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1.
北极斯瓦尔巴德地区近地层大气观测研究Ⅱ.湍流场特征   总被引:4,自引:0,他引:4  
利用"中国科学探险协会2002年北极科学探险考察"期间在北极朗伊尔宾地区获得的大气风温微气象脉动资料,讨论了该地区近地层湍流能谱、湍流方差、感热通量、动量通量、温度结构参数以及动量整体输送系数等的分布规律,给出了这一极端环境区夏季近地层微气象场的基本结构,分析了北极地区极昼期间陆地下垫面地-气之间能量交换,丰富了人们对该地区近地层湍流输送过程的深入理解.  相似文献   

2.
台风“珍珠”登陆期间动量通量的多尺度分析   总被引:2,自引:1,他引:1  
利用台风"珍珠"登陆前后的近地层湍流观测资料,分析了该台风经过观测场地前后地面气象要素的变化及其动量通量特征。结果表明,台风"珍珠"经过观测场地前后的近地层气象要素发生了急剧的变化,并且在台风前部存在强的中尺度对流系统,反映在风速能谱密度结构上,频率f在3×10-4~2×10-3Hz之间的中尺度信号对能谱的贡献比平稳天气形势下的能谱贡献大很多,尤其是顺风方向风速的能谱密度的峰值与湍流信号的峰值相当;动量通量分析结果表明,台风中心经过观测场地的前后三小时,近地层通量以向下输送的中尺度通量为主,湍流通量的贡献相对于中尺度通量较小,也是向下输送的;而在其他时段,近地层通量主要以向上输送的湍流通量为主,中尺度通量量值很小,可以忽略。  相似文献   

3.
沙漠地区沙尘天气近地层湍流输送特征分析   总被引:12,自引:3,他引:12  
利用1996-04-20-50-10在内蒙古自治区吉兰泰气象站以及1997-04-05-27在内蒙古自治区阿拉善右旗气象站观测到的风,温,湿廓线资料,应用空气动力学方法,计算了每天各观测时次的流动量通量,湍流感热通量和湍流潜热通量,并且比较分析了荒漠下垫面不同沙尘天气状况下的湍流动量通量,感热通量和潜热通量的日变化。结果表明,在沙漠地区春季无降水天气状况下,晴空条件下,白天热力湍流基于动力湍流,在近地层最重要的物质交换是湍流感热交换,浮尘天气条件下,近地层湍流输送较晴空天气条件下弱;扬沙天气条件下,近地层湍流感热交换和湍流动力量流感热通量的峰值大于交换,并且湍流动量通量的峰值较晴空峰值大将近一个量级,湍流感热通量的峰值大于浮尘天气峰值,但小于晴空条件下峰值,沙尘暴天气条件下,湍流动量通量和感热通量一样都是最重要的湍流交换,湍流交换强于扬沙天气,强的感热对沙漠地局地性沙尘暴的产生和加强起着重要作用。  相似文献   

4.
强风天气下边界层结构特征   总被引:2,自引:0,他引:2  
近地层观测的强风运动表明,叠加在平均流动之上的脉动通常有两种,一种是随机的湍流脉动,还有一种具有相干结构的阵风扰动。分析表明,上层强风的剪切运动产生阵风,并向下传递能量,对近地层的通量传输起到重要作用。本文利用北京325 m气象塔、位于海拔1257 m的妙峰山测风塔和位于海拔1688 m的灵山测风塔的资料,分析了强风天气下,边界层上层出现阵风并向下传递的过程,进一步证实无论在近地层还是边界层上层,强风期间,叠加在平均流动上除了高频湍流脉动之外,还有周期为1~10分钟的阵风,即相干结构。阵风峰期有下沉运动,阵风谷期有上升运动。这些相干结构在边界层上层产生,向下运动和传播过程中受到平均气流梯度的切变作用和地面摩擦,破碎为湍流结构。边界层上层的阵风和湍流产生的动量通量向下传递,使得强风期间,边界层中阵风和湍流对通量具有同样的输送能力,对边界层中沙尘、污染物等气溶胶的传输具有重要作用。本研究为模式中进行通量输送参数化方案的修正提供了观测和理论依据。  相似文献   

5.
青藏高原改则地区近地层湍流特征   总被引:41,自引:4,他引:37  
刘辉志  洪钟祥 《大气科学》2000,24(3):289-300
分析了第二次青藏高原气象科学试验(TIPEX)1998年6~7月加强期在改则取得的湍流资料,讨论了近地层湍流宏观统计量、温度、湿度结构参数以及通量整体输送系数等变化规律,结果表明在不稳定层结下,湍流宏观统计量等随稳定度的变化满足过去在平原地区得到的相似关系。  相似文献   

