急扩加速流缩放管气体换热器的结构及应用

根据传热场协同理论,研发出改进型缩放传热管——急扩加速流缩放管,对缩放管的凹凸肋面作了改进,使其能满足两场矢量夹角小于90°强化对流条件的传热管段比例由原先的60%提升到90%,从而有效地加强了近壁处传热滞流底层的对流传热作用。采用漩流片支撑取代空心环网板支撑,可使经过支撑物的流体形成自漩流的流动状态,从而可以发挥管间支撑物的对流强化传热作用。实际应用表明,与目前国内较先进的光滑管换热器相比,急扩加速流缩放管换热器换热面积减少约35%,设备总质量降低约45%。     

A NEW CLASS OF SIMILARITY SOLUTIONS OF AN UNSTEADY ELECTRICALLY CONDUCTING FREE-FORCED CONVECTIVE FLOW IN A VERTICAL POROUS SURFACE WITH DUFOUR AND SORET EFFECTS

The 2-D unsteady magnetohydrodynamic free-forced convective boundary layer flow of a viscous incompressible fluid is studied numerically taking into account heat and mass transfer. The fluid is subjected to uniform heat and mass fluxes embedded in a porous medium by the presence of coupled Dufour and Soret effects. A new class of similarity equations has been obtained by introducing a time-dependent length scale and a corresponding similarity variable. The resulting equations are then integrated numerically using the Nachtsheim-Swigert shooting iteration technique along with the sixth-order Runge-Kutta integration scheme. By developing locally similar solutions of the fluid flow, the behavior of the velocity, temperature, and concentration fields as well as the rate of heat transfer, wall temperature gradient, rate of mass transfer, and skin friction coefficient have been investigated. The effects of Grashof number (Gr), modified Grashof number (Gm), combined effects of the porous and magnetic parameter (S), suction/injection parameter Fw, Brinkman number (Br), Soret number (Sr), and Dufour number (D_f) have been observed on the flow field and discussed.     

稀疏气固两相湍流边界层拟序结构变动特性

应用PIV两相同时测量方法,对壁面Reynolds数为430的水平槽道稀疏气固两相湍流边界层拟序结构变动特性进行了研究。选取质量载荷为10^-4~10^-3的110 μm聚乙烯颗粒作为离散相。结果表明,低载荷颗粒仍能显著改变湍流拟序结构,进而影响宏观湍流属性。颗粒重力沉降形成的粗糙壁面增强了壁面附近湍流猝发行为,导致黏性底层中的气相法向脉动速度和雷诺剪切应力显著增大。颗粒与壁面的碰撞加强了低速流体上抛、削弱了高速流体下扫,同时增强了轨道交叉效应,从而抑制了湍流拟序结构发展,显著减小了黏性底层以上区域的法向脉动速度和雷诺剪切应力。此外,颗粒惯性还减小了黏性底层厚度、增大了流向速度梯度,导致气相流向脉动速度峰值增大,且其对应位置也更加靠近壁面。     

UNSTEADY FLUID AND HEAT FLOW INDUCED BY A STRETCHING SHEET WITH MASS TRANSFER AND CHEMICAL REACTION

The effect of chemical reaction on the flow, heat, and mass transfer within a viscous fluid on an unsteady stretching sheet is examined. The stretching rate, temperature and concentration of the sheet, and the chemical reaction rate are assumed to vary with time. The time-dependent boundary layer equations governing the flow are reduced through a convenient similarity transformation to a set of ordinary differential equations, which are numerically solved by applying the fourth-order Runge-Kutta-Fehlberg scheme with the shooting technique. Results for the velocity, temperature, and concentration distributions as well as the wall temperature and concentration gradients are presented graphically for various values of the unsteadiness parameter A, Prandtl number Pr, Schmidt number Sc, and chemical reaction parameter γ.     

