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Subsonic Jet Noise Source Location as a Function of Nozzle Geometry

机译:亚音速射流噪声源位置与喷嘴几何形状的关系

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Over the years, there have been numerous studies on determining subsonic jet noise source locations, typically plotted as Strouhal number as a function of distance from the nozzle exit. A comparison of the results of various studies yields a spread of about two nozzle diameters in measured source location. This work examines how nozzle geometry could be a potential cause of observed differences in different studies in subsonic jet noise source location. ASME and conical nozzles of nominally the same diameter are compared using source location, schlieren flow visualization, and velocity profile measurements. ASME nozzles, which are designed to have thinner nozzle exit boundary layers, have noise source distributions that are 0.25 to 2 diameters upstream of their conical counterparts. The thinner nozzle exit boundary layers of the ASME nozzles results in faster growth of turbulent structures in the mixing layer. Because the size of these structures is inversely proportional to the frequency of noise produced by the structures, this faster growth results in the upstream shift seen in the source location.
机译:多年来,已经进行了许多有关确定亚音速喷射噪声源位置的研究,通常将其绘制为斯特劳哈尔数作为距喷嘴出口距离的函数。各种研究结果的比较结果表明,在测得的光源位置上散布了大约两个喷嘴直径。这项工作研究了喷嘴几何形状如何可能成为在亚音速喷射噪声源位置的不同研究中观察到差异的潜在原因。使用源位置,schlieren流量可视化和速度分布测量结果,比较了ASME和标称直径相同的圆锥形喷嘴。被设计为具有更薄的喷嘴出口边界层的ASME喷嘴,其圆锥形上游的噪声源分布直径为0.25到2毫米。 ASME喷嘴的喷嘴出口边界层越薄,导致混合层中湍流结构的生长越快。由于这些结构的大小与这些结构产生的噪声的频率成反比,因此这种较快的增长会导致在源位置看到上游偏移。

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