塔克拉玛干沙漠腹地湍流能量耗散率和结构函数参数特征

利用塔中气象站垂直探测系统的湍流观测资料,计算并分析了塔克拉玛干沙漠腹地不同稳定层结条件的湍涡特征长度尺度、能量耗散率及湍流结构函数参数特征。结果表明：湍涡特征长度尺度在弱不稳定或近中性条件时最大,随不稳定程度的增强有明显减小的趋势,随着稳定程度的增加有先迅速减小后又缓慢增加的趋势,且热量特征长度尺度比动量特征长度尺度总体要大一个数量级;无因次湍流热量耗散率的拟合函数形式与其他试验一致,但经验系数略有差异;利用Kaimal公式和湍流谱方法间接计算的稳定条件湍流能量耗散率及湍流结构函数参数具有较好的一致性。     

巴丹吉林沙漠北缘拐子湖流沙下垫面近地层湍流强度和陆面过程特征

利用巴丹吉林沙漠北缘拐子湖流沙下垫面2013年7、10月和2014年1、4月的湍流通量资料，计算并分析了研究区近地层湍流强度，同时针对风速分量、温度、水汽和CO₂归一化标准差随稳定度的变化关系和总体输送系数等陆面过程特征进行分析。结果表明：（1）风速各分量的湍流强度均随风速的增加逐渐减小，风速处于2 m·s^-1以下时湍流发展最为旺盛。湍流强度主要由水平方向风速分量决定，垂直方向风速的作用较小，且近中性和不稳定层结利于湍流的发展。与其他地区相比，平坦且没有建筑物的沙漠地区，机械湍流较弱，湍流强度相应较小。（2）风速各分量的归一化标准差与稳定度（z/L）均满足1/3次方函数规律，其中垂直方向风速分量的拟合曲线方程较好。（3）动量输送系数C_d具有明显的夏季高、冬季低的变化状态且各月的日变化形态均呈夜间低、日间高的循环形态。热量输送系数C_h的不同月份日变化间并没有明显的排列次序，且日出日落前后具有明显的波动。不稳定层结时，C_d和C_h均随风速的增加逐渐减小；稳定层结时，C_d和C_h均随着风速的增加逐渐上升。     

沙漠腹地春夏季近地层大气湍流特征观测分析

利用塔克拉玛干沙漠腹地近地层10 m高度处快速响应探测系统的湍流资料,分析了摩擦速度和特征温度的变化,并且对不同稳定层结条件下无因次速度分量方差和无因次温度方差的普适函数进行详细拟合。研究表明,摩擦速度和特征温度有明显的日变化特征,且摩擦速度的最大值出现在z/L=-0.2处;无因次速度方差在不稳定和稳定层结条件下均符合相似理论的次幂律,但如果考虑到相关性,最佳幂指数可有不同;近中性时则接近常数,并给出了具体数值。无因次温度方差则在夏季不稳定层结条件时符合-1/3次幂律。     

塔克拉玛干沙漠夏季晴空对流边界层大涡模拟

为了探索塔克拉玛干沙漠夏季晴空对流边界层湍流结构和热对流运动规律,利用沙漠腹地探空及地表通量观测资料,开展了晴空对流边界层的大涡模拟研究。结果表明：（1）沙漠夏季晴空条件下,对流边界层湍能主要由地表热力浮力对流产生,机械剪切对边界层湍能的贡献较小,小尺度湍涡对湍能的耗散随高度呈减弱趋势,边界层湍能变化呈现间歇性特点。（2）沙漠夏季晴空边界层中存在着有组织的热对流泡现象,热泡最大上升速度可超过4.0 m·s^-1;沙漠热对流运动一般呈羽状和网状分布特征,在上升运动区周围伴随有大片的下沉辐散区域。（3）地表感热和逆温层顶盖强度是控制和影响沙漠对流边界层发展的两个重要因素,感热增大,对流边界层变暖且高度升高;感热减小,对流边界层变冷且高度降低。在感热不变的条件下,逆温层顶盖强度越强,越不利于对流边界层发展,反之则相反。     

塔克拉玛干沙漠腹地近地层湍流能谱特征分析

利用塔克拉玛干沙漠腹地近地层湍流观测资料,计算并分析了不同稳定层结条件的湍流速度谱、温度谱及局地各向同性特征。结果表明,湍流速度谱和温度谱在惯性副区均满足Kolmogorov的-2/3指数规律,且稳定条件的相关系数更高;速度谱满足湍流各向同性的低频限制理论。近中性条件的温度谱和弱不稳定条件的速度谱在高频段有尾部上翘现象;稳定情况下的v谱和近中性条件的u谱、T谱在低频处也有上翘现象。沙漠腹地水平湍流尺度范围介于森林和草地之间,不稳定层结比稳定层结的谱峰更偏向低频端,且峰值尺度更大。     

