降膜式吸收器的研究进展

综述了国内外水平管、垂直管和平板式降膜式吸收器的研究现状,对吸收器传热系数、传质系数和计算模型的研究进展。发现在降膜式吸收器中,氨水溶液形成的液膜是研究重点,传热和传质的阻力主要来源于液膜一侧。分析表明,改善降膜表面,增加液膜的扰动,添加纳米材料和添加磁场等措施可以显著提高液膜的传热传质系数,进而提高吸收器的吸收性能。进一步改善计算模型,提高液膜的传热传质能力将会是吸收器未来的研究方向,具有广阔的应用前景。     

新型气液逆流接触洗涤器流动-传质模型

通过冷模实验对一种新型气液逆流式洗涤器流动传质特性进行了考察。实验结果表明,在不同的操作条件下,洗涤器内气液两相流动会呈现出不同的流型。其中,洗涤器在泡沫流状态下的高效传质段体积和解吸率的数值均较大。将实验结果与理论分析相结合,依据其气液接触表面更新极快、形成高度湍动泡沫流的特点,提出了一种基于该洗涤器结构和操作特性、可以预测洗涤器传质效果的“两段式”流动-传质模型。模型将洗涤器内气液作用区分为两个区段：旋转射流段和高效传质段。利用该模型分析了解吸率与液气比L/G和旋流比ω的变化关系;结果表明,在不同操作条件下,该模型的计算结果与实验数据吻合较好,可供工程设计参考。     

新型气液逆流接触洗涤器流动-传质模型

通过冷模实验对一种新型气液逆流式洗涤器流动传质特性进行了考察。实验结果表明,在不同的操作条件下,洗涤器内气液两相流动会呈现出不同的流型。其中,洗涤器在泡沫流状态下的高效传质段体积和解吸率的数值均较大。将实验结果与理论分析相结合,依据其气液接触表面更新极快、形成高度湍动泡沫流的特点,提出了一种基于该洗涤器结构和操作特性、可以预测洗涤器传质效果的"两段式"流动-传质模型。模型将洗涤器内气液作用区分为两个区段:旋转射流段和高效传质段。利用该模型分析了解吸率与液气比L/G和旋流比ω的变化关系;结果表明,在不同操作条件下,该模型的计算结果与实验数据吻合较好,可供工程设计参考。     

旋流塔板传质模型研究

根据旋流塔板上的气液运动规律，建立气相二维定数混合池传质模型，并用ＣＯ_２－ａｉｒ／Ｈ_２Ｏ物系的传质试验结果进行验证，结果表明，模型计算值和实验值相当吻合。     

基于微吸收器的CO2吸收过程研究进展

微化工技术在流体流动、过程强化、传质与反应过程等领域备受关注,本文归纳整理了3种不同类型的微吸收器（微降膜吸收器、微通道吸收器和微网格吸收器）捕集CO₂过程中的水力学性质和传质过程及其机理研究进展,并对3种微吸收器吸收CO₂过程中存在的问题进行分析总结,同时对微吸收器能快速工业化提出展望。其中重点介绍了微通道泰勒流吸收器的水力学流动特性,包括泰勒流气泡的生成机制、气泡和液弹的长度、气泡的输运和运动速度、气泡截面形状及液膜厚度和气液两相流压降;归纳了微通道泰勒流吸收过程的传质过程机理和传质系数的模型以及不同影响因素（通道截面尺寸,通道长度,主通道结构及入口形状,气、液相组成及其流速,吸收剂和系统压力）作用下CO₂吸收效率和传质系数的研究进展。     

酸性气体膜吸收过程中浓差极化

用聚丙烯中空纤维膜吸收器，针对酸性气体膜吸收传质过程，根据浓差极化时存在局部高浓度区的特点，分别进行了SO2/空气混合气和CO2/空气混合气中酸性气体的选择性吸收实验. 实验测定了SO2和CO2两种不同酸性气体在不同浓度吸收液及不同液速下的总传质系数，比较了两种酸性气体在液相侧的传质特性，根据两组份间化学反应机理的不同，分析了浓差极化对膜吸收过程的影响.     

