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Dispersion of a Point-Source Release of a Passive Scalar Through an Urban-Like Array for Different Wind Directions

机译:通过不同城市风向的类似城市阵列的无源标量点源释放的色散

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摘要

The dispersion of a point-source release of a passive scalar in a regular array of cubical, urban-like, obstacles is investigated by means of direct numerical simulations. The simulations are conducted under conditions of neutral stability and fully rough turbulent flow, at a roughness Reynolds number of Re τ = 500. The Navier–Stokes and scalar equations are integrated assuming a constant rate release from a point source close to the ground within the array. We focus on short-range dispersion, when most of the material is still within the building canopy. Mean and fluctuating concentrations are computed for three different pressure gradient directions (0°, 30°, 45°). The results agree well with available experimental data measured in a water channel for a flow angle of 0°. Profiles of mean concentration and the three-dimensional structure of the dispersion pattern are compared for the different forcing angles. A number of processes affecting the plume structure are identified and discussed, including: (i) advection or channelling of scalar down ‘streets’, (ii) lateral dispersion by turbulent fluctuations and topological dispersion induced by dividing streamlines around buildings, (iii) skewing of the plume due to flow turning with height, (iv) detrainment by turbulent dispersion or mean recirculation, (v) entrainment and release of scalar in building wakes, giving rise to ‘secondary sources’, (vi) plume meandering due to unsteady turbulent fluctuations. Finally, results on relative concentration fluctuations are presented and compared with the literature for point source dispersion over flat terrain and urban arrays.
机译:通过直接数值模拟研究了无源标量的点源释放在规则的三次方城市样障碍物中的分散性。该模拟是在中性稳定性和完全粗糙的湍流条件下进行的,Re的雷诺数为Re τ =500。Navier–Stokes和标量方程式的积分是假设从点开始恒定速率释放源靠近阵列内的地面。当大多数材料仍在建筑物顶篷内时,我们专注于短距离色散。计算三个不同压力梯度方向(0°,30°,45°)的平均浓度和波动浓度。结果与水通道中0°流动角下测得的可用实验数据非常吻合。比较了不同力角下的平均浓度分布和分散模式的三维结构。识别并讨论了影响羽状结构的许多过程,包括:(i)标量沿“街道”的平流或引导,(ii)湍流波动引起的横向弥散和建筑物周围流线划分引起的拓扑弥散,(iii)倾斜流随着高度的变化而产生的羽流;(iv)由于湍流扩散或平均再循环而受阻;(v)建筑尾流中夹带和标量的释放,从而产生了“二次源”;(vi)由于不稳定的湍流而使羽流蜿蜒波动。最后,给出了相对浓度波动的结果,并将其与平面地形和城市阵列上点源扩散的文献进行了比较。

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