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1.
Sonic anemometers in aeolian sediment transport research 总被引：3，自引：0，他引：3
Fast-response wind and turbulence instruments, including sonic anemometers, are used more and more in aeolian sediment transport research. These instruments give information on mean wind, but also on fluctuations and turbulent statistics, such as the uw covariance, which is a direct measure of Reynolds' stress (RS) and friction velocity. This paper discusses the interpretation of sonic anemometer data, the transformations needed to get proper results and turbulence spectra, and how they are influenced by instrument size, sampling frequency, and measurement height.Turbulence spectra characterize how much the different frequencies in the turbulent signals contribute to the variance of wind speed, or to the covariance of horizontal and vertical wind speed. They are important in determining the measurement strategy when working with fast-response instruments, such as sonic anemometers, and are useful for interpreting the measurement results. Choices on the type of sonic anemometer, observation height, sampling period, sampling frequency, and filtering can be made on the basis of expected high and low-frequency losses in turbulent signals, which are affected by those variables, as well as wind speed and atmospheric stability.Friction velocity and RS, important variables in aeolian sediment transport research, are very sensitive to tilt or slope errors. During a field experiment, the slope sensitivity of the RS was established as 9% per degree of slope, which is 1.5 times the value reported in literature on the basis of theoretical considerations. An important reason for the difference probably is the large influence of streamline curvature on turbulence statistics and thereby on the slope sensitivity of the RS. An error of 9% per degree of slope in the RS will translate into an error of approximately 4% per degree of slope in the calculated friction velocity.Space–time correlation of the horizontal wind speed is much larger than that of the vertical wind speed and the instantaneous RS. This largely explains why, in previous studies, a poor correlation was found between instantaneous RS measured at 3 m height and saltation flux near the surface, whereas the correlation between wind speed at some height and saltation flux was much better. Therefore, the poor correlation between RS away from the surface and saltation flux does not contradict that saltation flux is caused by RS. 相似文献
2.
Studies of interactions between wind and saltating particles （i.e., the wind-saltation interaction） are usually conducted without consideration of the downwind air pressure gradient. However, in a wind tunnel with limited size, this gradient is required to maintain the movement of the saltation cloud. Attempts are made to investigate the effects of the downwind air pressure gradient on the wind-saltation interaction in a saltation boundary layer based on the experimental results from a wind tunnel with a relatively small cross-sectional area. The wind-saltation interaction is characterized by airborne stress, grain-borne stress, and the force exerted on the wind by the saltation cloud. Basic equations were developed for wind-saltation interactions without and with a downwind air pressure gradient. The results reveal that unacceptable values of negative grain-borne stress and negative force exerted on the wind by the saltation cloud are obtained if the downwind air pressure gradient is ignored. When this air pressure gradient is defined using the measured wind velocity profiles in the presence of saltation and the downwind air pressure gradient is taken into account, reasonable values for grain-borne stress and the force exerted on the wind by the saltation cloud are obtained. These results suggest that attention must be paid to the effects of downwind air pressure gradients when studying the wind-saltation interaction in a wind tunnel. Consideration of the downwind air pressure gradient, inertial forces, and other unidentified variables will provide a more thorough understanding of the interactions within a saltation boundary layer. 相似文献
3.
跃移质作为风沙流的主体,其近地表垂直分布规律是风沙物理学的重要研究内容,对防沙工程具有重要的指导意义。受研究条件与观测仪器限制,戈壁特别是极端大风区近地表风沙流结构特性研究较为薄弱。利用多梯度风蚀传感器与阶梯式集沙仪对兰新高铁烟墩风区戈壁近地表风沙流跃移质的垂直分布特性进行了观测研究。结果表明：兰新高铁烟墩风区戈壁沙粒发生跃移运动的2 m高临界风速达12 m·s-1;戈壁近地表风沙流具有明显的阵性特征,沙粒跃移发生的时间比例在50%以下,与平均风速成正相关关系,与风速脉动强度无显著相关关系;2 m高阵风7级风速下,戈壁跃移沙粒主要集中于地表50 cm范围内,近地表风沙流结构呈"象鼻效应",跃移质最大质量通量出现在地表2.5~5 cm高度处,沙粒最大跃移高度可达2 m,且沙粒跃移高度随2 m高风速的增加呈指数规律递增。因此,兰新高铁烟墩风区2 m高阻沙栅栏不足以完全阻截戈壁风沙流,是造成烟墩风区兰新高铁轨道积沙的重要原因之一。 相似文献
4.