液体表面活性剂膜的传质模型

本文提出了一个新的关于液膜传质的模型.该模型不仅考虑了溶质在乳状液球内核中的渗透过程,还考虑了由表面活性剂所致的界面阻力升高效应,因而更加准确地描述了液膜体系的传质过程.该模型的另一个特点是考虑了在传质过程中膜的破裂,从而使数学模型更加迫近液膜体系的实际情况.实验结果与理论分析均表明,溶质透过乳状液外围的表面活性剂薄层的分子扩散是整个液膜传质过程的速率控制段.这一结论将导致对液膜结构更加深刻的理解,并将有助于液膜体系的改进.     

旋转填充床中伴有可逆反应的气液传质

应用CO2-MDEA气液吸收体系,对旋转填充床中伴有可逆反应的气液传质过程进行了定量的模型研究。在所有反应都可逆的情况下,根据Higbie渗透理论建立了旋转床中CO2-MDEA体系的扩散-反应传质模型。通过模型对传质过程的定量描述以及实验结果对模型的验证,超重力旋转床的强化作用可进一步被揭示为:由于不断更新的液膜使得可溶性气体在液膜内形成较大的浓度梯度,从而极大地增大了传质系数,强化了传质;旋转床的强化作用是在动态的传质过程中完成的,液膜的寿命越短则传质系数越大。在不同转速、温度、MDEA浓度和气液流量条件下进行了实验,本文模型的模拟值和实验结果吻合较好。     

气-液两相降膜流动及传质过程的CFD研究

利用VOF法建立了考虑表面张力动量源项、气液相间摩擦力动量源项以及相问传质源项的CFD计算模型,定量描述了气．液两相逆流降膜传质过程。根据CFD模型,计算了不同液相进口浓度和不同气相流量条件下,异丙醇稀溶液的解吸过程,模拟得到的液相出口浓度与实验数据吻合很好。相界面处的浓度分布表明。随自由表面波动,界面浓度会发生剧烈脉动。液相总传质系数增强因子R的实验值与CFD模拟均表明,即使在很小的传质推动力下R也大于1。由于CFD模型不考虑Rayleigh-Benard-Maragoni效应,则这种现象,可解释为界面波动对传质增强的结果。这也证明增强界面波动是一种强化传质分离过程的有效途径。     

水力喷射空气旋流器分离空间结构对气液传质性能的影响

水力喷射空气旋流器(WSA)是一种利用液体射流在气体旋流场中雾化强化气液传质的新型传质设备, 可广泛用于废水、废气处理等环境工程过程中。为了优化水力喷射空气旋流器的分离空间结构, 本文通过废水氨氮吹脱实验对柱锥结合形WSA和柱形WSA分别进行了气液传质性能研究。研究结果表明, 分离空间结构对水力喷射空气旋流器的气液传质性能存在影响。在相同工作条件下, 与柱形WSA相比, 柱锥结合形WSA具有更好的气液传质性能和略高的气相压降, 后者吹脱氨的体积传质系数提高了约8%, 主要原因在于柱锥结合形WSA内部具有更好的射旋流耦合雾化作用和离心超重力强化传质的综合效果, 使得两相比传质面积增大, 传质效率增高。研究结果可为设计传质性能良好的WSA提供设计依据。     

Gas absorption into a turbulent liquid

Mass transfer coefficients were measured for the liquid phase for gas absorption into a turbulent liquid flowing down a long wetted-wall column. Helium, hydrogen, oxygen and carbon dioxide were absorbed into distilled water over a Reynolds number range of 1300–8300. The results indicate that the liquid phase mass transfer coefficient is proportional to the molecular diffusion coefficient raised to the 0·54 power. The results are interpreted in terms of an eddy diffusivity model and indicate that the eddy diffusivity increases as the square of the distance from the interface.     