6.
使用鄱阳湖北部70 m气象塔湍流和梯度观测数据,分析了2011年6月6日夜间一次暴雨过程中近地面边界层特征.结果表明,此次过程是在高空低槽和西南急流的天气背景下,受鄱阳湖复杂地表影响产生的局地性强降水.强降水发生前受东南暖平流影响,近地面边界层中水汽累积,不稳定性增加;强降水过程中,近地层感热、潜热通量迅速增加,同时,近地面层湍流动量通量下传和水平输送增加,鄱阳湖的水汽输送加强降水强度.另外,强降水过程中,近地面湍流动能迅速增大并达到最大值,而平均动能的增大发生在强降水结束后,表明地表作用明显,近地面边界层的湍流场为暴雨提供动力条件.尺度分析表明,强降水前,中尺度动量通量占主要地位,降水过程中湍流动量通量显著加强.  相似文献   

7.
青藏高原五道梁地区湍流输送特征的研究   总被引:25,自引:11,他引:25  
祁永强  王介民 《高原气象》1996,15(2):172-177
根据1994年6-7月在青藏高原五道梁地区的湍流脉动观测资料,分析了该地区近地层能量平衡、感热和谱热的日变化及湍流强度和端流谱特征。结果表明:晴天该地区近地层能量基本平衡,各能量分量的日变化与常情况相同;白天感热通量的输送占主导地位,潜热通量占次要地位,符合半干旱的一般特征。  相似文献   

8.
南京市近地层湍流结构及输送特征研究   总被引:8,自引:2,他引:6  
陈铭夏  李宗恺 《气象科学》2000,20(2):111-119
本文利用"城市生物气溶胶研究”中的超声风温仪观测资料,对南京市近地层大气的湍流强度、相关系数、速度谱及通量输送等进行研究,得到南京市近地层湍流结构及输送特征的一些结论.  相似文献   

9.
青藏高原改则地区近地层通量观测研究   总被引:37,自引:5,他引:32  
本研究利用首次对西藏西部改则地区大气边界层的湍流观测资料,分析了近地层动量、感热、潜热通量的变化情况,并对该地区能量收支进行了计算。最后,利用脉动资料计算了CD和CH值。  相似文献   

10.
沙尘天气过程沙地下垫面沙尘通量的获取与分析研究   总被引:9,自引:0,他引:9  
利用浑善达克沙地地区2004年春季沙尘暴和微气象学加强观测实验资料,计算了浑善达克沙地地区不同沙尘天气条件下湍流交换系数、湍流动量通量和感热通量、沙尘浓度通量;研究了沙尘暴过程中湍流作用、沙尘输送特征及起沙条件。结果显示:浑善达克沙地地区非沙尘天气白天近地层热力湍流作用强于动力湍流,湍流交换以感热交换为主;沙尘天气过程中,近地面层湍流动力作用明显增加,湍流动量和感热交换都对湍流输送有主要贡献,感热通量数值有不同程度的降低。较强沙尘暴天气过程中动力湍流强于热力湍流。随着沙尘天气经历起沙、平衡、沉降的演变过程,沙尘通量数值呈现由正值为主,过渡到向上和向下数值相当、向下数值比例增加。非沙尘天气、扬沙天气和沙尘暴天气过程的沙尘通量值范围分别是±5μg/(m2.s)、±30μg/(m2.s)和-200—300μg/(m2.s)之间。浑善达克沙地地区,非沙尘天气也存在一定量的沙尘输送,但数值较小。浑善达克沙地地区沙尘通量与摩擦速度的三次方成正比,为F=Cu3*。临界起沙风速和临界摩擦速度分别约为6m/s和0.4m/s。  相似文献   

11.
高山草甸下垫面夏季近地层能量输送及微气象特征   总被引:8,自引:5,他引:3  
李跃清  刘辉志  冯健武 《大气科学》2009,33(5):1003-1014
利用青藏高原东坡理塘站2007年6~8月的观测资料, 分析了高原东坡草甸下垫面夏季近地层气象要素和湍流通量日变化特征, 并用涡动相关法估算地面的曳力系数。结果表明: 水平风速、 动量通量、 摩擦速度等均在下午最大, 早晨最小。二氧化碳浓度表现为早晚高、 中午低的日变化特征, 比湿的最大值出现在早晨。地表辐射、 热量平衡各分量最高值出现在中午, 最低值出现在早晨。地表反照率表现出早晚高中午低的 “U” 型分布, 日平均值为0.164。夏季地面热源强度在白天午后表现为强的热源, 在夜里表现为弱的冷、 热源交替出现。夏季近地层地气热量交换中, 感热输送作用小, 潜热输送占主要地位。  相似文献   

