低密度循环流化床反应器床层截面平均颗粒速度的变化规律

本文在高8m,内径186mm 的循环流化床中采用 FCC 颗粒,利用 TSI 光纤激光多普勒测速仪测定了局部颗粒速度的径向分布,并获得了床层截面平均颗粒速度。实验结果表明:截面平均颗粒速度随操作气速的增大而增大,随固体循环速率的增大而略有减小。由实验数据回归得到了计算本实验条件下低密度速度的经验关联式。论文还从基本流体力学理论出发,在考虑颗粒加速运动的条件下,建立了一维气、固两相流模型,可以用于预测床层截面平均颗粒速度和空隙率的变化规律,模型计算结果和实验数据吻合较好。     

循环流化床提升管中颗粒速度的径向分布及其沿轴向的发展

采用5光纤速度探头对f100mm?5.1m循环床提升管8个高度截面上11个径向位置的局部颗粒速度进行了实验测试,并采用径向不均匀指数(RNI)对颗粒速度径向分布的不均匀性及其沿轴向的变化进行了定量描述。研究结果表明:在高气速、高颗粒循环量操作时,操作条件对颗粒上升速度和下降速度的径向分布的影响在加速段和充分发展段呈现出不同的规律;颗粒上升速度和下降速度沿轴向的变化在核心区和边壁区也表现出不同的趋势。当颗粒循环速率大于200 kgm-2s-1时,颗粒的加速段长度大大延长,以至于大于提升管的高度(15.1m)。颗粒速度径向分布的不均匀性沿轴向是逐渐增大的,并且与截面平均颗粒速度存在很强的相关性。     

新型液固循环床提升管颗粒速度径向分布的实验研究

新型液-固循环流化床与常规液-固循环流化床的区别在于提升管底部入口结构和顶部出口结构的不同.实验装置为φ80×8000 mm有机玻璃床,新结构可在较高表观液速和较高颗粒循环速率下操作.利用光纤速度测量仪测量床内颗粒速度径向分布,得到了颗粒速度径向分布规律.通过对实验结果分析发现,新型循环流化床颗粒速度径向分布与较高的表观液速和颗粒循环速率以及由此引发的较大的边壁效应密切相关.     

快速流化床中颗粒浓度及颗粒速度的径向分布

本文在φ140mm的气固并流下行快速流化床中,研究了颗粒浓度及颗粒速度的径向分布随操作气速、颗粒循环速率以及床层轴向位置的变化规律。并探讨了颗粒质量通量的径向分布及颗粒流动的均匀性,表明在相同操作条件下,下行快速流化床中气固流动远比上行快速流化床均匀。     

液固循环流化床中的颗粒速度场

利用超声多普勒测速仪（UDV）对液固循环流化床中颗粒流场进行了系统的实验研究.实验测定了不同轴向位置处的颗粒速度分布,得到了较完整的颗粒速度场,分析了入口区对流场分布的影响,考察了表观液速和颗粒循环速率等操作条件对颗粒速度场分布特点的影响,并利用各影响因素之间的相互关系对流型和速度的变化进行了分析.     

气固逆流下行流化床中颗粒速度的径向与轴向分布

在内径90 mm、高7 m的逆流下行床冷态实验装置中,研究了气固逆流下行床中循环锅炉灰(dp=300 mm)颗粒速度的径向分布及其沿轴向发展. 结果表明,局部颗粒速度沿径向分布是不均匀的,在完全发展区,颗粒速度中心和边壁低、在r/R=0.85附近颗粒速度最大. 由大量实验数据回归出预测充分发展段局部颗粒速度的关联式,该公式计算值与实验值的平均相对偏差小于±11%. 不同径向位置的局部颗粒速度沿轴向的变化趋势不同,边壁区域(r/R>0.622)颗粒速度沿轴向单调递增,而中心区域(0相似文献   