库布齐沙漠南缘抛物线形沙丘表面风沙流结构变异 总被引：5，自引：0，他引：5
对库布齐沙漠南缘抛物线形沙丘表面气流和输沙率的野外观测和分析结果表明,沙丘表面约90%的风沙输移集中在距沙面0.10 m高度范围内,输沙率随高度递减的形式在沙丘各部位因风速、下垫面状况和坡面形态不同而发生变异。沙丘迎风坡坡脚因出露坚硬、含砾石地表,颗粒跃移高度大,风沙流上层相对输沙率大;迎风坡沙粒沿坡向上运动,颗粒跃移高度减小,风沙流中近地表相对输沙率大;沙丘背风坡沙粒沿坡向下运动,加之来自丘顶变型跃移物质的影响,风沙流上层相对输沙率较大;脊线受迎风坡各个断面地形差异的影响,各观测点间风沙流结构差异显著。风沙流结构在迎风坡和丘顶均遵循指数递减规律(Q=aexp(-z/b)),其中,指数函数拟合中系数a与输沙率具有良好的幂函数关系,随风速增加而增加,但二者关系较弱;b与二者无相关性。背风坡风沙流结构具有明显的分段现象,以0.10 m高度为界,下层符合指数函数,上层符合幂函数。 相似文献
5.
The vertical distribution of the wind-blown sand flux in a 40-cm flow layer above the ground surface was investigated through laboratory wind-tunnel tests and field measurements on the mobile dune surface during sand storms in the Taklamakan Desert of China. Results show that vertical distribution of the horizontal mass flux of drifting sand is a discontinuous function of height. More than 90% of the total material is transported in the flow layer from the surface to 14 cm. From 2 to 4 cm above the surface, a distinct transition zone occurs wherein mixed transport by creep, saltation, and suspension becomes saltation and suspension. The flow layer from 14 to 15 cm represents a further transition from saltation to suspension, where the distribution curves of the transport rate against height converge. The basic natural exponential function cannot describe well the vertical distribution of the saltation mass flux in the Taklamakan Desert. As a function of height, saltation mass flux follows a function qsalt = a'Z-bZ, and the distribution of suspension mass flux fits the power function very well. A total transport rate from surface creep to saltation and suspension in the measured flow layer, which is directly proportional to the effective wind speed squared (V - Vt)2, can be predicted by integrating Q = a'Z-bZ + cZ-d. The height distribution of the average quantities of transported materials varies as an exponential function of wind speed, and deceases with the increase in total transport quantity. Higher wind speed results in a higher transport rate and a higher vertical gradient for the particle concentration. The increment of relative transport quantity in the higher flux layer increases as wind speed increases, which generates a higher concentration of drifting particles in the upper flow layer. [Key words: aeolian geomorphology, aeolian transport, horizontal sand flux, sand dune, vertical sediment distribution, Taklamakan Desert.] 相似文献
6.
7.