12.
The adjustment of the boundary layer immediately downstream froma coastline is examined based on two levels of eddy correlation data collected on a mast at the shore and six levels of eddy correlation data and profiles of mean variables collected from a mast 2 km offshore during the Risø Air-Sea Experiment. The characteristics of offshore flow are studied in terms of case studies and inter-variable relationships for the entire one-month data set. A turbulent kinetic energy budget is constructed for each case study.The buoyancy generation of turbulence is small compared to shear generation and dissipation. However, weakly stable and weakly unstable cases exhibit completely different vertical structure. With flow of warm air from land over cooler water, modest buoyancy destruction of turbulence and reduced shear generation of turbulence over the less rough sea surface cause the turbulence to rapidly weaken downstream from the coast. The reduction of downward mixing of momentum by the stratification leads to smaller roughness lengths compared to the unstable case. Shear generation at higher levels and advection of stronger turbulence from land often lead to an increase of stress and turbulence energy with height and downward transport of turbulence energy toward the surface.With flow of cool air over a warmer sea surface, a convective internal boundary layer develops downstream from the coast. An overlying relatively thick layer of downward buoyancy flux (virtual temperature flux) is sometimes maintained by shear generation in the accelerating offshore flow.  相似文献   

13.
森林下垫面陆面物理过程及局地气候效应的数值模拟试验   总被引:5,自引:0,他引:5  
文中基于大气边界层和植被冠层微气象学基本原理 ,建立了一个森林植被效应的陆面物理过程和二维大气边界层数值模式。并应用该模式进行了植被和土壤含水量等生物和生理过程在陆面过程和局地气候效应方面的数值模拟试验。所得数值模拟试验结果与实际情况相吻合。结果表明 ,应用该模式可获得植被温度、植被冠层内空气温度、地表温度日变化特征 ;森林下垫面大气边界层风速、位温、比湿、湍流交换系数的时空分布和日变化特征。该模式还可应用于不同下垫面 ,模拟陆面物理过程与大气边界层相互作用机制及其局地气候效应的研究 ,这将为气候模式与生物圈的耦合研究奠定一个良好的基础。  相似文献   

14.
Based on the basic principles of atmospheric boundary layer and plant canopy micrometeorology, a forest underlying surface land surface physical process model and a two-dimensional atmospheric boundary layer numerical model are developed and numerical simulation experiments of biosphere and physiological processes of vegetation and soil volumetric water content have been done on land surface processes with local climate effect. The numerical simulation results are in good agreement with realistic observations, which can be used to obtain reasonable simulations for diurnal variations of canopy temperature, air temperature in canopy, ground surface temperature, and temporal and spatial distributions of potential temperature and vertical wind velocity as well as relative humidity and turbulence exchange coefficient over non-homogeneous underlying surfaces. It indicates that the model developed can be used to study the interaction between land surface process and atmospheric boundary layer over various underlying surfaces and can be extended to local climate studies. This work will settle a solid foundation for coupling climate models with the biosphere.  相似文献   

15.
Fluxes of aerosol particles with sizes larger than 10 nm together with fluxes of momentum, sensible and latent heat and CO2 were measured 10 m above a Scots pine forest with the eddy covariance method. During days when nucleation events were observed particle size distribution measurements showed particle growth from 3 nm sizes to the Aitken mode. Analysis of the experimental data showed systematic differences in fluxes during the days when new particle production was observed compared to other days. During the nucleation events the particle flux measurements showed downward aerosol particle transport, i.e., indicating an elevated source, with respect to the measurement level, of particles larger than 10 nm. Furthermore the turbulence intensity and the heat fluxes were observed to be significantly higher. Evidences of mesoscale circulation were observed in wind speed records as well as in turbulent fluxes on nucleation days. The measurement results show that micrometeorology, the synoptic scale conditions and the particle formation are closely related.  相似文献   