塔克拉玛干沙漠北缘夏季典型晴天近地层湍流能谱特征

利用塔克拉玛干沙漠北缘肖塘地区涡动相关系统三维方向风速（u，v，w）、气温、CO₂、H₂O等观测数据，分析了夏季典型晴天不同大气稳定度条件下湍流功率谱和协谱。结果表明：大部分情况下湍流速度谱分布满足-2/3幂指数率，垂直方向高频段惯性副区符合程度更高，水平方向次之；CO₂和H₂O浓度则符合程度较低；温度谱与无因次频率总体上都具有很好的相关性。垂直风速与径向风速u的协谱斜率拟合值大多数情况下更接近-1，而在近中性层结条件下更符合-4/5斜线。稳定层结条件下的协谱峰值比不稳定层结时更大，且约大一个量级；不稳定层结条件下高频段协谱近直线型下降。u谱对应的谱峰波长随稳定度增加而减小，v谱和T谱对应的谱峰波长随稳定度的增加没有规律性增减；u、v、w、T谱谱峰波长约67~827、69~2417、4~54、12~661 m。     

南疆一次强沙尘暴的近地层特征和湍流输送分析

利用2006年4月10日沙尘暴过境期间塔克拉玛干沙漠腹地80 m垂直梯度探测系统的实时资料,分析了该地区近地面层气象要素和湍流输送特征的变化过程。结果表明,沙尘暴过境期间,近地层风速有先降低后增大的过程,10 m高度上动量向下输送明显,热量输送只有很小的上传趋势;沙尘暴过境前,近地面为弱稳定的逆温层,空气处于暖干的状态,10 m高度上垂直气流表现为系统性的下沉运动,随着沙尘暴爆发,湍流交换显著增强,空气进入相对冷湿状态,气流有上升运动趋势,但强度不大,仍以水平湍能为主。     

南极威德尔-斯科舍汇流区上层湍流混合特征及其与水团和环流的联系

利用中国第32次南极科学考察队于2015年12月至2016年1月在南极威德尔-斯科舍汇流区获得的湍流微结构、温盐深仪和下放式声学多普勒海流计观测资料,分析了该海域上层海洋(30～500 dbar)的湍流混合空间分布特征.结果显示,湍动能耗散率(ε)和湍扩散系数(Kρ)分布呈现明显的区域性特征,与当地的水团和环流分布密切...     

塔里木盆地南缘策勒典型下垫面水的湍流特征

基于2010年3月28日天气过程在策勒地区实测风速数据,分析戈壁、绿洲农田、灌木林三种典型下垫面3 m高度水平风速的最大脉动风速、湍流强度、阵风因子等湍流特征,结果显示:(1)近地层湍流在时间序列上具有多尺度复杂性,湍流强度、阵风因子均随分析时距增大呈对数增长;(2)以10 min为分析时距获得的各项参数都显示绿洲植被...     

南极中山站附近冰盖近地面层湍流参数的观测研究

利用2007/2008年中国第24次南极考察队在南极中山站附近冰盖上观测试验获得的湍流脉动及相关资料,对原始资料通过坐标旋转订正后,应用涡动相关法计算分析了冰盖近地面层的湍流强度(I)、稳定度参数(z/L)、摩擦速度(u*)、拖曳系数(Cd)、地表粗糙度(z0)及动量通量(τ)和感热通量(H),并与空气动力学方法的计算结果进行对比。结果表明,Louis方案能够较好地模拟近地面层湍流通量;在平均状态下,全天雪面以感热形式从大气获得净的能量;近中性层结下地表粗糙度z0为4.54×10-4m,拖曳系数Cd=1.7×10-3,在非中性条件下,稳定度越小Cd越大,反之,则稳定度越大Cd越小。     

The impact of heterogeneity of land surface roughness length on estimation of turbulent flux in model

Based on preliminary theoretical analysis and numerical experiment, it is found that land surface heterogeneity plays an important role in the models turbulent flux calculation. In nearly neutral atmosphere conditions, variation coefficient of sub-scale roughness length, cell-average roughness, and reference height are main factors affecting the calculation of grid turbulent fluxes. The first factor has a determinant role on calculation deviation. The relative error generated by roughness heterogeneity could be more than 40% in some cases in certain areas (e.g., in vegetation-climate transition belt). Selecting a specific reference height may improve the calculation of turbulent flux. In stable or unstable atmosphere conditions, with sensible heat flux as an example, analysis shows that the discrepancy is correlated to the sub-grid distributions of mean wind velocity, potential temperature gradient between land surface and reference levels, and atmosphere stability near surface layer caused by the heterogeneity of land surface roughness. The calculation of turbulent flux is the most sensitive to stability in the above three factors. The above analysis shows that it is necessary to make a further consideration for the calculation deviation of the turbulent fluxes brought from land surface heterogeneity in the present numerical models.     