Wind erosion of soil is an appreciable but unstudied event following fires in cold desert. We examined aeolian transport of sediment for 1 year following fire in semi-arid shrub steppe on loess soils in southern Idaho, USA. Sediment collectors were used to determine horizontal mass transport of soil and saltation sensors and anemometers were used to determine saltation activity (fraction of time having saltation) and threshold wind speed in an area burned in August and an unburned control site. Horizontal mass transport (per 30-day period) was negligible in the unburned area, but in the burned area was 5.40 kg m?1 in October and decreased to 2.80 kg m?1 in November and 0.32 kg m?1 in December. Saltation activity was high enough to determine threshold wind speeds only in the burn site during fall, when values ranged from 10.0 to 10.6 m s?1. Sediment flux and saltation activity in the burned site became much less pronounced following the emergence of herbaceous vegetation in the spring. Post-fire sediment flux in the shrub steppe we examined was of greater magnitude but shorter duration than post-fire fluxes in warm deserts or sandier regions that experience more frequent wind erosion. 相似文献
8.
Analysis of velocity profile measurements from wind-tunnel experiments with saltation 总被引：6，自引：0，他引：6
Investigations of wind-field modification due to the presence of saltating sediments have relied heavily on wind tunnels, which are known to impose geometric constraints on full boundary layer development. There remains great uncertainty as to which portion of the vertical wind-speed profile to analyze when deriving estimates of shear velocity or surface roughness length because the lower sections are modified to varying degree by saltation, whereas the upper segments may be altered by artificially induced wake-like effects. Thus, it is not obvious which of several alternative velocity-profile parameterizations (e.g., Law of the Wall, Velocity Defect Law, Wake Law) should be employed under such circumstances.A series of experimental wind-tunnel runs was conducted across a range of wind speed using fine- and coarse-grained sand to collect high-quality, fine-resolution data within and above the saltation layer using thermal anemometry and ruggedized probes. After each run, the rippled bottom was fixed with fine mist, and the experiment repeated without saltation. The measured wind-speed profiles were analyzed using six different approaches to derive estimates of shear velocity and roughness length. The results were compared to parameter estimates derived directly from sediment transport rate measurements, and on this basis, it is suggested that one of the six approaches is more robust than the others. Specifically, the best estimate of shear velocity during saltation is provided by the logarithmic law applied to the profile data within about 0.05 m of the bottom, despite the fact that this near-surface region is where profile modification by saltating sediments is most pronounced. Uncertainty remains as to whether this conclusion can be generalized to field situations because progressive downwind adjustments in the interrelationship between the saltation layer and the wind field are anticipated in wind tunnels, thereby confounding most analyses based on equilibrium assumptions. 相似文献
9.
为了研究沙丘迎风坡面上沙粒的跃移运动,本文根据风工程和空气动力学的最新理论,给出了沙丘迎风坡面上风场的空间分布规律,在此基础上对沙粒跃移运动进行了数值计算。由于沙丘周围流场情况较为复杂,各处的风速廓线也不同,故选取不同的坡面位置进行跃移计算,其中各处的起沙率由已有的实验结果或拟合公式给出。计算结果表明：从坡脚到坡顶,平均风速加速比和摩阻风速逐渐增加,到沙丘顶部达到最大值;同时沿坡面向上,各截面处单宽输沙率和距离当地地面相同高度处输沙浓度逐渐加强,这与已有文献报道的结果吻合良好。 相似文献
10.
