共查询到19条相似文献,搜索用时 187 毫秒
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高温鼓泡流化床的压力波动 总被引:3,自引:0,他引:3
在内径82mm,高1500mm的不锈钢流化床中,采用4种不同粒径加压流化床灰为实验物料,通过统计分析,功率谱分析和小波分析研究了流化床操作温度由室温至1000℃变化时压力波动行为。研究显示,灰在不同温度下随着流化数增加压力波动偏差增大。B类颗粒,流化数相同时,床层温度升高,压力波动标准偏差减小不明显。D类灰,当流化数相同时,床层温度升高使得压力波动标准偏差减小。在同样的温度下,随着流化数的增加,主频减小。高温鼓泡流化床压力波动信号包含低频成份和高频分份,高频成份较小。压力信号通过离散小皮变换可分解为5尺度的近似信号和1到5尺度的细节信号,5尺度细节信号图上幅值大于平均幅值的尖峰数代表了气泡生成数。 相似文献
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高温流化床的流化特性及结焦非流化行为 总被引:3,自引:0,他引:3
在 8 0 mm× 30 mm和 80 mm× 10 mm石英流化床中 ,以低温粘结的高密度聚乙烯和聚丙烯 ,高温粘结的玻璃珠为实验物料 ,研究了高温流化床的流化特性及高温下物料结焦产生的非流化行为。结果表明 ,在本文实验条件下 ,Geldart A、B类高温表面粘结物料 ,床层温度小于其最小粘结温度时 ,床层温度增大 ,颗粒的最小流化速度减小 ;Geldart D类高温表面粘结物料的最小流化速度随温度增加而增大。得出了不同温度下颗粒最小流化速度预测式。床层温度大于最小粘结温度时 ,流化床需在较高的表观气速下才能保持流化 ,床层温度愈高床层流化所需的表观气速越大。研究同时发现 ,颗粒物料的粒径减小 ,流化颗粒的最小粘结温度减小。 相似文献
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在自行搭建的双循环流化床冷态实验系统上研究了鼓泡床静床层高度、颗粒平均粒径、鼓泡床流化风速、快速床总流化风速及一次风量比例等控制参数对颗粒循环流率的影响,提出了基于上述控制参数的颗粒循环流率计算关联式。结果表明:随着鼓泡床流化风速的增加,颗粒循环流率变化不明显;随着快速床中一次风量比例和总流化风速的增加,颗粒循环流率均增大,当一次风量比例和总流化风速达到一定值后,颗粒循环流率的增幅逐渐变缓;颗粒循环流率随着静床层高度的增加而增大,随颗粒平均粒径的增大而减小,且颗粒平均粒径的影响程度较大;所提出的关联式能够较好地预测颗粒循环流率。 相似文献
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循环流化床(CFB)锅炉炉内的燃烧及传热与炉内床料的状态密切相关,而炉内床料主要是由燃煤含有的矿物组分经过燃烧、爆裂和磨耗过程形成的。文中对6种煤样在固定床燃烧后,使用可视化显微仪,获取了灰颗粒的微观形貌特征,根据灰颗粒的机械强度和耐磨性能的不同,将灰颗粒定义为3类不同性质的灰。以此为基点,采用固定床燃烧后冷态振动筛分和流化床实验台热态流化后筛分的方法,研究了不同燃烧温度下升温速率对灰颗粒粒径变化的影响,以及不同燃烧温度下燃烧时间对灰颗粒粒径变化的影响,推演了不同煤样在燃烧过程中的演化特征。结果表明:3类灰颗粒在不同的燃烧温度和时间的演化过程存在明显的不同,从而为预测循环流化床中的床料粒径分布提供了理论依据。 相似文献
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利用X射线荧光光谱仪、灰熔点仪和热重分析仪等对酒糟的灰成分、灰熔点及着火温度进行了测试,并在小型流化床试验台上进行了酒糟燃烧试验,对不同含水率酒糟的着火特性、烧结特性和NOx排放质量浓度进行了研究.结果表明:酒糟灰中K2O和Na2O的含量很低,只有4.936%;酒糟灰的软化温度较高,高于1 290℃;干燥酒糟的挥发分较高,高于250℃就能够着火燃烧;当石英砂的平均粒径为300μm、流化床内的流化速度大于0.36m/s时,流化状况良好;在900℃下,酒糟在石英砂流化床中燃烧不会出现烧结现象;在不同的燃烧温度下,NOx排放质量浓度均较大,且随着燃烧温度的升高而增大;酒糟可以在石英砂流化床中燃烧,且燃尽效果良好. 相似文献
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P. Ammendola R. Chirone G. Ruoppolo G. Russo R. Solimene 《International Journal of Hydrogen Energy》2008
This paper reports a model of fluidized bed thermo-catalytic decomposition (TCD) of methane. The novelty of the model consists of taking into account the occurrence of different competitive phenomena: methane catalytic decomposition, catalyst deactivation due to carbon deposition on the catalyst particles and their reactivation by means of carbon attrition. Comparison between theoretical and experimental data shows the capability of the present model to predict methane conversion and deactivation time during the process. The model demonstrates to be also a useful tool to investigate the role played by operative parameters such as fluidizing gas velocity, temperature, size and type of the catalyst. In particular, the model results have been finalized to characterize the attrition phenomena as a novel strategy in catalyst regeneration. 相似文献
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以410 t/hCFB锅炉为研究对象,在分析"选择性流化床冷渣器-炉膛"系统压力分布特性的基础上,研究了压力分布特性对该种冷渣器物料流动及物料量的影响规律.结果发现:"冷渣器-炉膛"系统的压力分布特性对冷渣器物料平衡有重要影响.在稳定运行时,选择室的床层压降都小于另外3室,即选择室的床料量(或炉渣量)会小于其它3室;由于排渣的作用,冷渣器排渣室的床料量略少于中间2个冷却室;随着炉膛或冷渣器流化风速的增大,冷渣器内的床料量都将降低;炉膛和选择性流化床冷渣器之间是一种复杂的串并联关系,这使炉膛与冷渣器各室之间的气固流动参数相互制约,底渣流动的可控性较差. 相似文献
