气液逆流鼓泡塔中的气含率与液速分布和数值模拟

分别采用线－线电导探针和背靠背式皮托和测定了气液逆流鼓泡塔中局部气含率和液体轴向速度的径向和轴向分布,讨论了操作条件对气含率与液体轴向速度分布的影响,利用双流体模型对塔内两相湍流流动进行了数值模拟。     

螺旋气升式内环流反应器流动特性

以水和空气两相系统为研究对象,建立螺旋气升式内环流反应器冷模实验装置,采用压差法测定导流筒升流区气含率,用电导法分别实测了升流区液相速度和反应器混合时间,研究螺旋气升式内环流反应器的流动特性,并与传统气升式内环流反应器的流动特性进行对比研究。结果表明,加螺环后反应器气含率明显增加,平均增幅为20%,升流区液相表观速度减小,混合时间增加。     

液固下喷自吸环流反应器流体力学特性

采用改进皮托管测定了液固下喷自吸环流反应器中的液体平均速度及液相湍流强度分布,采用PV4A颗粒浓度速度测量仪测定了固含率分布。试验结果表明:随着液体喷射流量的增大,液体平均速度、液相湍流强度及固含率均增大;在导流筒内液相平均速度近似管流分布,在环隙中的速度分布基本均匀;在导流筒和环隙内固含率沿径向分布均匀。该研究对于下喷环流反应器的放大与优化有重要指导意义。     

带导流筒的下喷环流反应器的模拟及研究

本文通过引入二维拟均相κ－ε模型方程,建立了描述气液下喷环流反应器内管流区流体流动规律的数学模型,并进行了求解,模型值与试验值吻合较好。以空气－水－玻璃球为研究物系,对有导流筒的下喷式环流反应器中局部液相性能进行了较深入研究,并分析了各种参数对反应器内流体流动状况的影响     

小颗粒滴流床反应器的流体力学研究

在内径为０．０４７ｍ，床层高０．７ｍ的滴流床反应器内，采用空气－水－玻璃珠（１．８，３．１８ｍｍ）体系，在常温、常压下进行实验。气、液流速分别在０．０５４－０．２３ｋｇ／（ｍ＾２ｓ）和３．２０－１４．７３ｋｇ／（ｍ＾２ｓ）内，用电导信号脉动法、压降波动法结合目测法测定了滴流床的流动状态及其变化，实验结果可用于确定不同操作条件下的流动状态。本研究还分别是用差计、示踪剂法和体积法对滴流床的压降，总持流     

多室环流反应器气含率的三维数值模拟与分析

在常温常压条件下,以空气为气相、水为液相,对多室气升式环流反应器内气液两相流动状态进行了数值模拟,采用Euler两相流模型模拟了不同表观气速条件下各室气含率的分布情况。数值模拟计算结果表明,上升室气含率随表观气速的增大近似呈线性增长;各上升室气含率受自身表观气速的影响较大,而受另外一上升室表观气速的影响较小。     

超声微反应器内气液传质过程的介尺度强化机制

采用CFD方法对超声微反应器内的Taylor气液两相流的传质过程进行了模拟。针对传质过程中主要的介尺度结构,包括气泡表面波、空化声流、液相内的局部浓度,分析了其空间分布和时间演化规律。模拟结果有效捕捉了实验难以观测的液膜区域,并将液膜厚度与气泡表面波振动进行了关联,阐释了气液界面附近的空化声流对传质过程的强化作用。根据超声微反应器内Taylor流的传质特点,分别研究了不同流动和超声条件对液弹内和液膜处传质过程的影响,比较了各局部传质对整体传质效率的贡献。通过分析整体/局部Sherwood数与Peclet数间的关系,研究了超声效应对气液传质速率的影响。分析结果从介尺度角度验证了文献关于超声微反应器传质系数的计算,完善了超声微反应器内气液传质过程的强化理论。     

