壁面湍流减阻正弦纹波最佳形状的实验与数值研究

M. Sasamori, O. Iihama, H. Mamori, K. Iwamoto, A. Murata
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引用次数: 1

摘要

背景和目的在壁面湍流中,蒙皮摩擦阻力显著增加。减少表面摩擦阻力的技术需要开发,因为它有望降低运输设备的能源成本。减少皮肤摩擦阻力的一种众所周知的方法是在壁面上安装流向微槽,这被称为“纹面”。由于波纹表面可以很容易地应用于现有设备,因此已经进行了许多类型的“二维波纹形状”(以下简称2-D波纹),并证实了它们的减阻效果,例如Walsh (1980);Bechert et al. (1997);崔(1989)。在这里,“二维”意味着条纹沿流方向排列。对二维波纹的形状进行了优化,其减阻率约为10% (Bechert et al., 1997)。优化后的二维波纹为叶片型,相邻壁面很薄,横向间距小于流向涡的直径。Choiet al.(1993)报道,由于肋波的横向间距小于流向涡的直径,肋波影响喷射和扫掠事件,并抑制流向涡接近近壁区域。然而,为了在实际应用中应用波纹管,需要具有更高减阻效果的波纹管表面,因为上述减阻效果所减少的燃料成本不足以支付波纹管的维护成本(Viswanath, 2002)。为了获得更高的减阻效果,研究人员还对三维纹面(3d纹面)进行了研究,而不是二维纹面。“3-D”意味着波纹的形状在流的方向上是不同的。Peet & Sagaut(2009)提出的波纹状波纹是一种预期的波纹状波纹。他们的目标是获得类似于跨向壁振荡技术的效果,例如,Choi和Graham(1998)。他们发现了7.4%的减阻率,并得出结论,减少横流湍流有助于减阻。然而,据笔者所知,三维波纹管的减阻率比优化后的二维波纹管要小。这是因为与二维波纹相比,三维波纹的形状参数较多,难以进行形状优化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
EXPERIMENTAL AND NUMERICAL STUDIES ON OPTIMAL SHAPE OF A SINUSOIDAL RIBLET FOR DRAG REDUCTION IN WALL TURBULENCE
BACKGROUND AND OBJECTIVES Skin friction drag significantly increases in wall turbulence. Techniques for reducing skin friction drag are required to be developed because it is expected to decrease energy costs of transportation equipment. A wellknown method for decreasing skin friction drag is installing streamwise micro grooves on wall surfaces, which are called as ‘riblet surfaces’. Since riblet surfaces can be readily applied to existing equipments, so many types of ‘twodimensional riblet shapes’ (refereed as 2-D riblets, hereafter) have been performed and their drag reduction effects have been confirmed, e.g., Walsh (1980); Bechert et al. (1997); Choi (1989). Here, the ‘2-D’ means that the riblets are aligned in the streamwise direction. The shape of 2-D riblets has been optimized, of which drag reduction rate is approximately 10% (Bechert et al., 1997). The optimized 2-D riblet is a blade-type with very thin adjacent walls, and the lateral spacing is smaller than the diameter of streamwise vortices. Choiet al. (1993) reported that the riblet affects ejection and sweep events and inhibits streamwise vortices approaching to near-wall regions, because the lateral spacing of the riblet is smaller than the diameter of streamwise vortices. However, riblet surfaces with higher drag reduction effect are required in order to apply riblets in practical applications, because decrease in fuel costs by the abovementioned drag reduction effect was not sufficient to cover maintenance costs of the riblet (Viswanath, 2002). Instead of 2-D riblets, three-dimensional riblet surfaces (3-D riblets) have also been investigated in order to obtain higher drag reduction. The ‘3-D’ means that a riblet shape varies in the streamwise direction. One of expected riblet shapes is a wavy riblet suggested by Peet & Sagaut (2009). They aimed to obtain an effect similar to spanwise wall oscillation technique, e.g., Choi & Graham (1998). They found 7.4% drag reduction rate and concluded that decrease of crossflow turbulence contributes to drag reduction. As best of author’s knowledge, obtained drag reduction rates by 3-D riblets, however, are smaller than that by the optimized 2-D riblet. It is because an optimization of the shape of 3-D riblets is difficult due to many parameters of the shape as compared with those of 2-D riblet.
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