三相循环流化床中气泡上升速度的实验研究

开发了一种新型的光纤探头多相流气泡测试系统,可用于气－液两相和气－液－固三相体系中气泡参数的测定。应用此系统研究了三相循环流环化床中不同径同位置气泡的上升速度分布,气泡上升速度均值的径向布以及操作条件对这现任中分布的影响。     

三相循环流化床中沸腾传热特性

提出了一种新型蒸发沸腾传热方式,即汽液固三相循环流化床沸腾传热。实验表明:该传热方式具有强化传热和防、除垢效果;其传热系数比汽液两相流沸腾传热膜系数高1.5～2.0倍,并能长期保持传热壁面的洁净。实验中研究了不同种类的固体粒子(玻璃球、陶瓷球、钛粒和钢球)、粒子体积分率、液相流速以及加热蒸汽压力等因素对循环流化床沸腾传热的影响。     

三相循环流化床中的气液相界面积和传质系数

采用溶氧法测量了三相循环流化床中液相溶氧浓度的轴向分布,并按轴向扩散模型处理实验数据,优化得到气液体积传质系数kLa,同时用光纤探头测量了体系中的气含率和气泡大小分布,计算得到了气液相界面积a和气液传质系数kL,并研究了主要操作条件(表观气速、表观液速和固含率)对气液传质系数的影响规律.     

喷射环流三相流化床反应器轴向液速分布的研究

在喷射环流三相流化床反应器中，应用本文所开发的内热式热膜流体速率探头，获得了带有沉降分离区的夹套式环流反应器在不同压力、气量、流量条件下，不同轴向位置的液体速率分布规律。对于本文所述这类反应器，喷射区流体运动速率最大；自喷口向上，速率先是随距离的增大易急骤下降，然后逐渐向一渐近点逼近；当进入环隙转折口处时，由于气体的逸出及流道的变化液速急骤下降；凝固相进入环隙时，液速随距离的变化也存在渐近点。当采用变径结构时，流道面积突变处的液速变化率仅次于喷射入口区。在环流反应器中，液速主要取决于喷射动能及气提推动力，受液体进料量及压力的影响较小。     

气液固循环流化床颗粒分布板实验研究

设计了用于气液固三相循环流化床换热器的固体颗粒分布板。采用功能强大的CCD图像采集分析系统,获得颗粒的分布和运动规律,考察了安装高度、运行参数等对分布板颗粒分布性能的影响。研究表明,分布板的安装高度、液体和气体流量、颗粒体积分数等对颗粒的速度和固含率分布有较大影响,得到了使固体颗粒在管束中分布效果较好的设计参数,以指导工程应用。     

二维三相循环流化床液体停留时间分布的研究

用脉冲示踪法对二维三相循环流化床液体停留时间分布(RTD)进行了测定。在气速2～3m／s,液体循环量0～0．35m^3／h,固体循环量1．5～1．75g／s的范围内测得的液体停留时间分布曲线均有明显的3峰分布。其中前两峰分布是由于提升管中颗粒与液体之间和液体与气体之间共同作用改变了液体轴向速度分散程度的结果。第三个峰的分布是由于液体进入循环仓循环后在出口处检测的RTD曲线,并且提出一维两组分扩散物理叠加模型,模型的预测结果与实验获锝的RTD曲线平均误差小于5％,可较好地描述提升管中液体停留时间分布曲线。     

液固循环流化床换热器中液相流场分布的测量

本文利用光电转换（CCD）技术对二维液固循环流化床中流体的速度分布进行了测定。实验结果表明：流化床的进口段前的管线结构对液体在流化床中的流场的影响,液体循环流量较小时,流体在流化床进口段的速度分布基本均匀,此时在床的对称轴两侧形成两个漩涡,且近似对称,流化床中的固含率在实验范围内对流场的影响不大。     

气液固三相循环流化床中气固相含率轴径向的分布

对气液固三相循环流化床中气固相含率沿轴径向的分布进行了实验研究和模拟。实验结果表明：与膨胀床相比，三相循环流化床内的相间接触较为充分；固含率轴向分布的一维沉降－扩散模型模拟值与实验值吻合较好。     

气液固三相循环流化床气液传质行为

<正>气液固三相流化床反应器在石油化工、湿法冶金、环境工程和煤的液化等工业领域得到了广泛应用,其基础研究也取得了很大进展.但是,传统三相床主要应用于低液速(U_L<     

汽液固三相循环流化床蒸发器强化传热和防垢研究

本文在已开发的汽液固三相循环流化床蒸发器装置上进行了条件试验研究。试验表明,这种新型的蒸发器具有明显的强化传热和防垢效果,其传热系数比汽液两相流沸腾传热膜系数提高１．５倍￣２．０倍,并能有效防止污垢的产生。文中对强化传热和防垢的机理进行了探讨。     

热示踪法测量循环流化床中颗粒循环速度

通过颗粒示踪和热示踪两种方法对鼓泡循环流化床中的颗粒循环速度进行了实验研究。实验结果表明：热示踪方法和颗粒示踪方法测量鼓泡循环流化床的移动床中颗粒循环速度在一定范围内是一致的。但热示踪方法还存在一定的局限性,还需要进一步从理论和实验上完善     