The influence of molecular diffusion on mass transfer between turbulent liquids

The influence of molecular diffusion on liquid—liquid mass transfer in a stirred transfer cell has been found by measuring the rates transfer of helium and iso-butane from water to toluene and dekalin. These solutes have very different diffusion coefficients, their presence does not alter the physical properties of the liquids and, because their equilibrium distributions strongly favour the organic phases, the water phase mass transfer coefficient could be determined and was found to depend on the square root of the diffusion coefficient.The results are compared with the predictions of a model for liquid—liquid mass transfer under turbulent conditions, based on the approach of an eddy to the interface being restrained by interfacial tension and gravitational forces and taking into account eddy pressure fluctuations in both phases. This model provides a correlation for these results, as well as water phase mass transfer coefficients for the transfer of iso-butane from water to n-octanol, and previous stirred transfer cell results.     

聚四氟乙烯膜气体吸收数学模型和孔隙率的影响

膜吸收是将膜分离与传统的吸收技术相结合的一种新型分离技术。在这些过程中经常使用多孔膜,多孔膜对过程的传质性能有一定的影响。对不同孔隙率的微孔聚四氟乙烯(PTFE)疏水性平板膜的膜气体吸收过程中液相传质性能进行了实验研究。当采用去离子水-CO2吸收体系时,多孔膜的孔隙率对液相传质性能没有影响;当采用NaOH水溶液-CO2吸收体系时,多孔膜的孔隙率对液相传质性能有明显的影响。在相同流速下,孔隙率大的膜液相传质系数高于孔隙率小的膜。以双膜理论为指导,建立了多孔膜气体吸收过程中液相传质模型。用该模型描述多孔膜孔隙率对液相传质系数的影响,其结果与实验数据具有良好的一致性。     

填料塔气液传质参数研究（Ⅰ）──有效传质面积及容积传质系数

用化学吸收法测定了拉西环填料的有效传质表面积和容积传质系数，并进一步用物理法比较测定了容积传质系数。实验证明，用化学法测得的容积传质系数大于物理法测定值。并得出有效传质表面积及容积传质系数与喷淋密度的关系式。     

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。     

Effect of Tween 80 on Bubble Size and Mass Transfer in a Bubble Contactor

Gas absorption in aqueous solutions with Tween 80 and absorption processes based on hydrodynamics and mass transfer is determined. The impact of surfactant concentration on gas holdup and gas‐liquid interfacial area is analyzed, observing an increase of these parameters with surfactant concentration. The influence of liquid‐phase contamination on the absorption process is investigated on the basis of the liquid‐film mass transfer coefficient, removing the effect caused by the presence of a surfactant and the gas flow rate on the interfacial area and, thereby, on the volumetric mass transfer coefficient. The opposite effect on the mass transfer coefficient can be observed which decreases in the presence of the surfactant.     

微通道内MEA/MDEA混合溶液吸收CO2的传质特性

研究了T形微通道内N-甲基二乙醇胺（MDEA）和单乙醇胺（MEA）混合水溶液吸收CO₂的传质过程。考察了弹状流型下气液两相流量、MEA和MDEA浓度对液侧传质系数k_L和体积传质系数k_La的影响。液侧传质系数和体积传质系数均会随着MEA浓度的升高而升高。与MEA相比,MDEA浓度的提高对传质影响较小。传质系数会随着液体流量的增大而增大,但气体流量的变化对其影响较小。体积传质系数随液体流量的增大而增大,但随气体流量的增大先增大,之后趋于稳定。考虑到化学反应对传质的强化作用,引入了Hatta数,提出了一个新的体积传质系数预测式,预测效果良好。     