Use of the polarographic method to measure wall shear stress

The measurement of the current to a small polarized electrode mounted flush to the wall allows the determination of the local velocity field closer to a surface than any other method. This technique has found use in measuring wall shear stresses in boundary-layer flows and in studying the structure of turbulence in the viscous sublayer. The interpretation of measurements in the wake behind a cylinder or behind a large amplitude wave is not clear because large amplitude flow oscillations make present analysis of the performance of these wall electrodes inapplicable. Recent numerical work on the inverse mass transfer problem seems to offer an approach that can handle measurements in these difficult flows.This paper was presented at the Workshop on Electrodiffusion Flow Diagnostics, CHISA, August 1990.     

THE TAYLOR PUMP: VISCOUS-FREE SURFACE FLOW DRIVEN BY ELECTRIC SHEAR STRESS

The pump invented by G.I. Taylor consists of low conductivity liquid in an insulated tank with electrodes at each end, one of which has an extension canted over the liquid/gas interface. When a potential difference is imposed between the electrodes, an electric shear stress acts on the interface and drives a Marangoni-like flow. The steady, two-dimensional flow of an incompressible, Newtonian, ohmic liquid in the tank is analyzed by solving simultaneously the Navier-Stokes equations for velocity and pressure in the tank and the Laplace equation for electric field in the liquid and the gas. The results show that an egg-shaped vortex develops in the liquid as the relative importance of inertial to viscous forces increases, in accordance with the experiments of Melcher and Taylor (1969). The methods developed here can be readily extended to analyze drop deformation and enhancement of mass transfer in two-phase systems due to an imposed electric field.     

小曲率蛇形微通道弯头处弹状流流动及传质特性的数值研究

采用CLSVOF（coupled level set and volume of fluid）方法,以空气和水为工作流体对小曲率矩形截面蛇形微通道内气液两相流动进行模拟研究。验证模型的合理性后,研究了曲率对弯通道内压降的影响,曲率及气相速度对弹状流气泡及液塞长度的综合影响;同时深入分析了弯管内气液两相流动的传质特性,包括不同曲率下气泡长度的变化,弯管内液侧体积传质系数与液膜体积传质系数的比较,曲率及气相速度对液相体积传质系数的影响。同时,对比了回转弯道与直微通道传质系数的差异,发现弯微通道可以强化传质。     

微通道中钒的液-液流型和萃取传质动力学研究

采用伯胺N1923萃取剂在微通道中研究V(V)的液-液流型和萃取传质动力学,以15vol% N1923作为连续相、钒氧酸根水溶液作为分散相,研究不同流速下两不混溶相的流型变化规律及两相停留时间和微通道管径作为流速的函数对传质的影响。随两相流速增大,段塞流长度和比界面面积基本不变,且两相流体由Raydrop微通道流入外接毛细管微通道时由于微通道的扩张会改变两相流动方式,使同一实验条件下在微通道中同时出现多种流型,与此同时两相流速和总体积传质系数(kLa)呈正相关,表明流型在本研究体系中对传质的影响可忽略。在相同管径通道内,停留时间与总体积传质系数呈负相关,表明在两相接触通道入口处发生了显著传质。在相同的两相混合速度和相比下,254 μm的管径传质效果是750 μm的9倍,表明小管径内传质效果更加,循环强度更大。最后将实验总体积传质系数结果与总体积传质系数的经验式进行了关联,有望为实现将微通道放大的绿色冶金技术提供理论基础。     

狭窄矩形通道内液固两相磨蚀特性

液固两相磨蚀研究主要集中于圆管弯头和射流工况,板式换热器等狭窄矩形通道内液固两相磨蚀特性的研究鲜见报道。在Fluent软件及其二次开发框架内构建了描述稀疏颗粒液固两相磨蚀特性的CFD-DPM-磨蚀耦合数学模型框架,研究了存在圆柱体阻挡物的狭窄矩形通道内两相流动特性和壁面磨蚀特性,揭示了壁面和固体颗粒的相互作用机制。研究结果表明：阻挡物的存在显著改变了狭窄矩形通道壁面的磨蚀行为;磨蚀速率随液固流速和壁面粗糙度的增加而增加,因此,保证设备较低的入口流速和壁面粗糙度对延长设备寿命至关重要;磨蚀速率随颗粒粒径的增加先增加后降低,在60μm左右时达到极大值;球形度系数对磨蚀行为影响较小。引入量纲为1颗粒尺寸,阐述了液相边界层束缚颗粒运动的作用机制;与光滑壁面工况相比,颗粒以较大能量高频撞击粗糙壁面,导致了壁面磨蚀较快。液固两相以较低的角度和速度撞击壁面,壁面材料去除机理以微切削为主。     