16.
夏季青藏高原低涡的能量场分析   总被引:3,自引:1,他引:3  
本文采用视热源方程,视水汽汇方程,扰动能量方程和涡度方程对1979年6月的三次低涡进行了分析和研究,得到了以下结论:在低涡生成和发展过程中,积云和乱流引起的总热量的垂直涡旋输送很大。当大气处于条件不稳定时,γs<γ<γα,积云和乱流的这种输送结果,使得低涡的正涡度增长上升到较高层次;另外,积云和乱流对总热量的垂直涡旋输送使得低涡内扰动有效位能增加,然后向扰动动能转换,使低涡得以生成和发展。  相似文献   

17.
城市建筑动力学效应对对流边界层影响的敏感性试验   总被引:3,自引:1,他引:2  
本文将大涡模拟应用于城市对流边界层(CBL)湍流结构和流场特征的研究,在大涡模式中,拖曳系数取与建筑物高度及建筑物高度标准差有关的表达式以考虑次网格建筑物对风速和湍流动能(TKE)的面积平均影响.模拟结果表明,由于城市建筑物对气流的拖曳作用,使建筑物冠层及整个CBL内风速大幅度减小,城市冠层内部风速减小尤为明显,在夹卷层内,风速有一明显的跃变.在边界层中部对流运动已经发展成为较强的热泡,城市建筑物的动力学效应使热泡的水平尺度增大,CBL内平均上升气流速度和下沉气流速度减小,同时使CBL中上升气流所占比例比平坦地面增大.城市建筑物使CBL低层热通量、动量通量、速度方差和位温方差明显增大,但对近地层高度以上的湍流量影响不大.  相似文献   

18.
Note on turbulence statistics in z-less stratification   总被引:1,自引:0,他引:1  
In boundary layer meteorology, surface layer similarity theory plays a critical role in measuring and modeling biospheric fluxes. In stable boundary layer, surface layer similarity called z-less stratification has been one of main research topics for over than two decades and the issue has yet to be settled in micrometeorology. In this scientific discussion on z-less turbulence, different turbulence statistics were used inconsistently and it was argued that z-less turbulence was valid if only any turbulence statistics were constant with different atmospheric stabilities. Consequently, such inconsistently tested turbulence statistics and misconception on z-less turbulence hinder us from correctly understanding turbulence structure in the stable boundary layer. This note revisits z-less turbulence and emphasizes that different dimensionless turbulence statistics generally do not exhibit a common behavior in the limit of z-less stratification.  相似文献   

19.
The upward transfer of heat from ocean to atmosphere is examined for an Arctic lead, a break in the Arctic ice which allows contact between the cold atmosphere and the relatively warm ocean. We employ a large-eddy model to compute explicitly the three-dimensional turbulent response of the atmosphere to a lead of 200 m width. The surface heat flux creates a turbulent plume of individual quasi-random eddies, not a continuous updraft, which penetrate into the stable atmosphere and transport heat upward.Maximum updraft velocities and turbulence occur downwind of the lead rather than over the lead itself, because the development time of an individual thermal eddy is longer than its transit time across the lead. The affected vertical region, while shallow over the lead itself, grows to a height of 65m at 600 m downwind of the lead; beyond that, the depth of the turbulent region decreases as the eddies weaken. The maximum vertical turbulent heat flux occurs at the downwind edge of the lead, beyond which a relative maximum extends upward into the plume. Negative surface heat flux immediately downwind of the lead creates a growing stable layer, but above that internal boundary layer the turbulent heat flux is still positive. Updraft maxima are typically 28 cm/s, but compensating downdrafts result in time-averaged vertical velocities of less than 1 cm/s in the plume. Conditional sampling separates the updraft and downdraft contributions. Formulas for the horizontal eddy development distance and for the vertical plume penetration height are presented. The relative importance of mean and turbulent transport is compared for both vertical and horizontal heat transfer: turbulence dominates the vertical heat transport whereas mean advection dominates the horizontal transport, these offsetting transports producing a quasi-stationary state.  相似文献   

20.
In spring preceding the record minimum summer ice cover detailed microstructure measurements were made from drifting pack ice in the Arctic Ocean, 110 km from the North Pole. Profiles of hydrography, shear, and temperature microstructure collected in the upper water column covering the core of the Atlantic Water are analyzed to determine the diapycnal eddy diffusivity, the eddy diffusivity for heat, and the turbulent flux of heat. Turbulence in the bulk of the cold halocline layer was not strong enough to generate significant buoyancy flux and mixing. Resulting turbulent heat flux across the upper cold halocline was not significantly different than zero. The results show that the low levels of eddy diffusivity in the upper cold halocline lead to small vertical turbulent transport of heat, thereby allowing the maintenance of the cold halocline in the central Arctic.  相似文献   

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