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1.
基于欧拉—拉格朗日模式的风沙跃移数值模拟方法   总被引:1,自引:0,他引:1       下载免费PDF全文
通过对沙粒的起动过程以及粒床相互作用机理进行参数化处理,利用计算流体力学方法与离散动力学模拟对风场和沙粒进行耦合迭代,建立了基于欧拉—拉格朗日模式的、适用于研究风沙流二维特征的风沙跃移数值模型。通过模拟沙粒集团以及单颗沙粒跃移运动的随机特征,有效描述了风沙流垂向以及沿程变化规律,并且能够输出任意时刻每颗沙粒的空间位置、速度和加速度等信息。输沙通量的空间分布与现场观测实验数据有较高的吻合度,摩阻风速和风速廓线两个宏观物理量的变化情况与风沙流形成和发展的物理实际相符,说明了本数值模型和计算方法的合理性。  相似文献   

2.
根据丘陵浅山地区8个测点低空风速实测资料进行风速廓线拟合,求得风速幂指数,将大气环境质量预测中的风速模式化,用来预测大气污染物的浓度分布.  相似文献   

3.
高风速相干结构对通量输送影响的实验研究   总被引:2,自引:0,他引:2  
切变湍流的相干结构是湍流研究中的重大发现,它表明湍流运动并非完全随机,其中具有可检测的有序结构.本文通过处理南京浦口地区大气边界层观测数据,来分析不稳定层结中高风速相干结构特征.本次观测项目包括对场地中央的气象铁塔上2 m和40 m高度上超声风速仪的脉动速度、温度测量以及风廓线雷达对边界层风速廓线的测量.对超声水平风速时间序列数据进行小波变换 (时间尺度400 s),通过阈值来识别这种高风速相干结构.与多普勒风廓线雷达测量结果对比后发现,这种方法确定的相干结构符合常规的认识,具有较长的时间尺度和较大的垂直尺度 (接近边界层厚度).分析三天相干结构特性得到无量纲空间间隔约为6,即每隔6个边界层厚度的水平位置出现一个高速相干结构.通过与垂直风速小波系数的比较,发现高风速相干结构与向下垂直风速之间有较好相关,这与湍流中 “阵风” 现象的研究结论相似.使用四象限分析方法分类得到两种动量通量输送为负的运动:较小水平风速的上扬 (ejection) 运动 (简称为上扬运动) 和较大水平风速的下扫 (sweep) 运动 (简称为下扫运动),这两种运动在整个湍流活动中处于主导地位.高风速相干结构通过促进下扫运动和抑制上扬运动来影响动量通量的输送.  相似文献   

4.
集沙仪作为一种风蚀研究装置,可直接和准确的测定风沙流中的输沙量和风沙流结构。为此,我们自行设计了一种全自动、高频风沙流采样器—CWHF全自动集沙仪,并通过与2 m高度风速和Sensit跃移撞击传感器的野外配合观测,对比分析其野外实地的应用性能。CWHF全自动集沙仪整体外形呈“L”状,其最大特点是集沙容器底部安装有高精度单点称重传感器,使其能够实现集沙累积值的实时高频测量及长时间的采样任务。在野外环境中对沙尘暴天气背景下的相关数据进行分析,发现CWHF全自动集沙仪的累积量和输沙通量均与风速和撞击颗粒数间有较高的一致性,其能够很好地捕捉沙物质的输移信息,野外应用效果良好。此外,通过其估算塔中流动沙面2015年5月18日和25日两次沙尘暴天气近地表100 cm高度内,宽度为100 cm的截面上的水平输沙通量分别为101.37 kg和110.83 kg。  相似文献   

