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An Observational and Numerical Study of a Sheared, Convective Boundary Layer. Part I: Phoenix II Observations, Statistical Description, and Visualization

机译:剪切对流边界层的观测和数值研究。第一部分:凤凰二号观测,统计描述和可视化

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Four-dimensional velocity fields derived from dual Doppler radar observations are the basis of a description and statistical analysis of a convective, sheared planetary boundary layer during an afternoon over the High Plains of eastern Colorado. Mean velocities and momentum fluxes are calculated directly from the radar data and are verified with aircraft and tower data. Perturbation pressure and buoyancy fields are recovered for turbulent kinetic energy budgets, and for estimates of horizontal heat advection across the analysis area. The surface layer and lowest third of the observed boundary layer were similar to minimally sheared convective boundary layers, but there were significant differences in the upper two-thirds of the boundary layer. An overrunning residual mountain boundary layer merged with the locally generated convective boundary layer, producing a deep, continuously sheared layer of turbulent activity. Computer visualization reveals a complicated flow characterized by clusters of vortical structures extending well into the slightly stable overrunning region, frequently dominated by clusters of large, longlived vortices. First- and second-order statistics vary with time of day and averaging volume, suggesting that appropriate parameterizations of similar boundary layers should be functions of the required spatial and temporal scales and mesoscale environment. A number of common simplifying assumptions, scalings, and parameterizations employed for purely convective boundary layers would be inappropriate for this flow.
机译:从双多普勒雷达观测中得出的四维速度场是对科罗拉多东部高平原上一个下午的对流,剪切行星边界层进行描述和统计分析的基础。平均速度和动量通量直接从雷达数据中计算出,并通过飞机和塔架数据进行验证。恢复扰动压力和浮力场以用于湍动能预算,并用于估计整个分析区域的水平热对流。表层和观察到的边界层的最低三分之一与最小剪切对流边界层相似,但在边界层的上部三分之二处存在显着差异。越过的残余山边界层与局部生成的对流边界层合并,产生了深层的,连续剪切的湍流活动层。计算机可视化揭示了一个复杂的流动,其特征是涡旋结构簇很好地延伸到稍微稳定的超车区域,通常由大型,长寿命的旋涡簇主导。一阶和二阶统计量随一天中的时间和平均量的不同而变化,这表明相似边界层的适当参数化应该是所需的时空尺度和中尺度环境的函数。用于纯对流边界层的许多常见的简化假设,比例缩放和参数化均不适用于此流程。

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