分布单元粗糙度模型在增材制造内冷却通道中的应用

Samuel Altland, Xiang I. A. Yang, K. Thole, R. Kunz, S. McClain
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摘要

内部流动系统的冷却效果设计依赖于动态损失和传热的精确模型。在这些系统中(例如,燃气轮机叶片,中间冷却器,热交换器),可以存在数千个不同配置和粗糙度形态的单独通道。近年来,增材制造(AM)进一步扩大了设计空间,但会产生大规模的粗糙度特征,其尺寸与通道高度相当。这些系统的粗糙度长度尺度的范围使得解决粗糙表面的CFD在设计水平上不切实际。另外,可以利用体积粗糙度建模方法,如分布式单元粗糙度模型(DERM),因为它们的计算成本要低几个数量级。本文提出了一种基于双平均Navier-Stokes (DANS)方程的DERM模型,并将其应用于以燃气轮机叶片冷却通道为代表的增材制造粗糙通道。这种DERM公式的独特之处在于对DERM阻力系数和空间平均雷诺应力的具体处理。这种广义的阻力系数公式允许在更广泛的潜在粗糙度场中提高模型精度,而不必依赖于每种形态的校准。提出了一种新的两层方法来模拟空间平均雷诺应力。麦克莱恩等人记录的三种不同的AM粗糙表面被配置为相对的光滑壁,以及彼此,以创建总共六个通道配置。在6种情况下,粗糙度波谷至峰值尺寸范围为0.15δ ~ 0.66δ,其中δ为通道半宽,粗糙度雷诺数范围为Rek = 60 ~ Rek = 300。对空间和时间平均平均流量的DERM预测与先前报道的DNS结果进行了比较。具体来说,我们观察到,在整个案例矩阵中,平均速度剖面、应力平衡和阻力划分的一致性很好。虽然DERM模型通常在相对较小的粗糙度雷诺数下校准到特定的确定性粗糙度形状族,但这些结果表明,对于目前更广义的公式,它们具有更广泛的适用性。结果表明,所提出的模型可以适应典型的增材制造的大尺度随机粗糙度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Application of a Distributed Element Roughness Model to Additively Manufactured Internal Cooling Channels
Design for cooling effectiveness in internal flow systems relies on accurate models for dynamic losses and heat transfer. In these systems (e.g., gas turbine blades, intercoolers, heat exchangers), thousands of individual passages of varying configuration and roughness morphology can be present. In recent years, additive manufacturing (AM) has further expanded the design space, but can give rise to large-scale roughness features, whose sizes are comparable to the channel height. The range of roughness length scales in these systems makes CFD of the resolved rough surfaces impractical at a design level. Alternately, volumetric roughness modeling approaches, such as distributed element roughness models (DERM) can be leveraged, as they have computational costs orders of magnitude lower. In this work, a DERM model based on the Double Averaged Navier-Stokes (DANS) equations is presented and applied to additively manufactured rough channels, representative of gas turbine blade cooling passages. Unique to this formulation of DERM is the specific treatment of the DERM drag coefficient and the spatially averaged Reynolds stresses. This generalized formulation of the drag coefficient allows for improved model accuracy across a wider array of potential roughness fields, without having to rely on calibration for each morphology. A novel two-layer approach to modeling the spatially averaged Reynolds stress is also proposed. Three different AM rough surfaces documented by McClain et al. [1] were configured opposite smooth walls as well as each other to create a total of six channel configurations. Across the six cases, th roughness trough to peak size ranges from 0.15δ to 0.66δ, where δ is the channel half-width, and the roughness Reynolds number ranges from Rek = 60 to Rek = 300. DERM predictions for spatially and temporally averaged mean flow quantities are compared to previously reported DNS results. Specifically, we observe good agreement in the mean velocity profiles, stress balances and drag partitions across the case matrix. While DERM models are typically calibrated to specific deterministic roughness shape families at comparatively small roughness Reynolds numbers, these results demonstrate a wider range of applicability for the present, more generalized formulation. It is demonstrated that the proposed model can accommodate random roughness of large scale, typical of AM.
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