气液固三相流化床局部相含率轴径向分布

应用开发的微电导探针测试技术,对小尺寸颗粒玻璃珠（粒径分别为0.48、0.80、1.25 mm）和1.45 mm苯乙烯树脂为固相,空气和水分别为气相和液相的三相流化床的各相局部含率进行了同时测定.在较宽操作条件下,获得了一系列局部相含率实验数据.通过对实验数据研究发现：在充分发展段,局部固含率在r/R=0.75～0.85范围内有一个极大值,床层截面平均气含率随表观液速的变化存在一个极小值.在气体分布器区,在距气体分布器轴向一定距离范围内,三相局部含率的径向分布存在明显的不对称分布.随着轴向距离的增加,局部气含率径向不对称分布逐渐消失,最终过渡到对称分布,而局部固含率的径向不对称分布消失得不明显.     

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     

循环流化床提升管中固体颗粒停留时间的分布

在内径１４０ｍｍ，高１０ｍ的循环流化床提升管中，采用磷光颗粒示踪法对床内固体颗粒的停留时间分布进行了测定。在气速１．５～９．０ｍ／ｓ，固体循环量１０～１４０ｋｇ／ｍ２ｓ的范围内，实验测得的停留时间分布曲线均有明显的双峰分布。这种双峰分布是由于提升管中弥散颗粒和颗粒团共同作用的结果。本文提出的一维两组分扩散叠加模型可较好地描述提升管中固体的混合行为。考察了在实验条件下，操作条件对固体混合行为的影响。发现：气速及固含对颗粒的轴向Ｐｅｃｌｅｔ数影响不大，提升管中颗粒的返混主要是由于颗粒团引起的。将研究结果与近期文献报道的其他研究进行了对比     

提升管循环流化床气,固局部滑落速度的分布

本研究采用光纤激光多普勒测速仪（ＬＤＶ），通过两列信号处理系统，同时测定了气体和颗粒局部速度，研究了低密度循环流化床提升管内局部滑落速度的变化规律。实验结果表明，提高颗粒循环速率，在任一径向位置的气固滑落速度均增加；提高气体表观速度，反而使气固之间局部滑落速度减小。由于固体颗粒在近壁区的团聚行为，在近壁区气、固局部滑落速度出现一个极大值。     

Solid Recycle Characteristics of Loop‐seals in a Circulating Fluidized Bed

Solid recycle characteristics through a conventional and a newly developed loop‐seal (0.08 m i.d.) system are determined in a circulating fluidized bed of FCC or silica sand particles. In the loop‐seal developed here, gas was injected downward tangentially to the wall of the loop‐seal to increase solids mass flux with stable flow. For conventional loop‐seal, solids mass fluxes increase linearly with increasing aeration rate but it reaches a maximum value. At the same aeration rate with different aeration locations (0.1 – 0.6 m) in a conventional loop‐seal, a maximum solids mass flux is seen at a height to diameter ratio of 2.5. For the newly developed loop‐seal, mass fluxes of FCC and sand particles are higher and more stable than in conventional loop‐seal at the same aeration rate. The solid mass fluxes obtained have been correlated with the aeration rate and Archimedes number.     

气固固循环流化床密相床层压力脉动研究

在不同实验条件下研究了气固固循环流化床密相床层的压力脉动。压力脉动的情况表明：细颗粒的循环及循环量对粗颗粒的流体力学行为有很大影响。气速越低,影响程度越大。     

循环流化床锅炉水冷壁防磨技术研究与应用

循环流化床锅炉炉内受高浓度床料冲刷、磨损影响,水冷壁管壁厚减薄,泄漏或爆管事件频繁发生。防磨梁技术是目前循环流化床锅炉采取的一种主动防磨措施,保证锅炉长周期安全稳定运行,同时延长了炉内喷涂防磨周期,综合效益突出。     

