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1.
城市表面粗糙度长度的确定   总被引:10,自引:0,他引:10  
张强  吕世华 《高原气象》2003,22(1):24-32
讨论了动量粗糙度长度与热量和水汽等标量粗糙度长度在形式上和物理本质上的不同,以及造成这些不同的原因和条件,分析了决定动量粗糙度的几种因素,并给出了确定动量粗糙度长度的简化关系式,并且根据城市冠层与其上惯性次层能量和动量守衡的原因,建立了热量和水汽粗糙度与动量粗糙度之间的联系,得到了确定热量和水汽粗糙度长度的简化关系式,最后,通过数值试验,表明了动量粗糙度和标量粗糙度变化特征以及对一些主要参数的敏感程度,以及动量粗糙度与标量粗糙度的动态关系。  相似文献   

2.
利用2013年7月1日至2014年6月30日鄱阳湖东岸70 m铁塔涡动相关观测资料,应用Martano方法和TVM(Temperature Variance Method)方法分别计算了该地地表零平面位移d和粗糙度z0,通过代回Monin-Obukhov相似性理论的风廓线关系计算摩擦速度,以验证与实测摩擦速度的一致性。速度和温度标准差的归一化拟合线分别与Panosky等和Tillman给出的曲线趋势一致,表明该站观测数据总体满足近地层相似性。Martano方法计算结果随季节变化较大,春夏季的粗糙度是秋冬季的6.3倍;陆面方向零平面位移和粗糙度分别为来自湖面的2倍和10倍;Martano方法比TVM方法对季节和方向的敏感性更强。Martano方法计算得到零平面位移和粗糙度对摩擦速度造成了约9.9%的高估;而TVM方法对摩擦速度造成了约32.8%的高估;Martano方法计算的摩擦速度和观测值的一致性更好。  相似文献   

3.
植物冠层动量交换特征的实验研究   总被引:2,自引:1,他引:2       下载免费PDF全文
使用湍流梯度测试资料,对植物冠层动量交换特征进行了详细研究,结果表明:森林冠层内惯性副区能谱曲线仍可用幂指数描述,但斜率比-2/3更负;森林冠层内湍流尺度有变小的趋势;森林上层的耗散系数比下层大;由植被吸收引起动量及动量通量随冠层深度增加而明显减小;冠层下层的动量通量和耗散系数分别与上层的量有好的正相关;森林冠层内耗散系数和动量通量随大气稳定度有明显变化。  相似文献   

4.
区域气候模式RegCM2对标量粗糙敏感性试验   总被引:3,自引:0,他引:3  
和渊  苏炳凯等 《气象科学》2001,21(2):136-146
在地气通量的计算中,一般没有考虑温度、水汽、动量的相应粗糙度之间的不同。本文将标量粗糙度Z0T和Z0q引入区域气候模式RegCM2的陆面过程BATS中,用1991年6月与7月的观测资料作了三组敏感性试验,并同实况进行了比较。结果表明:在区域气候模式RegCM2中引入标量粗糙度后,提高了地气间感热通量与潜热通量的计算精度,改善了地表温度和地表比湿的模拟,进而改变了降水的模拟,表明区域气候模式对标量粗糙是敏感的,并且在晴天状况下更为敏感。  相似文献   

5.
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   

6.
本文运用常通量层中的相似理论和湍流半经验理论,并通过Charnock提出的粗糙度随摩擦速度变化的经验公式,引入流动下界面的影响,建立了一维定常海上大气边界层数值模式。为检验模式的性能,对AMTEX’75实测资料进行了模拟,得到比较满意的结果。并计算了中性和不稳定层结下海上大气边界层中主要特征参量。  相似文献   