5.
利用风廓线雷达在延吉市开展了边界层风场的探测研究,根据2012年4个月逐日的边界层风场探测资料,分析了延吉市大气边界层风场的时空分布特征,得到了逐月的高空风廓线图。结果表明:1000m以下,水平风速和垂直风速随高度均呈现出增加的趋势,地面风速最小,750-1000m高度处存在明显的风切变层;2月和7月高空水平风速随高度的增加而增加,4月和10月高空水平风速变化呈单峰型的变化趋势;2月垂直风速随高度的增加逐渐增加,7月随高度的增加逐渐减少,4月和10月随高度呈双峰型的变化趋势;各月在1000~2000m高度垂直风速较小;各月水平风除个别高度外均以西风或偏西风为主导风向,垂直方向以下沉气流为主。  相似文献   

6.
苗曼倩  王彦昌 《大气科学》1985,9(3):300-307
根据大气边界层平均风速廓线实测资料,参照Lettau方法计算了湍流参数——动量交换系数k_m,摩擦速度u_*,湍流切应x和混合长l随高度的分布.并与国外研究结果进行比较,基本规律一致,某些参数有所修正.  相似文献   

7.
利用CFL-03边界层风廓线雷达,在塔中开展了边界层风场探测研究,根据2010年4月1日至2010年11月30日连续的边界层风场探测资料,分析了塔克拉玛干沙漠腹地大气边界层850 hPa、700 hPa和500 hPa特征层风场时空分布特征。结果表明,塔中地区850 hPa特征层主导风向为偏东风,风速年变化较小;700...  相似文献   

8.
集沙仪作为一种风蚀研究装置,可直接和准确地测定土壤风蚀过程中的输沙量和风沙流结构。为此,一种全自动、高频率的沙尘采样器(Continuously weighing,high frequency sand trap,简称:CWHF全自动集沙仪)被设计,并通过与2 m高度风速和Sensit跃移撞击传感器的野外配合观测,对比分析其野外实地的应用性能。CWHF全自动集沙仪整体外形呈"L"状,其最大特点是集沙容器底部安装有高精度单点称重传感器,使其能够实现集沙累积值的实时高频及长时间测量。通过对沙尘暴天气背景下的相关数据进行分析,发现CWHF全自动集沙仪的累积量和输沙通量均与风速和撞击颗粒数有较好的一致性,其能够很好地捕捉沙物质的输移信息,野外应用效果良好。  相似文献   

9.
王栋成  邱粲  曹洁  董旭光  王静 《气象科学》2018,38(3):416-422
采用统计、相关分析等方法,对2014年济南站边界层风廓线雷达观测资料和L波段雷达探空资料进行了长期时空变化规律的对比,进而研究了地面无降雨、有降雨时段两者的风向、风速数据的相关关系及差值。结果得出全年有降雨、无降雨时段两者的风向、风速总体一致性较好,相关性较高,并具有较好可比性和互补性的结论,对了解固定式边界层风廓线雷达探测的准确性,改进观测资料质量控制方法等具有很好的参考价值。  相似文献   

10.
应用大气二维边界层数值模式,对2008年夏季洪河国家级自然保护区沼泽湿地1000m高度边界层的温度、湿度廓线进行了3次模拟试验,并模拟分析了风速和下垫面粗糙度对湿地边界层温、湿廓线结构的影响.结果表明:(1)大气二维边界层模式可以较好的模拟湿地下垫面边界层的温、湿结构,并且该模式对位温的模拟效果优于比湿;(2)风速和粗...  相似文献   

11.
风蚀起沙对生态环境、人类健康及社会经济等具有很大的负面效应。利用美国Sensit公司生产的H11-LIN型风蚀传感器及贴地层风速梯度探测仪,对塔克拉玛干沙漠腹地塔中地区一次风蚀起沙过程进行了监测。结果表明:(1)风蚀起沙与微气象是一个互相影响互相制约的变化过程;(2)在此次观测试验过程中,我们观测到的最小起沙风速为6.0 m/s左右,同时发现起沙风速是一个变化的值,随着时间的延续呈现逐步增大的趋势,最小的起沙风速出现在风蚀开始发生的时候;(3)近地表风速廓线受沙粒运动影响明显,随着起沙量的增加,风速随高度变化的幅度增大,此时的风速廓线已不再遵循对数分布规律;(4)利用风蚀传感器测得塔中地区沙粒的临界起动摩擦速度为0.25 m/s,该值与经验公式估算的0.24 m/s非常接近,表明风蚀传感器在塔中地区具有较好的适用性;夏季塔中地区地表土壤湿度对风蚀起沙的阻碍作用可以忽略不计。 ?  相似文献   