风沙流输沙通量垂向分布研究
——以塔克拉玛干沙漠南缘流沙地表风沙流观测为例 总被引：1，自引：0，他引：1
于2010年4—6月在塔克拉玛干沙漠南缘策勒绿洲外缘流沙地进行风速、风向和输沙量同步观测,利用观测到的28组数据对输沙通量的垂向分布进行研究。结果表明,在4.5～8 m·s-1的风速区间内,总输沙率随风速增长速率较慢,大于8 m·s-1时增长迅速。在较小风速时,4个高度层(1 cm、3 cm、9 cm和19 cm)的输沙比率变化不明显,当风速大于6.6 m·s-1时,1 cm和19 cm高度输沙比率的调整较为明显,前者减小而后者增加,中间两层(3 cm、9 cm)则维持一定波动。不同的蚀积条件对于输沙通量的垂向分布具有一定的影响,平均跃移高度则在一定程度上反映了地表沙粒的吹蚀和堆积过程。在4种常见的描述输沙通量垂向分布的模型中,Zingg的修正幂函数具有最好的拟合程度,但反映的风沙流信息最少,简单幂函数的参数包涵了最为丰富的风沙流信息但拟合程度最差,指数函数同时具有较好的拟合程度和参数意义,Fryrear的幂函数则与指数函数恰恰相反。在沙物质以极细沙为主的塔克拉玛干沙漠南缘,指数函数较之简单幂函数能更好地描述该区域输沙通量的垂向分布,验证并补充了风洞实验的结果。综合比较认为,指数函数能更好地描述塔克拉玛干沙漠南缘输沙通量的垂向分布。 相似文献
11.
海岸湿沙表面风沙传输特征的风洞实验研究 总被引：4，自引：2，他引：2
通过湿沙表面风沙传输的风洞实验,研究了湿润海岸风沙流的垂直结构、输沙率随风速与表层湿度的变化规律。输沙测量使用60 cm高直立式积沙仪,湿度（M）为沙面表层1 mm厚的重量湿度值。结果表明,湿沙表面的输沙量和高度呈指数关系。一般,湿度增大,整体输沙率降低,高湿度床面的沙粒有相对更大的比例被传输到更高的位置。比起低湿度（M＜0.587%）沙粒,高湿度（0.587%＜M＜1.448%）沙粒的垂直运动对湿度变化的影响更加敏感,尤其是在跃移层的底部,当M＞1.448%时,输沙率已经很低,小于0.99 g·cm-1·s-1。伴随湿度0.587%和1.448%的过渡,风沙流垂向分布被分为3个不同坡度的区域,曲线坡度反映了沙粒间不同水分存在形式的影响差异。对于跃移沙粒,高湿度表面（M＞1.448%）仅起到了一个传输平台的作用;当表面变干到某种程度（M=0.587%）之前,表面湿度是跃移运动的主要控制因子,然后风速才重新开始影响输沙。 相似文献
12.
采用有限体积法模拟了风速正弦变化下的一维非平稳跃移风沙流发展过程。考虑风沙流跃移系统的4个子过程,沙粒的流体起动、沙粒的运动、击溅过程和沙粒对风场的反作用。给出在风速正弦变化时,风速变化频率和振幅对于沙粒输运的影响以及输沙率、风速廓线、床面剪切应力以及起跳沙粒数的变化规律。结果表明,输沙率随着振幅增大而增大,随着周期增大而减小;在初始的overshoot现象之后,床面剪切应力变化很小,但起跳的沙粒数随风速呈现类正弦周期变化。 相似文献
13.
乌兰布和沙漠东北缘地表风沙流结构特征 总被引：13，自引：4，他引：9
在国家林业局磴口荒漠生态站长期监测的基础上,利用多种积沙仪,对乌兰布和沙漠东北缘流动沙丘、油蒿半固定沙丘、白刺半固定沙丘、油蒿固定沙丘、白刺固定沙丘5种典型下垫面近地面（0～100 cm）的风沙流输沙量进行了实地观测和对比分析。结果表明：（1） 输沙率（q）随高度（h）增加呈幂函数（q=ah-b,R2≥0.8409）规律衰减,随风速（v）增大呈幂函数（q=avb,R2≥0.9256）规律增加,42.8%～70.7%的输沙量分布在10 cm高度内,67.6%～90.0%的输沙量分布于30 cm高度内。当地表植被盖度达到40%以上时,输沙率下降至无植被覆盖地表输沙率的6.6%以下,可有效阻止地表风蚀。（2） 沙物质主要由粒径为50～250 μm的细沙和极细沙构成,各高度层风蚀物粒度组成服从单峰态分布,峰值在100～250 μm。随高度增加,风蚀物粒径范围趋于变窄,粒径趋于更细。（3） 起沙风多出现在WSW和NW方向,占全年起沙风的53.19%。风沙流中跃移输沙、蠕移输沙的空间分布在理论上应与风向频率分布基本一致,差异性主要由各方位风的强度和持续时间等因素导致。研究结果可为该区域防沙工程设计提供理论参考。 相似文献
14.