SIMULTANEOUS ABSORPTION OF H2S AND CO2 INTO A SOLUTION OF SODIUM CARBONATE

The simultaneous absorption of H₂S and CO₂ has been studied both experimentally and theoretically. A model has been developed which predicts the absorption rates of H₂S and CO₂ into a sodium carbonate solution. The absorption rates are calculated according to the two-film theory. In the liquid film, the finite rate of the CO₂ reaction was considered. Otherwise, in the liquid film as well as in the liquid bulk, equilibrium conditions for all reactions were assumed. Absorption experiments were performed on a packed column using a counter-flow strategy. In the experiments the influence of the initial carbonate concentration, the gas flow rate and the temperature on the removal efficiencies of H₂S and CO₂ and the selectivity of H₂S were investigated. It is desirable to absorb the H₂S but not the CO₂. The agreement between the absorption model and the experimental results from the absorber tower was satisfactory. The mass transfer coefficients were determined by fitting the experimental data to the model with respect to the H₂S and CO₂ content in the outgoing gas. The H₂S content was used to determine the gas side mass transfer coefficient and the CO₂ content was used to determine the liquid side mass transfer coefficient, The effective contact area of mass transfer was taken from published data. With a constant packing height, both the experiments and the model indicated that high carbonate concentration benefits the removal efficiency of H₂S. Higher gas flow rate also benefits the selectivity for H₂S. However, the removal efficiency will decrease. At higher temperatures the selectivity and the removal efficiency of H₂S decreased. Under the conditions investigated, the absorption of H₂S was essentially controlled by gas-side mass transfer and the absorption of CO₂ was controlled by liquid-side mass transfer     

方肋微通道内流动沸腾的气泡动态与传热特性分析

为揭示方肋微通道热沉内流动沸腾的传热传质机理,本文基于耦合VOF方法与“饱和界面”相变模型对微通道内单个气泡绕流加热方肋的传热传质过程进行了数值研究。通过分析该过程中气泡增长速率与方肋壁面传热系数的变化,重点讨论了初始气泡体积和入口雷诺数Re对相变传热效率和流动结构的影响。结果表明：在气泡流经加热方肋过程中,气泡与方肋表面之间形成一层薄液膜,该薄液膜的相变蒸发极大强化方肋表面的换热效果,换热系数较相同条件下的单相流动提升6倍以上。此外液膜厚度随Re增大而变厚,液膜热阻相应增大,液膜蒸发对换热的促进作用随Re增大而降低。最后考察了气泡体积对方肋壁面换热的影响,结果表明：初始体积大的气泡具有更薄的液膜厚度及更大的蒸发面积,表现出更高的相变传热效率;而小气泡对壁面温度影响较小。     

Mass transfer in trickle-bed reactors at low reynolds number

Mass transfer rates were determined in a 3.4 cm i.d. trickle-bed reactor in the absence of reaction by absorption measurements and in presence of reaction. Gas flow rates were varied from 0-100 l/h and liquid flow rates from 0-1.5 l/h. The catalyst particles were crushed to an average diameter of 0.054 and 0.09 cm. Mass transfer coefficients remained unaffected by change in gas flow rate but increased with liquid rate. The data from absorption measurements were evaluated with predictions based upon plug-flow and axial dispersion model. Mass transfer coefficients were found greater in case of axial dispersion model than that of plug-flow model specially at low Reynolds number (Re₁ < 1).Hydrogenation of α-methylstyrene to cumene using a Pd/Al₂O₃ catalyst was taken as a model reaction. Intrinsic kinetic studies were made in a laboratory-stirred-autoclave. Mass transfer coefficients were determined using these intrinsic kinetic data from the process kinetic measurements in trickle-bed reactor. Mass transfer coefficients under reaction conditions were found to be considerably higher than those obtained by absorption measurements.Correlations were suggested for predicting mass transfer coefficients at low Reynolds number.The gas to liquid mass transfer coefficients for lower gas and liquid flow rates were determined in a laboratory trickle-bed reactor. The effect of axial dispersion on mass transfer was considered in order to evaluate the experimental data. Three correlations were formulated to calculate the mass transfer coefficients, which included the effect of liquid loading, particle size and the properties of the reacting substances. The gas flow rate influences the gas to liquid mass transfer only in the region of low gas velocities. In the additional investigations of gas to liquid mass transfer without reaction in trickle-bed reactor, the mass transfer coefficients were determined under reaction conditions and the intrinsic kinetics was studied in a laboratory scale stirred autoclave with suspended catalyst. A few correlations are formulated for the mass transfer coefficients. A comparison with the gas-liquid mass transfer coefficient obtained by absorption measurements showed considerable deviations, which were illustrated phenomenologically.