循环流化床气体返混及停留时间的分布

本文采用脉冲示踪技术,研究了直径140 mm循环流化床内气体的返混特性及其停留时间分布规律,并通过一维轴向扩散模型,得到了气体轴向扩散系数。实验结果表明,在循环流态化条件下,气体轴向流动明显偏离于平推流,并且随操作气速增大或颗粒循环速率的减小,气体轴向返混程度减小。     

Drying Kinetics in the Riser of Circulating Fluidized Bed with Internals

Solid particles were dried in the riser of circulating fluidized bed with internals to study the drying kinetics. Experiments were conducted in a circulating fluidized bed, having perforated plates as internals covering wide range in the operating parameters. The effects of various operating parameters, i.e., initial moisture content, temperature, and flow rate, of the heating medium and solid circulation rate on the rate of drying have been critically examined. It has been observed from the present investigation that the presence of internals enhances the solids holdup in the riser of circulating fluidized bed. The drying efficiency of a circulating fluidized bed with internals has been compared with the drying performance of a circulating fluidized bed without internals under the same operating conditions.     

Cotton Stalk Combustion in a Circulating Fluidized Bed

The basic properties of cotton stalk (CS) of length 10–100 mm and its ash were investigated. Studies concerning the combustion characteristics of CS were performed in a circulating fluidized bed (CFB) test facility with a heat input of 0.5 MW. According to previous cold tests, there is very little segregation during the mixing of CS with this size profile and bed material at a fluidization number of N > 7, but the hot experimental results indicate that slight segregation has a small effect on the steady combustion of the dense region. Experiments were carried out with the aim of investigating the effects of operating conditions on the axial temperature and gas concentration profiles along the combustor height, as well as the emission performance and combustion efficiency of the CFB. The experimental results indicate it is difficult to react alumina bed material with alkali metals from CS ash following 26 h of combustion. The overall conclusions appear to indicate that the application of circulating fluidized bed boilers to fire pure CS of length 10–100 mm, is feasible.     

Drying Kinetics in the Riser of Circulating Fluidized Bed with Internals

Solid particles were dried in the riser of circulating fluidized bed with internals to study the drying kinetics. Experiments were conducted in a circulating fluidized bed, having perforated plates as internals covering wide range in the operating parameters. The effects of various operating parameters, i.e., initial moisture content, temperature, and flow rate, of the heating medium and solid circulation rate on the rate of drying have been critically examined. It has been observed from the present investigation that the presence of internals enhances the solids holdup in the riser of circulating fluidized bed. The drying efficiency of a circulating fluidized bed with internals has been compared with the drying performance of a circulating fluidized bed without internals under the same operating conditions.     

Fluidization Characteristics of Circulating Fluidized Bed Boilers

The fluidization in the furnace of circulating fluidized bed (CFB) boilers is described. Data have been obtained from a 12 MW_th CFB boiler and from literature. The bottom bed is bubbling rather than fast or turbulently fluidized as is often assumed. There is an extended splash zone above this bed, in which particles are thrown up by the bubbles and fall back onto the bottom bed. Other particles are carried further into the transport zone, initially as a saturated gas flow, but some particles move into the wall layers and the density decays towards the exit. The density of the transport zone is low, and the circulation rate is relatively seen small. Therefore, this flow is in a state of dilute-phase transport and not in the fast fluidization regime, such as is often claimed.     

Design Parameters for Performing Circulating Turbulent Fluidization with a Single Feed Stage Fluidized Bed Reactor

A fluidization reactor was designed to study the possibility of performing circulating turbulent fluidized bed (CTFB) by using only single feed gas injection. The effect of the design parameters was studied based on the Geldart classification and Archimedes number. Two sizes of sand particles represented Geldart group B, whereas a polyvinyl chloride particle represented the Geldart group A. The effect of the operating parameters was studied by manipulating the solid recirculation rates. Interpretation of the solid fraction profile along riser height could be used to determine the bed front. The appearance of CTFB in the system was indicated by the disappearance of the bed front along the riser height. A suitable riser height was lower than the maximum solid particle bed expansion; this is a crucial design parameter to support the action of CTFB.