海岸风沙流中不同粒径组沙粒的垂向分布模式 总被引：4，自引：1，他引：3
通过对河北昌黎黄金海岸沙丘风沙流的野外实地观测与室内风洞模拟实验数据的数值模拟,探讨了我国典型海岸沙丘风沙流中不同粒径组沙粒输沙量的垂向分布模式。结果表明,河北昌黎黄金海岸沙丘表面风沙流中不同粒径组沙粒输沙量的垂向分布特征并不一致,其中细沙和中沙符合典型的指数递减分布规律,但粗沙则为负幂函数分布。究其原因,主要与不同粒径组沙粒输沙量的分布高度及运动方式差异有关。在实际非均匀沙床面上,粗沙主要集中分布于沙丘表面4cm高度内湍流发育的近地表层,运动方式以蠕移为主,沙丘表面湍流的主导作用使其输沙量随高度的变化满足负幂律关系,但中沙和细沙则以跃移运动为主,跃移沙粒输沙量的垂向分布呈现指数递减特征。 相似文献
15.
The vertical distributions of grain-size parameters of drifting sand flux during sand storms in the Taklamakan Desert, Central Asia, were investigated through field observation and laboratory wind-tunnel tests. The results show that grain-size parameters of the drifting sands near the ground surface are similar to those of the source deposits. Fine and very fine sands in the flux layer near the ground surface (from zero to 20 cm high) comprise more than 85% of the sample's weight, with a mean diameter of 0.09 mm. The distributions of transported particles are mainly negatively skewed, with good sorting. The creep population consists of poorly sorted coarser particles. In the saltation layer, particle size becomes finer as a power function of height from 4 to 14 cm. Sorting in the saltation layer is good and improves as a logarithmic function of height. The higher the transport layer, the more negatively skewed the particle distribution becomes as a logarithmic function of height. It becomes more leptokurtic as a power function of height in the transport layer from zero to 12 cm high. Grain-size parameters change irregularly at heights above 14 cm. Regional differences in the vertical distribution of grain-size compositions are affected by source deposits, wind speeds, and transport rates, but source has more influence on the sorting of the drifting material than wind velocity. 相似文献
16.
基于风沙流实时测量系统对流沙地表的输沙强度以及不同高度风速进行实时测量所获得的数据,分析野外实际风场中的风沙流脉动特征。结果表明:沙粒的存在削弱平均流场,但对风速的高阶统计矩和分布形式影响不大,不同高度、不同来流平均风速条件下,风沙流中风速仍近似符合高斯分布;瞬时输沙强度服从指数分布,滞后风速约1 s,脉动强烈;30 min输沙强度平均值和脉动标准差均随平均风速的增大而呈幂函数增加,但随风速脉动强度的变化呈先增大后减小的趋势。这意味着脉动风速对输沙率具有重要影响,需要在输沙率预测公式中予以考虑。 相似文献
17.
