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Receptivity and Stability of Supersonic Swept Flows

机译:超声速扫流的接受度和稳定性

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摘要

The receptivity, stability, and transition of three-dimensional supersonic boundary layers over 1) a swept cylinder, 2) a swept wing with a sharp leading edge, and 3) a swept wing with a blunt leading edge are numerically investigated for a freestream Mach number of 3. These computations are performed for the same conditions as those in the experimental and computational study of Archambaud et al. (Archambaud, J. P., Louis, F., Seraudie, A., Arnal, D., and Carrier, G., "Natural Transition in Supersonic Flows: Flat Plate, Swept Cylinder, Swept Wing,"AIAA Paper 2004-2245,2004). The steady flow fields with and without roughness elements are obtained by solving the full Navier-Stokes equations. The N factors computed in this study at the transition onset locations reported by Archambaud et al. for flows over the swept cylinder are approximately 16.5 for traveling crossflow disturbances and 9 for stationary disturbances. The N factors for the traveling crossflow are high based on past experiences. However, they are comparatively smaller than those reported by Archambaud et al., who found iV-factor values in the range of 20 to 25 for traveling disturbances and 13 to 20 for stationary disturbances. The N factors computed for the traveling and stationary disturbances for the flow over the sharp wing are approximately 7 and 2.5, respectively, and for the flow over the blunt wing are 6.5 and 4.8, respectively. The initial amplitudes of the stationary crossflow vortices originating from the isolated roughness elements for the flow over the cylinder are about 300 times smaller than those generated in flows over the sharp and blunt wings with the same roughness heights. This explains the large differences observed in the N factors at the transition onsets between the flow over the cylinder and the wings.
机译:对自由流马赫数进行了三维超声速边界层在1)扫掠圆柱体,2)带有锋利前缘的扫掠机翼和3)带有钝化前缘的扫掠机翼的接受度,稳定性和过渡的数值研究这些计算是在与Archambaud等人的实验和计算研究相同的条件下进行的。 (Archambaud,JP,Louis,F.,Seraudie,A.,Arnal,D。和Carrier,G。,“超音速流动的自然转变:平板,后掠圆柱体,后掠翼”,AIAA文件2004-2245,2004 )。通过求解完整的Navier-Stokes方程,可以获得带或不带粗糙度元素的稳态流场。在这项研究中计算出的N个因子是由Archambaud等报道的。对于行进的横流扰动,流过后掠缸的流量大约为16.5,对于固定扰动,大约为9。根据过去的经验,行进横流的N个因素很高。但是,它们比Archambaud等人的报告要小,后者发现行进干扰的iV因子值在20到25之间,静止干扰的iV因子在13到20范围内。计算出的锋利机翼上的流动和静止扰动的N因子分别约为7和2.5,而钝机翼上的流动的N因子分别为6.5和4.8。静止的错流涡流的初始振幅是由于在圆筒上流动而由孤立的粗糙度元素产生的,其初始振幅大约是在具有相同粗糙度高度的尖锐钝角机翼上的流动中产生的振幅的300倍。这解释了在汽缸和机翼上的流动之间的过渡开始时,在N因子中观察到的巨大差异。

著录项

  • 来源
    《AIAA Journal》 |2012年第7期|p.1476-1489|共14页
  • 作者

    P. Balakumar; Rudolph A. King;

  • 作者单位

    NASA Langley Research Center, Hampton, Virginia 23681;

    NASA Langley Research Center, Hampton, Virginia 23681;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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