循环流化床燃烧数学模型及试验研究

利用循环流化床内气－固两相流动基础方面的研究成果, 提出床内气固浓－淡流动模型, 建立适用不同结构参数的循环流化床燃烧模型, 考虑了床内气体、固体颗粒的返混、循环过程以及煤燃烧、污染气体的生成和分解、颗粒磨损等过程． 在循环流化床燃烧试验台上进行实验研究, 模型仿真结果和实验数据吻合良好, 表明气固两相浓－淡流动模型所建立的循环流动床燃烧系统模型可以正确地模拟循环流化床的燃烧过程．     

液-固流化床中单个变形气泡的上升速度

以气泡在上升运动过程中的受力分析为基础,建立了描述单个变形气泡在液－固流化床中上升速度的理论模。应用该模型分别对球形和球帽形气泡在液－固流化床中的上升速度进行了计算,并将计算民在不同的床内压力,温度与颗粒相体积分数下气泡上升速度的实验测量数据进行了比较。     

循环流化床下行管内气固两相流流体力学模型与数值模拟

从流体力学和湍流理论出发，将ｋ－ε模型运用到气固两相流动体系中，建立了气固两相湍流模型。模型计算得出的轴径向颗粒浓度及速度与实测值相吻合，为下行管的设计放大提供了理论依据。     

三相循环流化床蒸发器防除垢机理

引　言结垢是蒸发器加热壁面上经常遇到的问题 .垢层严重地降低了换热效率 ,使传热过程迅速恶化 ,蒸发器的防、除垢问题受到人们的普遍重视 .张利斌、李修伦等[1] 研究了汽液固三相循环流化床蒸发器沸腾传热和防、除垢性能 ,本文进一步考察该蒸发器的防、除垢机理 ,并对其进行了分析 .1　汽液固三相流剪应力“混相流”模型根据文献 [1],蒸发管内的汽液固三相流动呈现“混相流”的特性 ,因此为便于分析及突出问题的基本特征 ,假设 :(1)温度场引起的物性变化忽略不计 ;(2 )蒸发管内的汽液两相流动视为均相流动 ,蒸汽的惟一效果是改变了“流体…     

BUBBLE MOTION IN A THREE-PHASE LIQUID FLUIDIZED BED

This paper presents results for the rise velocities of air bubbles in liquids and liquid-solid fluidized beds. The bubble sizes ranged from approximately 0.03 to 0.45 cm radius. Tap water and distilled water were used as the fluidizing liquids. The solid phase consisted of low density alginate gel beads of mean radius 0.04 cm. The gel beads were translucent which permitted observation of bubbles inside the bed even at large solids volume fractions. Experiments were conducted for solids volume fractions ranging from 15% to 52% and in clear liquids. The goal of the experiments was to determine rise velocities of bubbles and to develop and evaluate correlations of bubble rise velocity based on bubble size, solids volume fraction and liquid properties. It was determined that, for moderate solids fractions (ranging from 28% to 45% solids), a semi-empirical correlation that treated the fluidized bed as a pure liquid with a higher viscosity than the liquid phase could be used to represent the data. The Thomas effective viscosity model was used to predict the viscosity. Provided that one restricts attention to a water fluidized bed, a second empirical correlation can be used to represent the data over a broader range of solids fractions.     

AN EXPERIMENTAL STUDY OF LIQUID-PARTICLE FLOW IN CIRCULATING FLUIDIZED BED

A liquid-solid circulating fluidized bed (LSCFB) is operated at high liquid velocity, where particle entrainment is highly significant and between the conventional liquid fluidized bed and the dilute phase liquid transport regimes. LSCFB has potential applications in the fields of food processing, biochemical processing, and petrochemical and metallurgical processing. It is well known that the flow characteristics in a liquid-solid circulating fluidized bed are different from those of a conventional liquid-solid fluidized bed. The limited studies available in literature do not provide complete understanding of the flow structure in this typical regime.

In the present work, experiments were carried out in a 0.0762 m ID and 3 m height laboratory-scale liquid-solid circulating fluidized bed apparatus by using various solid particles and tap water as fluidizing medium. In the experimental setup, two distributors (specially designed) were used to monitor solid circulation rate in the riser. The effects of operating parameters, i.e., primary liquid flow rate in the riser (Up), solid circulation rate (G_s), and particle diameter (dp), were analyzed from the experimental data. Finally, a correlation was developed from the experimental data to estimate average solid holdup in the riser, and it was compared with present experimental and available data in the literature. They agree well with a maximum root-mean-square deviation of 7.83%.     

EFFECTS OF SECONDARY AIR INJECTION ON GAS-SOLID FLOW BEHAVIOR IN CIRCULATING FLUIDIZED BEDS

Effects of secondary air injection on the hydrodynamics such as solid holdup and gas-solid flow behavior were investigated in a circulating fluidized bed. The gas velocity in the riser, the ratio of secondary air velocity to that of primary air, and the solid circulating rate were chosen as operating variables. Fluid cracking catalyst(FCC) with a density of 1840 kg/m³ and a mean diameter of 74 um was employed as the solid phase. The secondary air was fed to the riser radially or tangentially at the wall of the column. Pressure drop fluctuations in the riser were measured and analyzed by adopting the stochastic method to characterize the effects of secondary air injection on the gas-solid flow behavior in the bed.

It has been found that the injection of secondary air into the riser can increase the solid holdup in the riser considerably, and that the tangential injection of secondary air is more effective for the increasing the solid holdup than the radial injection. However, the gas-solid flow behavior has been found to become less persistent with the injection of secondary air; the resultant flow behavior is more complex when the air is injected tangentially than radially. The solid holdups in the primary as well as secondary zones of the riser have been well correlated in terms of not only operating variables but also fractal dimension of the pressure fluctuations.