下击暴流作用下平屋面风荷载CFD数值模拟
详细信息 本馆镜像全文    |  推荐本文 | | 获取馆网全文
摘要
下击暴流具有与常规大气边界层近地风完全不同的风场特征.基于CFD(Computationalfluid dynamics)数值仿真技术,完成了几何缩尺比为1∶2 000的下击暴流过程的数值模拟,并将其风剖面的模拟结果与理论模型进行了对比.在此基础上,研究在下击暴流作用下,将大跨平屋面置于距下击暴流中心不同径向位置时,屋面平均风压系数和速度场的分布规律,并与大气边界层风场中平屋面的风荷载特性进行了对比.结果表明:数值模拟方法能够较好地再现下击暴流的风场特性;下击暴流风场中平屋面风压分布规律明显区别于大气边界层风场中的风压特性;平屋面风压分布特性与其距下击暴流中心的距离密切相关,随着平屋面逐渐远离下击暴流中心,屋面所承受的压力逐渐由正压转为负压.
Wind profiles and characteristics in thunderstorm downburst are significantly different from the regular boundary layer winds.Based on the computational fluid dynamics(CFD) commercial software,thunderstorm downburst is simulated in the 1∶2 000 geometry scales,and the results are compared to the theoretical model.Effects on mean pressure coefficients of the distance from the roof to the center of the downburst are investigated by placing flat-roofs at different radial locations.Pressure coefficients and flow velocity around the roof are analyzed and compared to the results in the boundary layer winds.The results show that numerical simulations can appropriately reproduce the wind profiles and characteristics of the downburst.The pressure coefficient distribution of flat-roofs in the thunderstorm downburst is obviously different from that in the boundary layer winds.The pressure coefficient distribution depends on the distance between the flat-roof and the center of the thunderstorm downburst.The pressure of the roof gradually changes from positive value to negative when the flat-roof is moved away from the center of the impinging jet.
引文
[1]Fujita T T.Downburst:Meteorological features and windfield characteristic[J].Journal of Wind Engineering and In-dustrial Aerodynamics,1990,36:75-86.
    [2]Chen L,Letchford C W.Mult-i scale correlation analysis oftwo lateral profiles of ful-l scale downburst wind speeds[J].Journal of Wind Engineering and Industrial Aerodynamics,2006,94(9):675-696.
    [3]Holmes J D.Modeling of extreme thunderstorm winds forwind loading of structures of structures and risk assessment[C]//Wind Engineering Into 21st Century,Proceedings of10th International Conference on Wind Engineering,Copenhagen,Denmark,1999:1409-1415.
    [4]Nicholls M,Pielke R,Meroney R.Large eddy simulationof microburst winds flowing around a building[J].Journalof Wind Engineering and Industrial Aerodynamics,1993,46/47:229-237.
    [5]Anindya Sengupta,Partha P Sarkar.Experimental mea-surement and numerical simulation of an impinging jet withapplication to thunderstorm microburst winds[J].Journalof Wind Engineering and Industrial Aerodynamics,2008,96(3):345-365.
    [6]瞿伟廉,吉柏锋,李健群,等.下击暴流风的数值仿真研究[J].地震工程与工程振动,2008,28(5):133-139.QU Weilian,JI Baifeng,LI Jianqu,et al.The study on nu-merical simulation of downburst wind[J].Journal of Earth-quake Engineering and Engineering Vibration,2008,28(5):133-139.(in Chinese)
    [7]Hjelmfelt M R.Structure and life circle of microburst out-flows observed in Colorado[J].Journal of Applied Meteo-rology,1988,27(8):900-927.
    [8]瞿伟廉,王锦文.下击暴流风荷载的数值模拟[J].武汉理工大学学报,2008,30(2):70-74.QU Weilian,WANG Jinwen.Numerical simulation ofdownburst wind loads[J].Journal of Wuhan University ofTechnology,2008,30(2):70-74.(in Chinese)
    [9]Chen L,Letchford C W.A deterministic-stochastic hybridmodel of downbursts and its impact on a cantilever struc-ture[J].Engineering Structures,2004,26(5):619-626.
    [10]Vicroy D D.Assessment of microburst models for down-draft estimation[J].Journal of Aircraft,1992,29(6):1043-1048.
    [11]Oseguera R M,Bowles R L.A simple analytic 3-dimen-sional downburst model based on boundary layer stagna-tion flow[R].Langley Research Center,1988.
    [12]Wood G S,Kenny C S Kwok,Motteram N A,et al.Physical and numerical modeling of thunderstorm down-bursts[J].Journal of Wind Engineering and IndustrialAerodynamics,2001,89(6):532-552.

版权所有:© 2023 中国地质图书馆 中国地质调查局地学文献中心