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Effect of vortical structures on velocity and turbulent fields in the near region of an impinging turbulent jet

机译:涡流结构对撞击湍流射流近区速度和湍流场的影响

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摘要

This experimental study pertains to the formation of a secondary peak in heat transfer distribution for an axisymmetric turbulent impinging submerged jet. The analysis of instantaneous fields is undertaken at various Reynolds numbers based upon the bulk velocity and nozzle diameter (Re = 1300-10 000) and surface spacings (L/D = 0.25-6). Our analysis shows that flow separation and reattachment correspond to decrease/increase in local pressure and are caused by primary vortices; these are further linked to the location of maxima in streamwise and cross-stream velocities. It is further observed that the locations of maxima and minima in velocities are linked to fluctuations in rms velocities and thickening/thinning of the boundary layer. The vortices transported along the surface either coalesce among themselves or combine with other eddies to form a primary vortex. The primary vortex while getting convected downstream makes multiple interactions with the inner shear layer and causes waviness in instantaneous flow fields. In their later stage, the primary vortex moves away from the wall and accelerates, while the flow decelerates in the inner shear layer. The accelerated fluid in the outer shear layer pulls the downstream fluid from the inner shear layer and leads to the formation of a secondary vortex. After a certain distance downstream, the secondary vortex rolling between the primary vortex and the wall eventually breaks down, while the flow reattaches to the wall. The behavior of time average and instantaneous velocity fields suggests that unsteadiness in the heat transfer is linked to the location of maximum streamwise velocity, location of flow attachment, location of rms velocity, and thickness of the boundary layer. The instantaneous velocity fields show that for a given surface spacing, the chances for the appearance of the secondary vortex reduce with an increase in Reynolds number because of the reduction in space available for the secondary vortex to devel
机译:该实验研究涉及用于轴对称湍流撞击浸没射流的传热分布中的二次峰的形成。基于散装速度和喷嘴直径(RE = 1300-10000)和表面间距(L / D = 0.25-6),在各种雷诺数进行瞬时场的分析。我们的分析表明,流量分离和重新附着对应于局部压力的减少/增加,并由主涡流引起;这些进一步与最大线的位置相连,在流动和交叉流速度。进一步观察到,最大速度和最小值的位置与边界层的速度速度和增厚/变薄的波动相关联。沿着表面传输的涡流无论是合并的聚结,也可以与其他漩涡结合以形成主要涡旋。在进行对象时的主涡流使得与内剪切层进行多次相互作用,并在瞬时流场中引起波纹。在其后期的阶段,主要涡流远离墙壁移动并加速,而流动在内剪切层中减速。外剪切层中的加速流体从内剪切层拉动下游流体,并导致次级涡流的形成。在下游一定距离之后,初级涡流和墙壁之间的次级涡流最终破裂,而流向墙壁。时间平均和瞬时速度场的行为表明,传热中的不稳定性与最大流动速度,流动附件位置,RMS速度的位置和边界层的厚度的位置连接。瞬时速度场表明,对于给定的表面间隔,由于可用于开发的空间的空间减少,因此次级涡流外观的机会减少了雷诺数。

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  • 来源
    《Physics of fluids》 |2018年第3期|共17页
  • 作者单位

    Indian Inst Technol Dept Mech Engn Bombay 400076 Maharashtra India;

    Indian Inst Technol Dept Mech Engn Bombay 400076 Maharashtra India;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 流体力学;
  • 关键词

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