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Length Scales of Scalar Diffusion in the Convective Boundary Layer: Laboratory Observations

机译:对流边界层中标量扩散的长度尺度:实验室观察

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A laboratory study of scalar diffusion in the convective boundary layer has found results that are consistent with a 1999 large-eddy simulation (LES) study by Jonker, Duynkerke and Cuijpers. For bottom-up and top-down scalars (introduced as ‘infinite’ area sources of passive tracer at the surface and inversion, respectively) the dominant length scale was found to be much larger than the length scale for density fluctuations, the latter being equal to the boundary-layer depth h. The variance of the normalized passive scalar grew continuously with time and its magnitude was about 3–5 times larger for the top-down case than for the bottom-up case. The vertical profiles of the normalized passive scalar variance were found to be approximately constant through the convective boundary layer (CBL) with a value of about 3–8c * 2 for bottom-up and 10–50c * 2 for top-down diffusion. Finally, there was some evidence of a minimum in the variance and dominant length scale for scalar flux ratios (top-down to bottom-up flux) close to −0.5. All these convection tank results confirm the LES results and support the hypothesis that there is a distinct difference in behaviour between the dynamic and passive variables in the CBL.
机译:对流边界层中标量扩散的实验室研究发现,结果与Jonker,Duynkerke和Cuijpers的1999年大涡模拟(LES)研究一致。对于自下而上和自上而下的标量(分别作为表面和反面的无源示踪剂的“无限”区域源引入),发现主要长度尺度远大于密度波动的长度尺度,后者是相等的到边界层深度h。归一化被动标量的方差随时间连续增长,自上而下的情况比自下而上的情况大大约3-5倍。发现通过对流边界层(CBL),归一化的被动标量方差的垂直轮廓近似恒定,对于自下而上和10–50c,其值约为3–8c * 2 * 2 用于自上而下的扩散。最后,有一些证据表明标量通量比(自上而下至自下而上的通量)接近-0.5时方差和主导长度标度最小。所有这些对流槽的结果证实了LES结果,并​​支持了CBL中动态变量和被动变量之间的行为存在明显差异的假设。

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