首页 | 本学科首页   官方微博 | 高级检索  
     

变径组合提升管内压力脉动及其流型转变特性
引用本文:谢金朋,吴广恒,王德武,刘燕,张少峰. 变径组合提升管内压力脉动及其流型转变特性[J]. 石油学报(石油加工), 2019, 35(1): 83-90. DOI: 10.3969/j.issn.1001-8719.2019.01.011
作者姓名:谢金朋  吴广恒  王德武  刘燕  张少峰
作者单位:1. 河北工业大学 化工学院, 天津 300130;2. 天津职业大学 生物与环境工程学院,天津 300410
基金项目:河北省自然科学基金项目(B2017202185)和天津职业大学研究基金项目(20171102)资助
摘    要:采用变径组合提升管冷模实验装置,在固/气比(Gs/(ρg·Ug))为0~37.60,通过实验对变径组合提升管内的压力脉动信号及其流型转变特性进行了研究。结果表明,随着固/气比(Gs/(ρg·Ug)的增加,变径组合提升管内依次出现气力输送(Gs/(ρg·Ug)为0~15.00)、快速流态化(Gs/(ρg·Ug)为15.00~27.00)、高密度循环流态化(Gs/(ρg·Ug)为2700~3760)3种流型。变径组合提升管内压力脉动主要由两部分组成:一部分是由于进料波动产生的全局性压力脉动,主频在0.30 Hz左右;另一部分是由于局部气流扰动,气-固相互作用以及颗粒(团)和颗粒(团)之间的相互作用引起的局部压力脉动。气力输送流型下,局部压力脉动的频率主要集中在D5频段(1.56~3.13 Hz),主要由局部气流扰动引起;快速流态化流型下,局部压力脉动的频率主要集中在D4频段(3.13~6.25 Hz),主要由局部气体与颗粒(团)间的作用引起;高密度循环流态化流型下,局部压力脉动的频率主要集中在D5频段,主要由局部颗粒(团)与颗粒(团)间的作用引起。

关 键 词:循环流化床  变径提升管  压力脉动  小波分析  流型转变  
收稿时间:2018-02-02

Characteristics of Pressure Fluctuation in Adjustable Combined Riser and Flow Regime Transition
XIE Jinpeng,WU Guangheng,WANG Dewu,LIU Yan,ZHANG Shaofeng. Characteristics of Pressure Fluctuation in Adjustable Combined Riser and Flow Regime Transition[J]. Acta Petrolei Sinica (Petroleum Processing Section), 2019, 35(1): 83-90. DOI: 10.3969/j.issn.1001-8719.2019.01.011
Authors:XIE Jinpeng  WU Guangheng  WANG Dewu  LIU Yan  ZHANG Shaofeng
Affiliation:1. College of Chemical Engineering, Hebei University of Technology, Tianjin 300130, China;2. College of Biological and Environmental Engineering, Tianjin Vocational Institute, Tianjin 300410, China
Abstract:With using an adjustable combined riser cold model experiment device and solid-gas ratio (Gs/(ρg·Ug)) ranging from 0 to 37.60, characteristics of both pressure fluctuation and flow regime transition were studied. Study results suggested that there were three kinds of flow regime in the riser, i.e, pneumatic conveying  (Gs/(ρg·Ug) 0-15.00), fast fluidization  (Gs/(ρg·Ug) 15.00-27.00), high-density circulating fluidization  (Gs/(ρg·Ug) 27.00-37.60). Pressure fluctuation in the adjustable combined riser is mainly composed of two parts: one is the global fluctuation caused by feed fluctuation, which is about 0.30 Hz at the main frequency; the other is local fluctuation caused by local air turbulence, gas solid interaction and clusters interaction. In the pneumatic conveying regime, the main frequency of local pressure fluctuation caused by the local air turbulence is concentrated in D5 (1.56-3.13 Hz) frequency. In the fast fluidization regime, the main frequency of local pressure fluctuation caused by the interaction between the local gas and particles (clusters) is concentrated in D4 (3.13-6.25 Hz) frequency. In the high-density circulating fluidization, the local pressure fluctuation caused by clusters interaction is concentrated in D5 frequency.
Keywords:circulating fluidized bed  adjustable riser  pressure fluctuation  wavelet analysis  flow regime transition  
本文献已被 CNKI 等数据库收录!
点击此处可从《石油学报(石油加工)》浏览原始摘要信息
点击此处可从《石油学报(石油加工)》下载全文
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号