Characteristics of land-atmosphere energy and turbulent fluxes over the plateau steppe in central Tibetan Plateau

The land-atmosphere energy and turbulence exchange is key to understanding land surface processes on the Tibetan Plateau(TP). Using observed data for Aug. 4 to Dec. 3, 2012 from the Bujiao observation point(BJ) of the Nagqu Plateau Climate and Environment Station(NPCE-BJ), different characteristics of the energy flux during the Asian summer monsoon(ASM) season and post-monsoon period were analyzed. This study outlines the impact of the ASM on energy fluxes in the central TP. It also demonstrates that the surface energy closure rate during the ASM season is higher than that of the post-monsoon period. Footprint modeling shows the distribution of data quality assessments(QA) and quality controls(QC) surrounding the observation point. The measured turbulent flux data at the NPCE-BJ site were highly representative of the target land-use type. The target surface contributed more to the fluxes under unstable conditions than under stable conditions. The main wind directions(180° and 210°) with the highest data density showed flux contributions reaching 100%, even under stable conditions. The lowest flux contributions were found in sectors with low data density, e.g., 90.4% in the 360° sector under stable conditions during the ASM season. Lastly, a surface energy water balance(SEWAB) model was used to gap-fill any absent or corrected turbulence data. The potential simulation error was also explored in this study. The Nash-Sutcliffe model efficiency coefficients(NSEs) of the observed fluxes with the SEWAB model runs were 0.78 for sensible heat flux and 0.63 for latent heat flux during the ASM season, but unrealistic values of-0.9 for latent heat flux during the post-monsoon period.     

Three-dimensional structure of flow at a confluence of river channels with discordant beds

This paper presents three-dimensional data of the mean and turbulent structure of flow collected at a natural confluence of rivers with discordant beds to (1) describe the three-dimensional flow field of a natural junction of channels; (2) assess the role of changes in bed morphology occurring during transport-effective events on the structure of flow at a confluence; and (3) examine how the three-dimensional structure of flow varies with changes in the ratio of momentum flux between the two confluent streams. Three-dimensional measurements of velocity were reconstructed from the measurements obtained with an array of four, two-component electromagnetic current meters. Six detailed velocity profiles were taken at five cross-sections in a wide range of flow conditions. The mean field of flow is characterised by (1) the acceleration of flow in the downstream portion of the post-confluence channel, but by lower velocities upstream in the mixing layer area; (2) a stagnation zone at the apex of the junction; (3) a zone of flow deviation, and strong fluid upwelling, close to the avalanche face and at the margin of the tributary mouth bar; and (4) reduced velocities over the depositional bar at the downstream junction corner. The position and extent of these zones vary with changes in the ratio of momentum flux. Very high intensity of turbulence (peaks up to 50%) and turbulent kinetic energy were observed in the mixing layer region. Distortion of the mixing layer, characteristic of flow where bed discordance is present between the two tributary channels, was evident from mean and turbulent flow data. This field study suggests that the effects of bed discordance on flow, sediment transport, and the resultant bed morphology must be incorporated into conceptual and numeric models of these sites of complex flow.     

塔克拉玛干沙漠腹地地表辐射与能量平衡

利用2013年塔克拉玛干沙漠塔中流动沙面地表辐射、土壤热通量、土壤温湿度和湍流通量观测资料,分析了沙漠腹地地表辐射和能量收支特征及闭合状况。结果表明：除潜热通量外,其余地表辐射各分量和能量平衡分量的月平均日变化结果整体均表现为标准的单峰型日循环形态,其中R_s↓与R_s↑变化同步,R_l↑、R_l↓滞后R_s↓0.5 ~ 1 h。各分量均表现出夏季高、春秋季次之、冬季低的季节波动性。干旱和极低的植被覆盖造成沙漠腹地全年潜热通量始终较为微弱,约占净辐射的2.8%,感热通量成为能量的主要消耗形式,约占净辐射的49%。偶尔的降水会刺激潜热通量突然增加。地表反照率相对较高且稳定,日变化呈早晚大、正午小的“U”型趋势,并具有明显的冬季高、夏季低的季节波动性,年均值0.28,月均值0.25~0.32。能量残差各月的日变化也均呈单峰曲线,日出后和日落前能量闭合程度最佳,并出现过闭合现象,全年夏季小,春秋季次之,冬季较大,月平均日峰值5.1~99.9 W·m^-2。土壤表层热储存是影响该地区能量平衡的重要因子之一,考虑表层土壤热存储后,地表能量闭合率达75.3%,能量闭合率夏季 > 春季 > 秋季 > 冬季,白天相比夜间有大幅提升。     

紊流风场中起跳沙粒的轨迹特征

运用颗粒流体二相流的随机行走扩散模型(DRW)研究了紊流风场下起跳沙粒的运动轨迹特性。得出了轨迹特性(长度、高度、撞击角)随沙粒的大小和风速的变化规律,发现随沙粒粒径的减小紊流脉动对轨迹的影响显著增大。粒径在200μm以下时,紊流风场下计算得的轨迹形状与平均风场下得到的轨迹有明显差异。