喷射环流反应器的放大效应

实验测量了两种塔径(?200和?500mm)和两种操作模式(气体单独喷射和气液同轴喷射)下喷射环流反应器内的全塔平均气含率、局部气含率及轴向液速径向分布、循环液速,归纳出全塔平均气含率的关联式。实验发现,喷射环流反应器具有十分显著的放大效应。小塔(?200)与大塔(?500)中的全塔平均气含率存在很大差异:小塔的全塔平均气含率～气速关系曲线比大塔陡峭,低气速下小塔气含率低于大塔、较高气速下高于大塔。根据漂移通量法分析得到小塔中流型转变点在表观气速0.1 m·s~(-1)左右,在实验气速范围内只存在拟均匀鼓泡流;大塔中流型转变点在表观气速0.04 m·s~(-1)左右,随气速增大从拟均匀鼓泡流转变为湍动鼓泡流。喷射环流反应器比气升式环流反应器、一般鼓泡塔全塔平均气含率略低,但循环液速更大,适用于强化固体悬浮与混合的气液固三相反应过程。     

非牛顿流体在气升式反应器中的流动特性

以非牛顿型流体在气升式内环流反应器中流动特性为研究对象，考察了在气－液－固三相体系中气含率和液体循环速度随不同的表观气速、固体颗粒粒径和浓度、设备结构尺寸的变化规律。对实验数据进行了回归处理得到气含率和循环速度的经验关联式，并对非牛顿型流体和牛顿型流体在同一反应器中的流动特性作了比较     

多相气升式环流反应器局部相含率和环流速度

气升式环流反应器流动特性研究大多都局限于流动参数的平均特性研究,涉及气-液-固系统流动特性的研究也较少。在200×2500mm气升式环流反应器内,实验研究了空气-水两相及空气-水-玻璃珠三相体系中局部气、固相含率以及浆(液)相环流特性等随操作条件以及液、固相物性的变化规律。结果表明:1两相体系导流筒中截面平均气含率轴向分布有局部极大值,而固体和乙醇的加入使得气含率轴向分布平缓;2两相体系循环液速在导流筒中呈径向抛物分布,在环隙分布较均匀,加入固体和乙醇后对循环速度分布和大小影响不大;3三相体系中导流筒内固含率沿轴向升高呈增大趋势,环隙内轴向分布均匀;导流筒内、外固含率径向分布均不均匀,以近壁处为大;加入乙醇后对固含率分布影响不大。     

LOCAL OVERALL GAS-LIQUID VOLUMETRIC MASS TRANSFER COEFFICIENTS IN A GAS-LIQUID TWO-PHASE REVERSED FLOW JET LOOP REACTOR

Local overall gas-liquid volumetric mass transfer coefficient profiles at the specified point were experimentally investigated in a gas-liquid two-phase reversed flow jet loop reactor with Newtonian and non-Newtonian systems. It was observed that the local overall gas-liquid volumetric mass transfer coefficient profiles of this reactor with Newtonian and non-Newtonian systems increase with increase in gas jet flow rates and liquid jet flow rates, and with decrease in nozzle diameter and CMC concentration.     

下喷自吸环流反应器内局部气泡平均直径及其径向分布

引　言喷射环流反应器因具有规整的流型、良好的分散效果、相对低的功耗及较好的相间传递特性等优点 ,而广泛应用于化学工业、生物及环境化工领域 ,如发酵、废水和废气处理等 ,以及化学工业中众多的多相反应[1,2 ].鉴于下喷环流反应器和自吸各自的特点 ,文献 [3]开发出了新型高效反应器———下喷自吸环流反应器 ,并对该反应器性能进行了系统的研究 .开展下喷自吸环流反应器内局部气泡大小及其分布的研究 ,不仅对了解该反应器内混合、相间作用和相间耦合的微观流动与传质机理及其传递特性具有极其重要的意义 ,而且也为此类反应器的工业放大…     

分布器结构对环流反应器气含率分布的影响

采用κ-ε二方程模型和欧拉多相流模型,对一种单筒单级气升式气液环流反应器内的湍流气液两相流进行了全尺寸的数值模拟研究,考察了采用3种不同气体分布器时反应器内气含率和流速分布的细节.模拟结果表明不同结构的分布器对总体气含率和内筒中的两相速度分布有很大影响,因而对气含率分布和气液两相接触效果有较大影响,从而对反应过程产生影响.单环分布器产生的气液两相接触效果较差,对于反应过程很不利.对于大直径的环流反应器推荐使用多环分布器.计算所得的整体气含率与实测的整体气含率进行了对比,吻合较好.     