12.
Separation of electrostatic charge during the transport of particles by wind adds a force to the gravitational and fluid forces that determine trajectories of particles moving by saltation. Evaluating this electrostatic force requires the electric field strength very near the saltation surface, and charge-to-mass ratios for the moving particles. Field mill readings 4 cm above the surface in a moderate blizzard showed electric field strength as high as +30 kV m-1. Another experiment gave charge-to-mass ratios of individual saltation particles in low-level drifting that ranged between +72 C kg-1 and -208 C kg-1. From these measurements, we estimated electrostatic forces as large as the gravitational force on some saltating particles. Including forces of this magnitude in the equations of motion significantly alters predicted saltation trajectories from those for uncharged particles. Predictions appear reasonable that for some saltating particles, the electrostatic force prevents new surface impacts. These results should help improve models of energy transfer in the planetary boundary layer during blizzards and sandstorms.  相似文献   

13.
Heterogeneous Saltation: Theory, Observation and Comparison   总被引:7,自引:0,他引:7  
In the theory of saltation, under development since the 1940s, it is often assumed that saltation is homogeneous, i.e., saltating particles are uniform in size and follow identical trajectories. This assumption is a limitation to the development of saltation theory. In this paper, as in some other studies made since the 1980s, we are concerned with the saltation of multi-sized particles in turbulent flows, a process that we refer to as heterogeneous saltation. The theory deals with several questions, including the variation of particle size distribution with height, the entrainment rates of particles in different size ranges, and the associated profiles of saltation flux, particle momentum flux and particle concentration. It is hypothesised that saltation is dynamically similar and ‘universal’ similarity functions can be established. The similarity function for saltation flux is presented. Field observations are carried out at the southern fringe of the Takla Makan Desert in April 2002. Measurements of streamwise saltation flux of 32 particle size groups are made using a sand particle counter, together with measurements of wind speed and other atmospheric variables. These data are used to validate the saltation theory, by examining whether the observed saltation flux and particle size distribution can be reproduced. It is shown that the theory is promising in predicting these quantities.  相似文献   

14.
15.
The mean flow profile within and above a tall canopy is well known to violate the standard boundary-layer flux–gradient relationships. Here we present a theory for the flow profile that is comprised of a canopy model coupled to a modified surface-layer model. The coupling between the two components and the modifications to the surface-layer profiles are formulated through the mixing layer analogy for the flow at a canopy top. This analogy provides an additional length scale—the vorticity thickness—upon which the flow just above the canopy, within the so-called roughness sublayer, depends. A natural form for the vertical profiles within the roughness sublayer follows that overcomes problems with many earlier forms in the literature. Predictions of the mean flow profiles are shown to match observations over a range of canopy types and stabilities. The unified theory predicts that key parameters, such as the displacement height and roughness length, have a significant dependence on the boundary-layer stability. Assuming one of these parameters a priori leads to the incorrect variation with stability of the others and incorrect predictions of the mean wind speed profile. The roughness sublayer has a greater impact on the mean wind speed in stable than unstable conditions. The presence of a roughness sublayer also allows the surface to exert a greater drag on the boundary layer for an equivalent value of the near-surface wind speed than would otherwise occur. This characteristic would alter predictions of the evolution of the boundary layer and surface states if included within numerical weather prediction models.  相似文献   

