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Stable Boundary Layer Depth from High-Resolution Measurements of the Mean Wind Profile

机译:高分辨率平均风廓线测量结果得出的稳定边界层深度

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The depth h of the stable boundary layer (SBL) has long been an elusive measurement. In this diagnostic study the use of high-quality, high-resolution (Az = 10 m) vertical profile data of the mean wind U(z) and streamwise variance omega_u~2(z) is investigated to see whether mean-profile features alone can be equated with h. Three mean-profile diagnostics are identified: _1, the height of maximum low-level-jet (LLJ) wind speed U in the SBL; hi, the height of the first zero crossing or minimum absolutevalue of the magnitude of the shear dU/dz profile above the surface; and h_2, the minimum in the curvature delta~2U/delta z~2 profile. Boundary layer BL here is defined as the surface-based layer of significant turbulence, so the top of the BL was determined as the first significant minimum in the omega_u~2(z) profile, designated as h_(omega). The height h_(omega) was taken as a reference against which the three mean-profile diagnostics were tested. Mean-wind profiles smooth enough to calculate secondderivatives were obtained by averaging high-resolution Doppler lidar profile data, taken during two nighttime field programs in the Great Plains, over 10-min intervals. Nights are chosen for study when the maximum wind speed in the lowest 200 m exceeded5 m s~(-1) (i.e., weak-wind, very stable BLs were excluded). To evaluate the three diagnostics, data from the 14-night sample were divided into three profile shapes: Type I, a traditional LLJ structure with a distinct maximum or "nose," Type II, a "flat"structure with constant wind speed over a significant depth, and Type III, having a layered structure to the shear and turbulence in the lower levels. For Type I profiles, the height of the jet nose hj, which coincided with h_1 and h_2 in this case, agreed with the reference SBL depth to within 5 %. The study had two maj or results: 1) among the mean-profile diagnostics for h, the curvature depth h_2 gave the best results; for the entire sample, h_2 agreed with h_(omega) to within 12%; 2) considering the profile shapes, the layered Type III profiles gave the most problems. When these profiles could be identified and eliminated from the sample, regression and error statistics improved significantly: mean relative errors of 8% for hj and hi, and errorsof <5% for h_2, were found for the sample of only Type I and II profiles.
机译:长期以来,稳定边界层(SBL)的深度h一直难以捉摸。在此诊断研究中,研究了使用平均风量U(z)和流向方差omega_u〜2(z)的高质量,高分辨率(Az = 10 m)垂直剖面数据的情况,以查看是否仅靠平均剖面特征可以等于h。确定了三个平均轮廓诊断:_1,SBL中最大低空喷射(LLJ)风速U的高度; hi,表面上方的第一个零交叉的高度或剪切dU / dz轮廓的大小的最小绝对值; h_2是曲率δ〜2U /δz〜2曲线中的最小值。边界层BL在此定义为具有明显湍流的基于表面的层,因此将BL的顶部确定为omega_u〜2(z)轮廓中的第一个重要最小值,称为h_(ω)。高度h_(ω)作为参考,对这三个均值轮廓诊断程序进行了测试。平均风廓线足够平滑以计算二阶导数,是通过对高分辨率的多普勒激光雷达廓线数据进行平均而获得的,该数据在大平原地区的两个夜间野外计划中以10分钟为间隔。当最低200 m的最大风速超过5 m s〜(-1)(即弱风,非常稳定的BL排除在外)时,选择夜晚作为研究对象。为了评估这三种诊断,将14个晚上的样本中的数据划分为三种轮廓形状:I型,一种传统的LLJ结构,具有明显的最大值或“鼻子”,II型,一种“平坦”的结构,在整个过程中风速恒定较大的深度和III型,在较低的水平上具有分层的剪切和湍流结构。对于类型I轮廓,喷头高度hj(在这种情况下与h_1和h_2一致)与参考SBL深度在5%之内一致。该研究有两个主要结果:1)在h的平均轮廓诊断中,曲率深度h_2给出了最佳结果;对于整个样本,h_2与h_(ω)相符,在12%以内; 2)考虑到轮廓形状,分层的III型轮廓存在最多的问题。当可以从样本中识别出这些轮廓并将其消除时,回归和误差统计显着改善:仅I型和II型轮廓的样品的hj和hi的平均相对误差为8%,h_2的误差为<5% 。

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