Numerical analysis of heat transfer mechanisms to pneumatically conveyed dense phase flow

Mass and energy balances are required in power generation, chemical, pharmaceutical, food and commodity transfer processes in order to achieve efficient utilization of energy and raw materials. There is a need for accurate, reliable, on-line, continuous and non-invasive measurement of solids' mass flow rate in many industrial processes mentioned above. Thermal flowmeters, in theory, provide a true indication of the mass flow of solids in pneumatic conveying pipelines.A complicated heat transfer between a pipe wall and a gas-solid flow in a conveying pipeline inevitably takes place in a thermal solids' mass flow measurement process. A study of heat transfer mechanisms to pneumatically conveyed gas-solid dense phase flow as a means to mass flow rate measurement has been conducted experimentally and numerically to evaluate the heat transfer coefficient between the hot wall and the gas-solid dense phase flow. The prediction of the heat transfer coefficient is compared with the experimental findings. It was found that the heat transfer coefficient between the pipe wall and the gas-solid dense flow is a function of solids loading ratio. Increasing the gas stream velocity significantly augments the heat transfer between the hot wall and the gas-solid dense phase flow.     

Velocity of isolated particles along a pipe in stratified gas–liquid flow

The average velocity of isolated grains of sand was experimentally measured in smooth stratified flow in slightly declined pipes. Isolated particles in smooth stratified flow behave similarly to isolated particles propelled by both hydraulic conveying and intermittent gas/liquid flow. In all three cases, particle velocity is linear with respect to the average liquid velocity of the flow (or the average fluid velocity in the slug body for intermittent flow) and has a gradient of approximately one. The data in stratified flow are successfully correlated dimensionlessly (Eq. 7). The correlation is extrapolated to zero particle velocity to estimate the conditions required to ensure sand transport in a flowline in smooth stratified flow. The experimental results suggest that particle velocity is strongly governed by the size of a particle relative to the depth of the viscous sublayer at the pipe wall. If a particle is larger than the viscous sublayer, it is exposed to more coherent turbulent structures and therefore experiences a greater drag.     

Mass Transport from Single Droplets in Imposed Electric Fields

Abstract

The influence of electric charge phenomena on mass transfer in systems involving droplets in a continuous medium is of increasing importance. The enhanced transport behavior of droplets in imposed fields on mass transfer and the influence of naturally occurring charges on droplets, particularly in the atmosphere, are both subjects of current interest. The objective of this study is to elucidate the hydrodynamic and mass transfer effect of imposed fields on charged single droplets. Investigations of both static and pulsed electric fields are reported.

The experimental approach is based on the suspension of single droplets in a precisely machined expanding channel. A stationary, saturated water droplet is fluidized by the upflow of 2-ethylhexanol. This arrangement allows precise photographic monitoring of droplet size and shape as well as the hydrodynamics of both phases in the region of the interface.

Baseline continuous-phase mass transfer studies with internally circulating droplets corroborate earlier studies with the same system. The effect of the accumulation of unavoidable surfactant on droplet circulation and mass transport rate at long exposure times is reported. The imposition of a static electric field in the axial direction caused distortion of droplets into prolate spheroidal shape.

An electric field pulsed at a tuned frequency is observed to cause oscillation of droplets between prolate-and oblate-spheroidal shapes. In addition to frequency and field amplitude, the interfacial properties of the fluid system as well as viscosities and densities of the two phases influence the oscillation. The effect of the pulsation of the field on mass transfer to the continuous phase is reported. These data are compared with results for both nonoscillating mass transfer and theoretical models.     

