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倾斜圆管内空泡份额径向分布及形成机制

刘国强 孙立成 阎昌琪 田道贵

刘国强, 孙立成, 阎昌琪, 田道贵. 倾斜圆管内空泡份额径向分布及形成机制[J]. 航空动力学报, 2014, (6): 1346-1351. doi: 10.13224/j.cnki.jasp.2014.06.012
引用本文: 刘国强, 孙立成, 阎昌琪, 田道贵. 倾斜圆管内空泡份额径向分布及形成机制[J]. 航空动力学报, 2014, (6): 1346-1351. doi: 10.13224/j.cnki.jasp.2014.06.012
LIU Guo-qiang, SUN Li-cheng, YAN Chang-qi, TIAN Dao-gui. Radial distribution and formation mechanism of thevoid fraction in an inclined circular tube[J]. Journal of Aerospace Power, 2014, (6): 1346-1351. doi: 10.13224/j.cnki.jasp.2014.06.012
Citation: LIU Guo-qiang, SUN Li-cheng, YAN Chang-qi, TIAN Dao-gui. Radial distribution and formation mechanism of thevoid fraction in an inclined circular tube[J]. Journal of Aerospace Power, 2014, (6): 1346-1351. doi: 10.13224/j.cnki.jasp.2014.06.012

倾斜圆管内空泡份额径向分布及形成机制

doi: 10.13224/j.cnki.jasp.2014.06.012
基金项目: 

国家自然科学基金(51076034,51376052);中央高校基本科研专项资助(HEUCFZ1122);黑龙江省博士后启动基金

详细信息
    作者简介:

    刘国强(1987- ),男,内蒙古赤峰人,硕士生,主要从事气液两相流动方面的研究.

  • 中图分类号: V232.8;TL334

Radial distribution and formation mechanism of thevoid fraction in an inclined circular tube

  • 摘要: 采用光纤探针测量方法,对倾斜圆管中气液两相流动的空泡径向分布特性进行了实验研究,并对其形成原因进行了分析.实验选用有机玻璃圆管内径为50mm,竖直倾斜角度为5°,15°和30°,液相折算速度为0.071~0.284m/s,气相折算速度的范围为0~0.05m/s.结果表明:随着倾斜角度的增加,空泡份额径向分布逐渐由“核峰”、“壁峰”分布向单一“壁峰”分布转变;通过分析气泡受到的横向升力、浮力径向分量和壁面力,发现升力、浮力、壁面力的共同作用,使气泡在圆管径向位置15mm与22mm之间处聚集,从而造成空泡份额沿径向呈“壁峰”型分布.

     

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出版历程
  • 收稿日期:  2013-03-27
  • 刊出日期:  2014-06-28

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