. On the other hand, the distance x between the transfer surface and the bubble track was found very important. In this study we also determined the critical values of the bubble diameter and frequency which characterize the beginning of interaction between two successive bubbles.We propose a velocity potential model so as to take into account the form of the agitation zone of particles around the bubbles.