CFD simulation of hydrodynamics of gas-liquid-solid fluidised bed reactor

A three dimensional transient model is developed to simulate the local hydrodynamics of a gas-liquid-solid three-phase fluidised bed reactor using the computational fluid dynamics (CFD) method. The CFD simulation predictions are compared with the experimental data of Kiared et al. [1999. Mean and turbulent particle velocity in the fully developed region of a three-phase fluidized bed. Chemical Engineering & Technology 22, 683-689] for solid phase hydrodynamics in terms of mean and turbulent velocities and with the results of Yu and Kim [1988. Bubble characteristics in the racial direction of three-phase fludised beds. A.I.Ch.E. Journal 34, 2069-2072; 2001. Bubble-wake model for radial velocity profiles of liquid and solid phases in three-phase fluidised beds. Industrial and Engineering Chemistry Research 40, 4463-4469] for the gas and liquid phase hydrodynamics in terms of phase velocities and holdup. The flow field predicted by CFD simulation shows a good agreement with the experimental data. From the validated CFD model, the computation of the solid mass balance and various energy flows in fluidised bed reactors are carried out. The influence of different interphase drag models for gas-liquid interaction on gas holdup are studied in this work.     

CFD analysis of two‐phase turbulent flow in internal airlift reactors

The hydrodynamic performance of three internal airlift reactor configurations was studied by the Eulerian–Eulerian k–ε model for a two‐phase turbulent flow. Comparative evaluation of different drag and lift force coefficient models in terms of liquid velocity in the riser and downcomer and gas holdup in the riser was highlighted. Drag correlations as a function of Eötvös number performed better results in comparison to the drag expressions related to Reynolds number. However, the drag correlation as a function of both Reynolds and Eötvös numbers fitted well with experimental results for the riser gas holdup and downcomer liquid velocity in configurations I and II. Positive lift coefficients increase the liquid velocity and decrease the riser gas holdup, while opposite results were obtained for negative values. By studying the effects of bubble size and their shape, the smaller bubbles provide a lower liquid velocity and a gas holdup. The effects of bubble‐induced turbulence and other non‐drag closure models such as turbulent dispersion and added mass forces were analysed. The gas velocity and gas holdup distributions, liquid velocity in the riser and downcomer, vectors of velocity magnitude and streamlines for liquid phase, the dynamics of gas holdup distribution and turbulent viscosity at different superficial gas velocities for different reactor configurations were computed. The effects of various geometrical parameters such as the draft tube clearance and the ratio of the riser to the downcomer cross‐sectional area on liquid velocities in the riser and the downcomer, the gas velocity and the gas holdup were explored. © 2011 Canadian Society for Chemical Engineering     

分布孔大小对环流反应器内流动影响数值模拟

采用k-ε二方程模型和欧拉多相流模型,对一种气升式环流反应器内的湍流气液二相流进行了全尺寸的数值模拟研究,考察了采用具有不同大小分布孔气体分布器时反应器内气含率和流速分布的细节。模拟结果表明采用小分布孔的反应器内的平均气含率较高,气液二相接触效果较好,对于反应过程有利。计算所得的整体气含率与实测的整体气含率进行了对比,吻合较好。     

气-液-固三相下喷环流反应器局部气相流动特性

The local gas-phase flow characteristics such as local gas holdup (εg), local bubble velocity (Vb) and local bubble mean diameter (db) at a specified point in a gas-liquid-solid three-phase reversed flow jet loop reactor was experimentally investigated by a five-point conductivity probe. The effects of gas jet flow rate, liquid jet flow rate, solid loading, nozzle diameter and axial position on the local εg, Vb and db profiles were discussed. The presence of solids at low solid concentrations not only increased the local εg and Vb, but also decreased the local db. The optimum solid loading for the maximum local εg and Vb together with the minimum local db was 0.16 × 10-3 m3, corresponding to a solid volume fraction, εS = 2.5%.     

气升式内环流反应器内局部气含率径向分布

The local gas holdup profiles in an internal-loop airlift reactor were studied experimentally by using dual electrical conductivity probe under different conditions,including superficial velocity,surface tension and liquid viscosity.The results showed that the radial gas holdup profile has a parabolic shape,which was consistent with the empirical model of Luo.Local gas holdup distribution parameters were obviously influenced by flow regime and almost remained unchanged in the same flow regime.In the gas distributor region,the profiles were steeper in the homogenous flow regime than in the heterogeneous flow regime.However,in the stable region,there was an inverse change trend in two flow regimes.The increase of surface tension,superficial velocity and liquid viscosity made the profile of local gas holdup steeper in two flow regimes.