对流边界层表层的温度分布、羽流和光谱

K. Mcnaughton, S. Chowdhuri
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引用次数: 0

摘要

我们调查了温度模式和热输运在对流边界层(CBLs)的角度来看,这些是紧急性质的远非平衡,复杂的动力系统。我们引入了一个双温度(2T)玩具模型来定义羽流的横截面积,并将温度梯度、温度方差和热输运的标度特性与该区域联系起来。我们研究了温度($T$)概率密度函数和$w$-$T$联合概率密度函数,$T$光谱和$wT$共光谱在表面摩擦层内部和上面观察到。这里w是垂直速度。在讨论$T$谱和$wT$共谱时,我们着重讨论了SFL以上羽流和通量事件的自相似性。我们将$T$光谱中波数的混合长度尺度的$z^{1/2}$依赖性解释为反映羽流的横截面积,因此与$z^{-1/2}$形式的温度剖面有关,其中$z$为观测高度。基于SLTEST实验的数据,我们介绍了表面摩擦层(SFL)内的$T$谱和$wT$共谱的新的标度结果。我们证实了先前的结果,表明$T$光谱和$wT$共光谱的缩放行为在$z/z_s<0.1$(其中$z_s$为SFL的高度)以下发生变化,并开始显示与随机扩散相关的性质。最后,我们将我们对浮力在CBL流动中作为全系统作用的解释与理查森的解释进行了对比,理查森的观点为目前对边界层流动的统计流体力学模型的解释提供了信息。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Temperature profiles, plumes, and spectra in the surface layer of convective boundary layers
We survey temperature patterns and heat transport in convective boundary layers (CBLs) from the perspective that these are emergent properties of far-from-equilibrium, complex dynamical systems. We introduce a two-temperature (2T) toy model to define the cross-sectional areas of plumes, and connect the scaling properties of temperature gradients, temperature variance and heat transport to this area. We examine temperature ($T$) probability density functions and $w$-$T$ joint probability density functions, $T$ spectra and $wT$ cospectra observed both within and above the surface friction layer. Here $w$ is vertical velocity. In our discussion of $T$ spectra and $wT$ cospectra we focus on the self-similarity property of the plumes and flux events above the SFL. We interpret the $z^{1/2}$ dependence of the mixed length scale for wavenumbers in the $T$ spectra as reflecting the cross-sectional areas of the plumes, and so with the $z^{-1/2}$ form of the temperature profile, where $z$ is observation height. We introduce new scaling results for $T$ spectra and $wT$ cospectra from within the surface friction layer (SFL), based on a data from the SLTEST experiment. We confirm earlier results showing that the scaling behaviours of $T$ spectra and $wT$ cospectra change for heights below $z/z_s<0.1$, where $z_s$ the height of the SFL, and come to display properties associated with random diffusion. We conclude by contrasting our interpretation of the role of buoyancy as a system-wide action in CBL flows with that of Richardson, whose ideas inform the current interpretation of the statistical fluid mechanics model of boundary-layer flows.
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