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Turbulent fluctuations above the buffer layer of wall-bounded flows

机译:壁面流动缓冲层上方的湍流波动

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The behaviour or the velocity and pressure fluctuations in the logarithmic and outer layers or turbulent flows is analysed using spectral information and probability density functions from channel simulations at R-e tau <= 2000. Comparisons arc made with experimental data at higer Reynolds numbers. It is round, in agreement with previous investigations, that the intensity profiles or the streamwise and spanwise velocity components have logarithmic ranges Una one traced to the widening spectral range of scales as the wall is approached. The same is true for the pressure. both theoretically and observationally, Nu not For Me normal velocity or For the tangential stress cospectrum. although even those two quantities have structures will lengths of the order of several hundred times the wall distance. Bemuse the logarithmic range grows longer as the 1 Reynolds number increases, variables which am 'attached' in this sense scale I the buffer layer in mixed units. These results give Strong Support to the attached-eddy scenario Proposed by Townsend ( 1976), but they are not linked to any particular eddy model. The scaling or me outer nudes is also examined. The intensity of the streamwise velocity at fixed y/h increases with the Reynolds number. This is traced to the large-scale modes, and to an increased intensity of the ejections but not or me sweeps. Several differences are Found between Me outer structures of different flows. The outer modes of the spanwise and wall-normal velocities in boundary layers am stronger 01,111 in internal flows, and their streamwise velocities penetrate closer to the wall. As a consequence, their logarithmic layers am thinner, and some or their logarithmic slopes are different. The channel statistics am available electronically at http://torroja.dmt.upm.es/ftp/channels/.
机译:使用R-e tau <= 2000的通道模拟中的频谱信息和概率密度函数,分析了对数层和外层或湍流中的行为或速度和压力波动。使用雷诺数更大的实验数据进行了比较。圆形的,与先前的研究一致,强度分布或沿流向和沿跨度的速度分量具有对数范围。随着壁的接近,一个对数范围的扩大光谱范围可追溯。压力也是如此。在理论上和观察上,Nu都不适合我法向速度或切向应力谱。尽管即使这两个量具有结构,其长度也将是壁距的数百倍。因为对数范围随着1雷诺数的增加而变长,在这种意义上,变量“附加”在缓冲层中,以混合单位表示。这些结果为Townsend(1976)提出的附加涡流方案提供了有力的支持,但它们与任何特定的涡流模型均没有关联。还检查了缩放比例或我的外部裸体。固定y / h处的流向速度强度随雷诺数增加。这可以追溯到大型模式,并且可以提高喷射强度,但不能扫描。在不同流动的Me外部结构之间发现了几个差异。边界层中翼展方向和壁法向速度的外部模式在内部流中的强度为01,111,并且它们的流向速度更靠近壁。结果,它们的对数层更薄,并且一些或它们的对数斜率不同。频道统计信息可通过以下网址以电子方式获得:http://torroja.dmt.upm.es/ftp/channels/。

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