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A wind tunnel simulation of the mean velocity fields behind upright porous fences.

机译:风洞模拟垂直多孔栅栏后面的平均速度场。

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Porosity is the most important parameter that determines the efficiency of wind fences. The present study provided a deeper understanding of mean flow regime behind fences with different porosities at different wind velocities by means of a scaled wind tunnel simulation. Velocities were measured using particle image velocimetry and the mean velocity field was obtained and discussed. The mean velocity fields obtained at different wind velocities were similar. Analyzing the streamline patterns revealed an inherent link between fence porosity and mean airflow characteristics behind the fence. The optimal fence porosity is considered to be the critical porosity above or below which airflow characteristics differ strongly. According to the present study, the optimal porosity is found to be around 0.2 or 0.3, which corresponds to a critical porosity above which bleed flow dominates and below which reversed flow becomes significant. The parameters characterizing the reverse cell behind fences were well correlated with porosity. The velocity profiles revealed seven typical flow regions behind fences, characterized by different velocity gradients. The airflow becomes less complicated and the number of flow regions decreases as fence porosity increases. Some regions, especially the reverse cell and small vortex, disappear when the porosity exceeds a certain value. The flow regions gradually merge as the distance downwind increases, and eventually recover a single velocity profile due to downward transfer of momentum from overlying layers. The recovery distance decreases with increasing fence porosity.
机译:孔隙度是决定风挡效率的最重要参数。通过比例风洞模拟,本研究对不同风速下具有不同孔隙率的围栏后面的平均流态有了更深入的了解。使用粒子图像测速仪测量速度,并获得并讨论了平均速度场。在不同风速下获得的平均速度场相似。分析流线型式显示,围栏孔隙率与围栏后面的平均气流特征之间存在固有联系。最佳栅栏孔隙率被认为是高于或低于其临界值的临界孔隙率,气流特性差异很大。根据本研究,发现最佳孔隙率约为0.2或0.3,这对应于临界孔隙率,在该临界孔隙率之上,渗流占主导地位,在其之下,反向流动变得显着。栅栏后面的反向电池的特征参数与孔隙度密切相关。速度分布图揭示了栅栏后面的七个典型流动区域,其特征是速度梯度不同。随着围栏孔隙率的增加,气流变得不太复杂,流动区域的数量减少。当孔隙率超过一定值时,某些区域,特别是反向孔和小涡旋消失。流动区域随着顺风距离的增加而逐渐融合,并由于动量从上覆层向下转移而最终恢复了单一速度分布。恢复距离随着围栏孔隙率的增加而减小。

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