圆管内置梯形翼片的流场特性PIV实验

诱导流体产生纵向涡结构可以有效强化对流换热,因此研究纵向涡发生器的扰流特性对于深化强化传热机理具有重要意义。利用粒子成像测速(PIV)技术,对圆管内置梯形翼片扰流后的流场进行了测量,实验中4个梯形翼片沿周向均布,与管壁夹角135°呈迎流放置,分析了横、纵截面内的流场结构和流动特点。结果显示,管内放置翼片能够诱导形成多纵向涡流动,在下游产生了4个对称的涡偶,每个涡偶对应的两个涡旋转方向相反,形成了内侧向壁流,外侧背壁流的流动结构,增大了垂直于主流方向上的速度分量。实验涉及的Reynolds数范围内,翼片下游横截面内的横向速度和径向速度分别达到主流均速的27%和20%以上;纵向涡沿壁面向下游发展可对流体产生持续扰动,使近壁流体的速度相对于光滑管提升了约1.0～3.6倍;翼片对流体的扰动作用随着Reynolds数的增大而增强,对于圆管内对流换热的强化具有促进作用。     

孔板管道流动加速腐蚀受温度影响的数值模拟

电厂汽水管道的运行中,流动加速腐蚀（FAC）普遍存在且威胁着管道系统。为很好预测电厂管道流动加速腐蚀,本文基于电厂管道实际工况,采用流体动力学软件根据温度变化相应地调整水的物性参数,模拟了孔板管道下的流场,观察高速及高湍流动能分布区域,模拟计算得到不同温度下溶解度、速度、壁面剪切力及传质系数的变化,并结合流动加速腐蚀预测模型更精确地分析了温度对流动加速腐蚀的影响。结果显示：温度通过影响速度及黏性系数,进一步影响到壁面剪切力及传质系数,最终影响到FAC速率;传质系数与溶解度均受温度影响,在150℃以下,温度对FAC速率的影响显著且主要是通过传质系数实现的;FAC速率在Z/D≈0.7~1.0达到峰值,在Z/D≈3.8~4.3出现第二峰,这两处为孔板管道高危腐蚀区域。     

三相下喷式环流反应器的传质性能

在三相非牛顿型流体体系中，对下喷式环流反应器传质特性进行了实验研究。讨论了表观气速、能量耗散速率、导流筒直径与反应器直径比、喷嘴直径、导流筒下端距反应器底部的距离、固体装填量、羧甲基纤维素钠（ＣＭＣ）溶液浓度及其流变特性对它的影响。实验结果表明，容积传质系数随表观气速和能量耗散速率的增加有所增加，在实验条件下，发现最优的导流筒直径与反应器直径比在０．４～０．４５这一范围、固体装填量大约为３％（体积百分比）、导流筒下端距反应器底部的距离为０．０８ｍ左右。同时提出了容积传质系数的经验关联式。     

Limiting flux in microfiltration of colloidal suspensions by focusing on hydrodynamic forces in viscous sublayer

Cross‐flow microfiltration tests were performed on colloidal suspensions under turbulence conditions. By changing the particle diameter, flow rate, and channel height in the membrane housing to measure limiting fluxes, the influence of each parameter on the limiting flux was assessed from the viewpoint of hydrodynamic forces exerted on a particle in the viscous sublayer. In analyzing all the data taken, the particle Reynolds number calculated from the limiting flux is proportional to the 1.5 power of that calculated from the flow rate at the boundary between the viscous sublayer and the intermediate layer. This fact indicates that the limiting flux can be determined in situations where the drag force exerted by the flux is balanced by the lift force in the viscous sublayer. © 2017 American Institute of Chemical Engineers AIChE J, 64: 1760–1765, 2018     

Electrochemical mass transfer measurements in a Y‐bifurcation model

A novel technique was used to fabricate nickel flow models of a straight pipe and a Y‐bifurcation. These were used to obtain integral mass transfer coefficients by the electrochemical technique. For the straight pipe, good agreement was obtained with previously reported mass transfer correlations. The use of an upstream anode in addition to the downstream anode led to higher mass transfer at the cathode with laminar flow because of the additional near‐wall ions produced by the upstream anode. With increasing Schmidt number, the effect of transition from laminar to turbulent flow on mass transfer was delayed to progressively higher Reynolds numbers because of the reduced mass transfer boundary layer thickness relative to the viscous sublayer. With the Y‐bifurcation, possible flow separation and the formation of a new mass transfer boundary layer in the daughter branches significantly influence the mass transfer behaviour.     

