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CATEGORY 5: SOUND GENERATION IN VISCOUS PROBLEMS, PROBLEM 2: SOUND GENERATION BY FLOW OVER A CAVITY

机译:第5类:声音在粘性问题中产生,问题2:通过流动的声音产生

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The discrete frequency sound produced by the flow of air at low subsonic speeds over a deep cavity was investigated. A long aspect ratio rectangular cavity with a leading edge overhang that cut off 1A of the cavity opening was placed flush with the top surface of a wind tunnel. The approach flow velocity was maintained at 50 m/s for the benchmark problem although results are also presented for other conditions. Boundary layer measurements conducted with a single element hotwire anemometer indicated that the boundary layer thickness just upstream of the cavity was equal to 17 mm. Sound pressure level measurements were made at three locations in the cavity: the center of the leading edge wall, the center of the cavity floor, and the center of the trailing edge wall. Three discrete tones were measured at all three locations with corresponding Strouhal numbers (based on cavity opening length and approach flow velocity) equal to 0.24, 0.26, and 0.41. The amplitudes of each tone were approximately equal at each measurement location in the cavity. Measurements made at other approach flow conditions indicated that the approach flow velocity and the boundary layer thickness affected the frequency characteristics of the discrete tones.
机译:研究了通过在深腔上低亚音速速度的空气流产生的离散频声。长纵横比具有前缘突出的矩形腔,其截止腔开口1a的截止值与风洞的顶表面齐平。虽然也呈现出其他条件,但是,接近流速在50米/秒保持在50米/秒的基准问题。用单个元件热线风速计进行的边界层测量结果表明,腔的上游的边界层厚度等于17mm。在腔中的三个位置进行声压级测量:前缘壁的中心,腔底板的中心,以及后缘壁的中心。在所有三个位置测量三个离散音,具有相应的斯特鲁姆数(基于腔开口长度和方法流速)等于0.24,0.26和0.41。每个音调的幅度在腔内的每个测量位置处大致相等。在其他方法流动条件下进行的测量表明,接近流速和边界层厚度影响了离散音的频率特性。

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