在增材制造的超粗糙通道中流动

IF 2.8 Q2 MECHANICS
Samuel Altland, X. Zhu, S. McClain, R. Kunz, Xiang I. A. Yang
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引用次数: 4

摘要

金属增材制造已经为涡轮和热交换器应用提供了几何形状复杂的内部冷却通道,但该过程会产生与通道高度(500 $\mathrm {\mu }$ m)相当的大规模粗糙度。这些超粗糙通道给实验测量、数据解释和粗糙度建模带来了前所未有的挑战。首先,尚不清楚在特定流向和跨度位置的测量是否仍然提供平均(时间和平面平均)流量的准确表示。其次,我们不知道对数层是否存在。第三,尚不清楚以前开发的粗壁模型对这些大规模粗糙度的工作效果如何。为了回答上述实际问题,我们对增材制造的超粗糙通道的流动进行了直接数值模拟。考虑了三个粗糙表面,它们都是由增材制造表面的计算机断层扫描获得的。粗糙度的波谷到峰尺寸分别为0.1 $h$, 0.3 $h$和0.8 $h$,其中$h$是预期的半通道高度。每个粗糙表面相对于光滑壁和其他两个粗糙表面放置,导致六个粗糙壁通道配置。考虑两个雷诺数,即$Re_\tau =180$和$Re_\tau =395$。我们首先表明,在一个流向和跨向位置的测量是不够的,因为整个通道的平均流动不均匀性很强;其次,尽管平均流动不均匀,壁面的对数定律仍然存在;第三,建立的粗糙度遮蔽模型仍然准确。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flow in additively manufactured super-rough channels
Abstract Metal additive manufacturing has enabled geometrically complex internal cooling channels for turbine and heat exchanger applications, but the process gives rise to large-scale roughness whose size is comparable to the channel height (which is 500 $\mathrm {\mu }$m). These super-rough channels pose previously unseen challenges for experimental measurements, data interpretation and roughness modelling. First, it is not clear if measurements at a particular streamwise and spanwise location still provide accurate representation of the mean (time- and plane-averaged) flow. Second, we do not know if the logarithmic layer survives. Third, it is unknown how well previously developed rough-wall models work for these large-scale roughnesses. To answer the above practical questions, we conduct direct numerical simulations of flow in additively manufactured super-rough channels. Three rough surfaces are considered, all of which are obtained from computed tomography scans of additively manufactured surfaces. The roughness’ trough to peak sizes are 0.1$h$, 0.3$h$ and 0.8$h$, respectively, where $h$ is the intended half-channel height. Each rough surface is placed opposite a smooth wall and the other two rough surfaces, leading to six rough-wall channel configurations. Two Reynolds numbers are considered, namely $Re_\tau =180$ and $Re_\tau =395$. We show first that measurements at one streamwise and spanwise location are insufficient due to strong mean flow inhomogeneity across the entire channel, second that the logarithmic law of the wall survives despite the mean flow inhomogeneity and third that the established roughness sheltering model remains accurate.
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CiteScore
2.40
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