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Three dimensional Fluid Flow and Heat Transfer Characteristics of a Backward-Facing Step Flow in a Rectangular Duct

机译:三维流体流动和矩形管道中的背面步长的传热特性

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Various fundamental researches have been done in the backward-facing step flow that can easily produce separation and reattachment. While the relationship between fluid flow structure and heat transfer on the bottom wall is yet completely understood when the effect of side wall is taken into consideration. Here, a duct of 30mm height and of 240 mm width with a step of 15mm height were introduced. Velocity measurements have been done by PIV for various low Reynolds numbers based on the step height from 400 to 900. Distributions of local heat transfer coefficients were measured by making use of a thermosensitive liquid crystal sheet that showed the different color distribution for various temperature values. Large attention was paid to the relationship between fluid flow structures and heat transfer. The local Nusselt number changes not only in streamwise direction but also spanwise direction, the maximum Nusselt number always appear near the side wall region even if the flow Reynolds number is varied. As the Reynolds number increases, the average heat transfer coefficient on the bottom wall increases. The heat transfer coefficient increases near the reattachment region while is higher on the slightly downstream side of the reattached region. The region with the large velocity fluctuation intensity on the bottom wall surface is located slightly downstream of the reattachment region. And the high heat transfer region is in good agreement with that with large flow fluctuation. The reason why the maximum heat transfer area is located on the side wall is mainly related to the strong flow fluctuation.
机译:在后面的步骤流动中已经完成了各种基本研究,可以轻松地产生分离和重新附着。虽然当考虑侧壁的效果时,尚未理解流体流动结构与底壁的热传递之间的关系。这里,引入了30mm高度和240 mm宽度的管道,宽度为15mm高度。基于400至900的台阶高度,通过PIV进行各种低雷诺数的速度测量。通过使用热敏液晶片来测量局部传热系数的分布,所述热敏液晶片显示出各种温度值的不同颜色分布。对流体流动结构和传热之间的关系支付了很大的关注。局部纽带的数量不仅在流动方向上变化,而且也是翼展的方向,即使流动雷诺数数量变化,最大露天数始终在侧壁区域附近出现。随着雷诺数的增加,底壁的平均传热系数增加。热传递系数在重新连接区域附近增加,而重新连接区域的略微下游侧较高。底壁表面上具有大的速度波动强度的区域位于重新连接区域的略微下游。高温传递区域与具有大流量波动的良好一致。最大传热区域位于侧壁上的原因主要与强流量波动有关。

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