Sand velocity in aeolian sand transport was measured using the laser Doppler technique of PDPA (Phase Doppler Particle Analyzer) in a wind tunnel. The sand velocity profile, probability distribution of particle velocity, particle velocity fluctuation and particle turbulence were analyzed in detail. The experimental results verified that the sand horizontal velocity profile can be expressed by a logarithmic function above 0.01 m, while a deviation occurs below 0.01 m. The mean vertical velocity of grains generally ranges from − 0.2 m/s to 0.2 m/s, and is downward at the lower height, upward at the higher height. The probability distributions of the horizontal velocity of ascending and descending particles have a typical peak and are right-skewed at a height of 4 mm in the lower part of saltation layer. The vertical profile of the horizontal RMS velocity fluctuation of particles shows a single peak. The horizontal RMS velocity fluctuation of sand particles is generally larger than the vertical RMS velocity fluctuation. The RMS velocity fluctuations of grains in both horizontal and vertical directions increase with wind velocity. The particle turbulence intensity decreases with height. The present investigation is helpful in understanding the sand movement mechanism in windblown sand transport and also provides a reference for the study of blowing sand velocity. 相似文献
18.
《Journal of Arid Environments》1998,39(3):395-401
A fundamental feature of any wind-eroding surface is its threshold — the lowest wind speed (or friction velocity) at which soil movement is initiated. Many theoretical equations and numerical models of the saltation process include threshold as an important basic parameter. The question addressed here is whether or not the averaging time of a wind speed measurement affects the observed wind speed threshold. Using wind speed data taken at 1 Hz and simultaneously measuring saltation activity with a piezoelectric saltation sensor it was possible to calculate threshold. Threshold was then recalculated using the same data set averaged over periods of 2, 5, 10, 20, 30, and 60 s. The results reveal that, under typical field conditions with gusty turbulent winds, long averaging times produce an apparent threshold that is considerably lower than the true wind speed at which saltation is initiated. This result suggests that high-frequency sampling of wind speed and saltation activity is critical to the accurate determination of the true threshold of a wind-eroding surface. 相似文献
19.
考虑沙粒带电情形下的单宽输沙率经验公式 总被引：1，自引：0，他引：1
单宽输沙率是风沙流研究的一个重要参数。基于考虑跃移运动沙粒带电的风沙流演化过程理论模型,对单宽输沙率进行了大量详细的数值模拟,在此基础上,拟合得到一个便于实际应用的单宽输沙率经验公式。该公式包含来流风速、沙粒粒径和平均荷质比等影响风沙流演化过程的重要可测参数。与已有模型相比较发现,通过对公式中参数沙粒荷质比赋予（-160 μc·kg-1, 0 μc·kg-1）范围内的值,预测的输沙率与现有许多输沙率预测公式的预测结果都能符合,意味着静电作用可能是导致众多输沙率公式预测结果不统一的原因之一。 相似文献
20.
Based on the sand dust storms data and climatic data in 12 meteorological stations around sand dust storm originating areas of the Taklimakan Desert, we analyzed the trends of the number of dust storm days from 1960 to 2005 as well as their correlations with temperature, precipitation, wind speed and the number of days with mean wind speed ≥ 5 m/s. The results show that the frequency of dust storm events in the Taklimakan region decreased with the elapse of time. Except Ruoqiang and Minfeng, in the other 10 meteorological stations, the frequency of dust storm events reduces, and in 4 meteorological stations of Kuqa, Korla, Kalpin and Hotan, the frequency of dust storm events distinctly decreases. The temperature has an increasing trend, while the average wind speed and the number of days with mean wind speed ≥ 5 m/s have decreasing trends. The correlation analysis between the number of days of dust storms and climatic parameters demonstrates that wind speed and the number of days with mean wind speed ≥ 5 m/s have strong positive correlation with the number of days of dust storms, with the correlations coefficients being 0.743 and 0.720 (p<0.01), respectively, which indicates that strong wind is the direct factor resulting in sand dust storms. Whereas precipitation has significant negative correlation with the number of days of dust storms (p<0.01), and the prior annual precipitation has also negative correlation, which indicates that the prior precipitation restrains the occurrence of sand dust storms, but this restraining action is weaker than the same year’s precipitation. Temperature has negative correlation with the number of dust storm days, with a correlations coefficient of –0.433 (p<0.01), which means that temperature change also has impacts on the occurrence of dust storm events in the Taklimakan region. 相似文献