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A mathematical model has been developed to describe the agglomeration process in bio-fuel fired fluidized bed combustor. Based on the balance mechanism of the adhesive force caused by liquid bonding between two parti- cles and the breaking force induced by bubbles in the fiuidized bed, the model considers modified Urbain model and chemical equilibrium calculations using FactSage modeling. This model prediction accounts for the evolve- ment of the adhesive and breaking forces, and clearly demonstrates that the different composition of ash, the in- creasing liquid phase matter and the fiuidization velocity cause defluidization in fluidized bed. In this model, it is the first time to hypothesize that the bonding stress between two particles is proportional to mass fraction of liq- uid phase and inversely proportional to the diameter of particles and viscosity of liquid phase. The defluidization time calculated by this model shows good agreement with that from the experimental data. 相似文献
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Combustion of isolated bubbles was investigated with a laboratory-scale fluidized-bed reactor. Two different combinations of oxygen and argon were employed as the fluidizing gas. Single bubbles of methane were injected into an incipiently fluidized bed maintained at elevated temperatures. Gas composition inside the bubbles was measured using a suction probe connected to an on-line mass spectrometer, and the temperature of the bubbles was monitored using a fast-response thermocouple. The effects of bed particle type, particle size, bubble size, bed temperature, and oxygen concentration in the emulsion phase were examined for bed temperatures between 923 and 1203 K. A theoretical model of homogeneous combustion within the bubble phase was developed for comparison to the experimental results. The model accounted for the heat and mass transfer between bubble and emulsion phases, but only considered combustion within the bubble. The results indicated that small bubble size and high oxygen concentrations in the emulsion phase enhanced bubble-phase combustion. The bed temperature also proved to be an important parameter, with higher temperatures promoting bubble combustion, but unlike some other investigations, no critical ignition temperatures were observed in either experiments or model results. The fluidized bed's particle size and particle composition influence the heat and mass-transfer coefficients, and therefore the bubble-phase combustion, but these have a smaller influence than bed temperature and bubble size. Model results for bubble-phase gas composition and temperature compared favorably with the experimental measurements. 相似文献
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全面分析了目前运行的大型循环流化床热水锅炉存在的问题,提出了采用塔式布置、多床复合、低流化风速、低循环倍率、低温气固分离等技术措施来实现循环流化床热水锅炉大型化的技术思想,并介绍了据此开发大型复合床式低倍率循环流化床热水锅炉的技术原理和结构特点。 相似文献