16.
17.
Wind profiles,momentum fluxes and roughness lengths at Cabauw revisited   总被引:1,自引:1,他引:1  
We describe the results of an experiment focusing on wind speed and momentum fluxes in the atmospheric boundary layer up to 200 m. The measurements were conducted in 1996 at the Cabauw site in the Netherlands. Momentum fluxes are measured using the K-Gill Propeller Vane. Estimates of the roughness length are derived using various techniques from the wind speed and flux measurements, and the observed differences are explained by considering the source area of the meteorological parameters. A clear rough-to-smooth transition is found in the wind speed profiles at Cabauw. The internal boundary layer reaches the lowest k-vane (20 m) only in the south-west direction where the obstacle-free fetch is about 2 km. The internal boundary layer is also reflected in the roughness lengths derived from the wind speed profiles. The lower part of the profile (< 40 m) is not in equilibrium and no reliable roughness analysis can be given. The upper part of the profile can be linked to a large-scale roughness length. Roughness lengths derived from the horizontal wind speed variance and gustiness have large footprints and therefore represent a large-scale average roughness. The drag coefficient is more locally determined but still represents a large-scale roughness length when it is measured above the local internal boundary layer. The roughness length at inhomogeneous sites can therefore be determined best from drag coefficient measurements just above the local internal boundary layers directly, or indirectly from horizontal wind speed variance or gustiness. In addition, the momentum and heat fluxes along the tower are analysed and these show significant variation with height related to stability and possibly surface heterogeneity. It appears that the dimensionless wind speed gradients scale well with local fluxes for the variety of conditions considered, including the unstable cases.  相似文献   

18.
In wind tunnel studies of aeolian transport, the number and position of pitot tubes are decided by the researcher, so that there are important variations in the computation ofU * between studies. Velocity measurements seldom are made very close to mobile surfaces because the tubes become blocked by drifting sand grains. This practice is fortuitous as demonstrated by recent selfregulatory models of saltation which indicate that fluid and grain-borne shear stress vary substantially within the lowest 0.01 m and application of the logarithmic law is therefore unsound. This study reports detailed velocity measurements which further suggest that no single logarithmic expression, based on fixed values of κ and τ, adequately represents the full wind profile which includes the inner saltation cloud above 0.01 m and the outer grain-free region of the boundary layer. A much improved fit over the logarithmic wind profile model is achieved with a square root relation, although there is no known physical basis for this specific form of power model. Relatively shallow boundary-layer development in wind tunnels forces the velocity gradient above the region of momentum extraction to attain exceptionally large values, uncommon in natural settings.  相似文献   

19.
The effects of sea-surface waves and ocean spray on the marine atmospheric boundary layer(MABL) at different wind speeds and wave ages were investigated. An MABL model was developed that introduces a wave-induced component and spray force to the total surface stress. The theoretical model solution was determined assuming the eddy viscosity coefficient varied linearly with height above the sea surface. The wave-induced component was evaluated using a directional wave spectrum and growth rate. Spray force was described using interactions between ocean-spray droplets and wind-velocity shear. Wind profiles and sea-surface drag coefficients were calculated for low to high wind speeds for wind-generated sea at different wave ages to examine surface-wave and ocean-spray effects on MABL momentum distribution. The theoretical solutions were compared with model solutions neglecting wave-induced stress and/or spray stress. Surface waves strongly affected near-surface wind profiles and sea-surface drag coefficients at low to moderate wind speeds. Drag coefficients and near-surface wind speeds were lower for young than for old waves. At high wind speeds, ocean-spray droplets produced by wind-tearing breaking-wave crests affected the MABL strongly in comparison with surface waves, implying that wave age affects the MABL only negligibly. Low drag coefficients at high wind caused by ocean-spray production increased turbulent stress in the sea-spray generation layer, accelerating near-sea-surface wind. Comparing the analytical drag coefficient values with laboratory measurements and field observations indicated that surface waves and ocean spray significantly affect the MABL at different wind speeds and wave ages.  相似文献   

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