CFD Study of Effects of Module Geometry on Forced Convection in a Channel with Non‐Conducting Fins and Flow Pulsation

CFD simulations were carried out to investigate the effects of the module geometry on forced convection in a rectangular channel containing series of regularly spaced non‐conducting baffles with flow oscillation. The simulations were performed at constant wall temperature. Steady‐flow Reynolds numbers Re in the range of 200 and 600 were studied. The results of the CFD simulations show that, for the effect fin spacing to be significant on heat transfer enhancement in finned system with oscillating flow, the oscillating flow velocity must be higher than the mean flow velocity. Superposition of oscillation yields increasing heat transfer performance with increasing fin height. Fin geometry with pyramidal shape yields highest performance in terms of the heat transfer effectiveness.     

UNSTEADY MAGNETOHYDRODYNAMIC NON-NEWTONIAN FLOW DUE TO NON-COAXIAL ROTATIONS OF DISK AND A FLUID AT INFINITY

An analysis is carried out to study the flow generated in a semi-infinite expanse of an incompressible second-grade fluid bounded by a porous oscillating disk. The flow is due to non-coaxial rotations of a disk and a fluid at infinity. The fluid is electrically conducting in the presence of a uniform transverse magnetic field. The solutions of the developed flow are obtained for the cases when the angular velocity is greater than, smaller than, or equal to the frequency of oscillation. The velocity field is found analytically by a Laplace transform technique. It is found that for uniform suction and blowing at the disk, shear oscillations are confined to the Ekman-Hartmann layer near the disk for all values of the frequencies.     

A qualitative computational study of mass transfer in upward bubble train flow through square and rectangular mini-channels

In this paper we present a new method for numerical simulation of conjugate mass transfer of a dilute species with resistance in both phases and an arbitrary equilibrium distribution coefficient. The method is based on the volume-of-fluid technique and accounts for the concentration jump at the interface by transforming the discontinuous physical concentration field into a continuous numerical one. The method is validated by several test problems and is used to investigate the mass transfer in upward bubble train flow within square and rectangular channels. Computations are performed for a single flow unit cell and a channel hydraulic diameter of 2 mm. The simulations consider the transfer of a dilute species from the dispersed gas into the continuous liquid phase. Optionally, the mass transfer is accompanied by a first-order homogeneous chemical reaction in the liquid phase or a first-order heterogeneous reaction at the channel walls. The results of this numerical study are qualitative in nature. First, because periodic boundary conditions in axial direction are not only used for the velocity field but also for the concentration field and second, because the species diffusivity in the liquid phase is arbitrarily increased so that the liquid phase Schmidt number is 0.8 and the thickness of the concentration and momentum boundary layer is similar. Two different equilibrium distribution coefficients are considered, one where the mass transfer is from high to low concentration, and one where it is vice versa. The numerical study focuses on the influence of the unit cell length, liquid slug length and channel aspect ratio on mass transfer. It is found that for the exposure times investigated the liquid film between the bubble and the wall is saturated and the mass transfer occurs by the major part through the bubble front and rear so that short unit cells are more efficient for mass transfer. Similar observations are made for the homogeneous reaction and for the heterogeneous reaction when the reaction is slow. In case of a fast heterogeneous reaction and when the main resistance to mass transfer is in the gas phase, it appears that for square channels long unit cells are more efficient, while large aspect ratio rectangular channels are more efficient than square channels, suggesting that for these conditions they might be more appropriate for use in monolithic catalysts.