7.
利用2007—2017年余姚地区44个气象自动站观测数据和欧洲中心ERA5再分析资料,对余姚地区日极大风分布进行了统计分析,并提出一种本地化的经验阵风预报模型(雷暴日除外)。研究发现:余姚地区日极大风呈正态分布,风力峰值为4~5级,平均每年大风日占比达7.03%,累计大风时次占比3.32%,年平均大风日26 d。风力越小,阵风与平均风之间的线性拟合效果越好。影响阵风预报的因子主要有10 m平均风速、925 hPa风速、地面粗糙度、摩擦速度和3 h变压。6级及以下阵风预报中,业务中的阵风经验系数1.4容易造成余姚本地阵风预报偏低,适用于余姚本地阵风预报经验系数为1.775;6级以上阵风预报经验方程考虑了平均风速、垂直动量下传、水平动量传输、地面摩擦和海拔高度订正,其与925 hPa风速的平方呈正相关,与摩擦速度呈自然指数相关,经验方程相对于经验阵风系数的预报拟合优度提升了59.61%;经验阵风预报方程通过了2018—2019年的数据检验,该方程对1~2级阵风预报偏高,3~5级效果最好,6级阵风的预报偏低;6级以上的阵风等级预报准确率达55.2%。地形摩擦作用在冷空气大风与台风大风过程中尤为重要,这两类过程阵风系数分布类似,但台风带来的动量下传比冷空气更为明显。  相似文献   

8.
卫星遥感结合地面资料对区域表面动量粗糙度的估算   总被引:10,自引:0,他引:10  
利用地面湍流观测资料估算了黑河实验区几个典型下垫面的局地地表动量粗糙度,与卫星观测Landsat TM资料相结合得到了由标准化差值植被指数(NDVI)计算地表动量粗糙度的经验关系式,进而估算了实验区夏季和近冬季的地表粗糙度的区域分布,并对所得关系式进行了合理性检验。  相似文献   

9.
张海宏  姜海梅  周秉荣  祁栋林 《气象》2019,45(11):1550-1559
利用玉树隆宝湿地的观测资料,分析了未冻结、冻结和冻结有积雪覆盖三种情况下动量通量和感热通量的日变化情况,计算了三种情况下动量总体输送系数、感热总体输送系数、动力学粗糙度和热力学粗糙度,分析了附加阻尼和粗糙度雷诺数的关系,并将三种附加阻尼的参数化方案进行了比较,结果表明:冻结状态下动量通量和感热通量的日变化幅度最大,冻结有积雪覆盖时,动量通量和感热通量的日变化幅度最小。动量总体输送系数C_D和感热总体输送系数C_H的值在冻结时最大,冻结有积雪覆盖时最小,动力学粗糙度和热力学粗糙度在冻结状况下最小,冻结有积雪覆盖时最大。未冻结、冻结和冻结有积雪覆盖状态下,三种附加阻尼kB~(-1)参数化方案中,幂函数型方案较为合适。  相似文献   

10.
青藏高原总体输送系数的特征   总被引:17,自引:1,他引:17  
利用中日亚洲季风机制合作研究计划设在西藏的 4个自动气象站(AWS)获得的5a多(199年7月~1998年12月)时次密集、观测连续的近地层梯度资料,以最小二乘法确定出相应站点各季节的地表粗糙度,并应用廓线-通量法计算了4站逐日的总体输送系数,分析了其随时间的变化特征。结果表明:青藏高原动量输送系数的多年平均值为3.53×10-3~4.99×10-3,热量输送系数为4.67×10-3~6.73×10-3,并且两种输送系数都存在明显的日变化和季节变化,部分站点还存在较明显的年际变化。另外,还讨论了总体输送系数与近地层大气层结稳定度、地表粗糙度以及地面风速等因子的关系,初步建立了可用常规气象站地面观测资料计算青藏高原总体输送系数的拟合公式。  相似文献   

11.
It has previously been shown that aerodynamic roughness length changes significantly along with nearsurface atmospheric thermodynamic state; however, at present, this phenomenon remains poorly understood, and very little research concerning this topic has been conducted. In this paper, by using the data of different underlying surfaces provided by the Experimental Co-observation and Integral Research in Semi-arid and Arid Regions over North China, aerodynamic roughness length (z0) values in stable, neutral, and unstable atmospheric stratifications are compared with one another, and the relationship between z0 and atmospheric thermodynamic stability (ζ) is analyzed. It is found that z0 shows great differences among the stable, neutral, and unstable atmospheric thermodynamic states, with the difference in z0 values between the fully thermodynamic stable condition and the neutral condition reaching 60% of the mean z0. Furthermore, for the wind speed range in which the wind data are less sensitive to z0, the surface z0 changes more significantly with ζ, and is highly correlated with both the Monin-Obukhov stability (ζ0) and the overall Richardson number (Rib), with both of their correlation coefficients greater than 0.71 and 0.47 in the stable and unstable atmospheric stratification, respectively. The empirical relation fitted with the experimental observations is quite consistent with the Zilitinkevich theoretical relation in the stable atmosphere, but the two are quite distinct and even show opposite variation tendencies in the unstable atmosphere. In application, however, verification of the empirical fitted relations by using the experimental data finds that the fitted relation is slightly more applicable than the Zilitinkevich theoretical relation in stable atmospheric stratification, but it is much more suitable than the Zilitinkevich relation in unstable atmospheric stratification.  相似文献   

