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The analysis of flow on round-edged delta wings

机译:圆边三角翼的流动分析

摘要

The flow around three-dimensional aircraft wings, including delta-wings is very complicated. Much experimental and numerical work has been performed to discover its complexity. To date, all numerical calculations on delta wings have been carried out for either fully laminar or fully turbulent boundary layers. The transition status of the boundary layer is considered unknown despite several efforts to identify transition from laminar to turbulent flow. One such study, called the International Vortex Flow Experiment – 2 (VFE-2), has been carried out by an international group and mainly focuses on the boundary layers on delta wings. The data from the VFE-2 experimentals potentially provide the location of transition on the upper and lower surfaces of the wing to guide associated numerical studies. The effects of Reynolds number, Mach number, angle of attack and the leading edge bluntness are also investigated. Almost all delta wing studies to date have involved tests on wings with sharp leading edges and these have led to the conclusion that the flows are relatively independent of Reynolds number. In fact, most real wings have finite leading edge radii. Hence, the flow separation is no longer fixed at the leading edge, thus making the flow dependent on Reynolds number. This particular aspect has been studied extensively by the VFE-2 team. As part of the VFE-2 project, Glasgow University constructed a delta wing with four different sets of leading edges. Small-, medium- and large-radius edges and a pair of sharp leading edges were constructed in order to compare results from four delta wing configurations. In the current study experiments were carried out on these wings in the 2.65 metre by 2.04 metre, closed circuit, Argyll Wind tunnel of Glasgow University. The models were mounted on a specially designed sting support structure that allowed them to be pitched around a constant centre of rotation throughout the experiments. Tests were conducted at speeds of 20.63 m/s and 41.23 m/s representing Reynolds numbers of 1 x 106 ;2 x 106 respectively, based on the mean aerodynamic chords of the wings. The tests were conducted in three phases. In the first phase, steady and unsteady forces and moments on all wings were measured at an angle of attack that varied from α =100 to 250. The forces and moments were captured at two sampling rates; i.e., 100 Hz and 8000 Hz. The second test series captured flow visualization data on the four wings. In these experiments, a mixture of Ondina oil and paraffin was combined with Dayglo powder and applied to the surfaces of the delta wings. The images of the flow topology on the wings were recorded. The final series of experiments involved Particle Image Velocimetry measurements. A stereo-PIV arrangement was applied in this experiment and two CCD-Cameras were positioned outside the test section for image capture. The current study has identified interesting features of the interrelationship between the conventional leading edge primary vortex and the occurrence and development of the inner vortex on the round-edged delta wings. The inner vortex was first identified and verified by the VFE-2 team. The effects of Reynolds number, angle of attack and leading-edge radii on both vortices are discussed in detail. The steady balance data have shown that the normal force coefficients are sensitive to leading edge bluntness at moderate angles of attack but are less so at high angles of attack. In relation to this, the flow visualization images have also shown that the primary vortex origin is located further aft on the wing at higher leading edge bluntness. This impacts on the strength of the inner vortex which remains a significant flow feature until the primary vortex approaches the apex. The lateral extent of the inner vortex is very dependent on the primary vortex at the leading edge; i.e. the weakening of the primary vortex has positive effects on the inner vortex. Particle Image Velocimetry shows that the increase in leading edge bluntness significantly decreases the swirl magnitude of the primary vortex. The results obtained from the current investigation provide considerable insight into the effects of Reynolds number, angle of attack and bluntness on the flow structures experienced by delta wings, with rounded leading edges. This work will, therefore, inform and guide future investigations of delta wing flows and has the potential to impact on future wing design.
机译:三维飞机机翼(包括三角翼)周围的流动非常复杂。为了发现其复杂性,已经进行了许多实验和数值工作。迄今为止,已经对完全层流或完全湍流的边界层进行了三角翼上的所有数值计算。尽管人们为识别从层流到湍流的过渡做出了许多努力,但仍认为边界层的过渡状态未知。一个国际组织进行了一项这样的研究,称为国际涡流实验– 2(VFE-2),主要研究三角翼的边界层。 VFE-2实验的数据可能提供机翼上下表面的过渡位置,以指导相关的数值研究。还研究了雷诺数,马赫数,攻角和前沿钝度的影响。迄今为止,几乎所有的三角翼研究都涉及对具有锋利前缘的机翼进行的试验,这些试验得出的结论是流量相对独立于雷诺数。实际上,大多数实际机翼的前缘半径都有限。因此,流分离不再固定在前缘,从而使流取决于雷诺数。 VFE-2小组已对该特定方面进行了广泛研究。作为VFE-2项目的一部分,格拉斯哥大学建造了带有四组不同前缘的三角翼。构造了小,中,大半径的边缘以及一对尖锐的前缘,以便比较四个三角翼构造的结果。在当前的研究中,实验是在格拉斯哥大学Argyll风洞的2.65米x 2.04米闭路封闭机翼上进行的。将模型安装在特殊设计的支撑结构上,该结构可在整个实验过程中围绕恒定的旋转中心进行俯仰。根据机翼的平均空气动力弦,分别以20.63 m / s和41.23 m / s的速度进行测试,分别表示雷诺数为1 x 106; 2 x 106。测试分三个阶段进行。在第一阶段,以α= 100到250的迎角测量所有机翼上的稳定力和非稳定力和力矩。即100 Hz和8000 Hz。第二个测试系列捕获了四个机翼上的流量可视化数据。在这些实验中,将Ondina油和石蜡的混合物与Dayglo粉末混合,并涂在三角翼的表面。记录了机翼上流动拓扑的图像。最后一系列实验涉及粒子图像测速仪的测量。在该实验中采用了立体声PIV装置,并且将两个CCD相机放置在测试部分的外面以进行图像捕获。当前的研究已经确定了常规前沿初级涡旋与圆形三角翼上内部涡旋的发生和发展之间相互关系的有趣特征。内部涡旋首先由VFE-2小组识别并验证。详细讨论了雷诺数,迎角和前沿半径对两个涡流的影响。稳定的平衡数据表明,法向力系数在中等迎角下对前缘钝度敏感,而在大迎角下则较小。与此相关的是,流动可视化图像还显示出,主要涡旋起点位于机翼的后部,其前缘钝度较高。这影响了内部涡流的强度,该强度仍然是重要的流动特征,直到初级涡流接近顶点为止。内部涡旋的横向范围在很大程度上取决于前缘的初级涡旋。即,初级涡旋的减弱对内部涡旋具有积极影响。粒子图像测速表明,前缘钝度的增加显着降低了初级涡旋的旋涡量。从目前的研究中获得的结果为雷诺数,攻角和钝度对三角翼具有圆形前缘的流动结构的影响提供了相当深入的见识。因此,这项工作将为三角翼流动的未来研究提供信息并提供指导,并可能影响未来的翼设计。

著录项

  • 作者

    Mat Shabudin Bin;

  • 作者单位
  • 年度 2011
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  • 原文格式 PDF
  • 正文语种 English
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