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湍流管道流动中最优放大的大规模条纹及减阻

Optimally amplified large-scale streaks and drag reduction in turbulent pipe flow.

作者信息

Willis Ashley P, Hwang Yongyun, Cossu Carlo

机构信息

Laboratoire d'Hydrodynamique (LadHyX), École Polytechnique, 91128 Palaiseau, France.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2010 Sep;82(3 Pt 2):036321. doi: 10.1103/PhysRevE.82.036321. Epub 2010 Sep 28.

DOI:10.1103/PhysRevE.82.036321
PMID:21230185
Abstract

The optimal amplifications of small coherent perturbations within turbulent pipe flow are computed for Reynolds numbers up to one million. Three standard frameworks are considered: the optimal growth of an initial condition, the response to harmonic forcing and the Karhunen-Loève (proper orthogonal decomposition) analysis of the response to stochastic forcing. Similar to analyses of the turbulent plane channel flow and boundary layer, it is found that streaks elongated in the streamwise direction can be greatly amplified from quasistreamwise vortices, despite linear stability of the mean flow profile. The most responsive perturbations are streamwise uniform and, for sufficiently large Reynolds number, the most responsive azimuthal mode is of wave number m=1 . The response of this mode increases with the Reynolds number. A secondary peak, where m corresponds to azimuthal wavelengths λ_{θ}^{+}≈70-90 in wall units, also exists in the amplification of initial conditions and in premultiplied response curves for the forced problems. Direct numerical simulations at Re=5300 confirm that the forcing of m=1,2 and m=4 optimal structures results in the large response of coherent large-scale streaks. For moderate amplitudes of the forcing, low-speed streaks become narrower and more energetic, whereas high-speed streaks become more spread. It is further shown that drag reduction can be achieved by forcing steady large-scale structures, as anticipated from earlier investigations. Here the energy balance is calculated. At Re=5300 it is shown that, due to the small power required by the forcing of optimal structures, a net power saving of the order of 10% can be achieved following this approach, which could be relevant for practical applications.

摘要

针对雷诺数高达100万的湍流管道流动,计算了小相干扰动的最优放大情况。考虑了三个标准框架:初始条件的最优增长、对谐波强迫的响应以及对随机强迫响应的卡尔胡宁 - 勒夫(本征正交分解)分析。与湍流平面通道流和边界层的分析类似,发现尽管平均流型具有线性稳定性,但沿流向拉长的条纹可以从准流向涡中得到极大放大。最敏感的扰动是沿流向均匀的,并且对于足够大的雷诺数,最敏感的方位角模式的波数(m = 1)。该模式的响应随雷诺数增加。在初始条件的放大以及强迫问题的预乘响应曲线中,还存在一个次峰值,其中(m)对应于壁面单位中方位角波长(\lambda_{\theta}^{+}≈70 - 90)。在(Re = 5300)下的直接数值模拟证实,对(m = 1)、(2)和(m = 4)的最优结构进行强迫会导致相干大尺度条纹的大幅响应。对于适度的强迫幅度,低速条纹变得更窄且能量更大,而高速条纹变得更分散。进一步表明,如早期研究所预期的那样,通过强迫稳定的大尺度结构可以实现减阻。这里计算了能量平衡。在(Re = 5300)时表明,由于强迫最优结构所需的功率较小,采用这种方法可以实现约10%的净功率节省,这可能与实际应用相关。

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