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Study of bubble-induced turbulence in upward laminar bubbly pipe flows measured with a two-phase particle image velocimetry

机译:两相粒子图像测速仪测量层流气泡流中气泡引起的湍流

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In the present study, focusing on characterizing the bubble-induced agitation (turbulence), spatially varying flow statistics of gas and liquid phases in laminar upward bubbly flows (Reynolds number of 750) with varying mean void fraction are investigated using a two-phase high-speed particle image velocimetry. As the flow develops along the vertical direction, bubbles with small-to-moderate void fractions, which were intentionally distributed asymmetrically at the inlet, migrate fast and show symmetric distributions of wall or intermediate peaking. Meanwhile, the mean liquid velocity saturates relatively slowly to a flat distribution at the core region. Despite small void fractions considered, the bubbles generate a substantial turbulence, which increases with increasing mean void fraction. Interestingly, it is found that the mean vertical velocity, bubble-induced normal stress in radial direction, and Reynolds stress profiles match well with those of a single-phase turbulent flow at a moderate Reynolds number (e.g., 10(4)), indicating the similarity between the bubble-induced turbulence and wall-shear-generated turbulence in a single-phase flow. Previously suggested scaling relations are confirmed such that the mean bubble rise velocity and bubble-induced normal stress (in both vertical and radial directions) scale with mean volume void fraction as a power of -0.1 and 0.4, respectively. Finally, based on the analysis of measured bubble dynamics (rise in an oscillating path), a theoretical model for two-phase turbulent (Reynolds) stress is proposed, which includes the contributions by the non-uniform distributions of local void fraction and relative bubble rise velocity, and is further validated with the present experimental data to show a good agreement with each other.
机译:在本研究中,着重于表征气泡引起的搅动(湍流),使用两相高压流研究了层流向上气泡流(雷诺数为750)的层流向上气泡流中气相和液相的空间变化流统计数据。速度粒子图像测速仪。随着流动沿垂直方向发展,有小到中等空隙率的气泡在入口处有意非对称地分布,它们迅速迁移并显示出壁的对称分布或中间峰。同时,平均液体速度在芯部区域相对缓慢地饱和至平坦的分布。尽管考虑到较小的空隙率,但气泡仍会产生明显的湍流,并随着平均空隙率的增加而增加。有趣的是,发现平均垂直速度,气泡在径向方向上引起的法向应力和雷诺应力分布与中等雷诺数(例如10(4))下的单相湍流的分布非常吻合,表明在单相流中气泡引起的湍流和壁切产生的湍流之间的相似性。先前建议的比例关系得到确认,以使平均气泡上升速度和气泡引起的法向应力(在垂直方向和径向方向上)均以平均体积空隙率(分别为-0.1和0.4的幂)缩放。最后,在对测得的气泡动力学(振荡路径上升)进行分析的基础上,提出了两相湍流(雷诺)应力的理论模型,该模型包括局部空隙率和相对气泡的不均匀分布的贡献。上升速度,并进一步验证与目前的实验数据,以显示彼此之间的良好协议。

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