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首页> 外文期刊>Journal of Fluid Mechanics >Experimental study of the fine-scale structure of conserved scalar mixing in turbulent shear flows. Part 2. Sc approximate to 1
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Experimental study of the fine-scale structure of conserved scalar mixing in turbulent shear flows. Part 2. Sc approximate to 1

机译:湍流剪切流中守恒标量混合细尺度结构的实验研究。第2部分。Sc近似于1

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Results are presented from an experimental study into the fine-scale structure of generic, Sc approximate to 1, dynamically passive, conserved scalar fields in turbulent shear flows. The investigation was based on highly resolved, two-dimensional imaging of laser Rayleigh scattering, with measurements obtained in the self-similar far field of an axisymmetric coflowing turbulent jet of propane issuing into air at local outer-scale Reynolds numbers Re-delta = u delta/v of 11000 and 14000. The resolution and signal quality of these measurements allowed direct differentiation of the scalar field data zeta(x, t) to determine the instantaneous scalar energy dissipation rate field (Re Sc)(-1)del zeta . del zeta(x, t). Results show that, as for large-Sc scalars (Buch & Dahm 1996), the scalar dissipation rate field consists entirely of strained, laminar, sheet-like diffusion layers, despite the fact that at Sc approximate to 1 the scale on which these layers are folded by vorticity gradients is comparable to the layer thickness. Good agreement is found between the measured internal structure of these layers and the self-similar local solution of the scalar transport equation for a spatially uniform but time-varying strain field. The self-similar distribution of dissipation layer thicknesses shows that the ratio of maximum to minimum thicknesses is only 3 at these conditions. The local dissipation layer thickness is related to the local outer scale as lambda(D)/delta = Lambda Re-delta(-3/4) Sc-1/2, With the average thickness found to be [Lambda] = 11.2, with both the largest and smallest layer thicknesses following Kolmogorov (Re-delta(-3/4)) scaling. [References: 3]
机译:通过实验研究的结果给出了通用的Sc的精细尺度结构,Sc近似于1,湍流剪切流中的动态被动守恒标量场。该研究基于激光瑞利散射的高分辨率二维成像,在丙烷以局部外部尺度雷诺数Re-delta = u释放到空气中的轴对称同流湍流射流的自相似远场中获得的测量结果delta / v分别为11000和14000。这些测量的分辨率和信号质量允许直接区分标量场数据zeta(x,t)以确定瞬时标量能量耗散率场(Re Sc)(-1)del zeta。 del zeta(x,t)。结果表明,对于大Sc标量(Buch&Dahm 1996),标量耗散率场完全由应变,层状,片状扩散层组成,尽管事实是在Sc处近似为这些层的标度由涡度梯度折叠的折角与层厚度相当。对于空间均匀但随时间变化的应变场,在这些层的内部结构测量结果与标量传输方程的自相似局部解之间找到了很好的一致性。耗散层厚度的自相似分布表明,在这些条件下,最大厚度与最小厚度之比仅为3。局部耗散层的厚度与局部外标度有关,如λ(D)/δ=λ再δ(-3/4)Sc-1 / 2,平均厚度为λ= 11.2,其中Kolmogorov(Re-delta(-3/4))缩放后的最大和最小层厚度。 [参考:3]

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