12.
Based on the Coupled Ocean-Atmospheric Response Experiment(COARE)bulk algorithm and the Naval Postgraduate School(NPS)model,a universal evaporation duct(UED)model that can flexibly accommodate the latest improvements in component(such as stability function,velocity roughness,and scalar roughness)schemes for different stratification and wind conditions,is proposed in this paper.With the UED model,the sensitivity of the model-derived evaporation duct height(EDH)to stability function(Ψ),ocean wave effect under moderate to high wind speeds,and scalar roughness length parameterization,is investigated,and relative contributions of these factors are compared.The results show that the stability function is a key factor influencing the simulated EDH values.Under unstable conditions,the EDH values from stability functions of Fairall et al.(1996)and Hu and Zhang(1992)are generally higher than those from others;while under stable conditions,unreasonably high EDHs can be avoided by use of the stability functions of Hu and Zhang(1992)and Grachev et al.(2007).Under moderate to high wind speeds,the increase in velocity roughness length z0 due to consideration of the true ocean wave effect acts to reduce modeled EDH values;this trend is more pronounced under stable conditions.Although the scalar roughness length parameterization has a minor effect on the model-derived EDH,a positive correlation is found between the scalar roughness length z0qand the model-derived EDH.  相似文献   

13.
基于2019年12月至2020年11月峨眉山站梯度塔资料、辐射观测资料和地表通量资料,采用涡动相关法对峨眉山地区近地层的地表通量和蒸散发量的变化进行分析,并估算了零平面位移、空气动力粗糙度、空气热力粗糙度、动量通量输送系数和感热通量输送系数等重要的空气动力学和热力学参数.研究表明:近地面风速呈现高层高、低层低的特征,且...  相似文献   

14.
The influence of surface heterogeneities extends vertically within the atmospheric surface layer to the so-called blending height, causing changes in the fluxes of momentum and scalars. Inside this region the turbulence structure cannot be treated as horizontally homogeneous; it is highly dependent on the local surface roughness, the buoyancy and the horizontal scale of heterogeneity. The present study analyzes the change in scalar flux induced by the presence of a large wind farm installed across a heterogeneously rough surface. The change in the internal atmospheric boundary-layer structure due to the large wind farm is decomposed and the change in the overall surface scalar flux is assessed. The equilibrium length scale characteristic of surface roughness transitions is found to be determined by the relative position of the smooth-to-rough transition and the wind turbines. It is shown that the change induced by large wind farms on the scalar flux is of the same order of magnitude as the adjustment they naturally undergo due to surface patchiness.  相似文献   

15.
The relationship of surface albedo with the solar altitude angle and soil moisture is analyzed based on two-year (January 2002 to December 2003) observational data from the AWS (Automatic Weather Station) at MS3478 in the northern Tibetan Plateau during the experimental period of CEOP/CAMP-Tibet (Coordinated Enhanced Observing Period Asia-Australia Monsoon Project on the Tibetan Plateau). As a double-variable (solar altitude angle and soil moisture) function, surface albedo varies inconspicuously with any single factor. By using the method of approximately separating the double-variable function into two, one-factor functions (product and addition), the relationship of albedo with these two factors presents much better. The product and additional empirical formulae of albedo are then preliminarily fitted based on long-term experimental data. By comparison with observed values, it is found that the parameterization formulae fitted by using observational data are mostly reliable and their correlation coefficients are both over 0.6. The empirical formulae of albedo though, for the northern Tibetan Plateau, need to be tested by much more representative observational data with the help of numerical models and the retrieval of remote sensing data. It is practical until it is changed into effective parameterization formulae representing a grid scale in models.  相似文献   

16.
The influence of surface roughness on the dispersion of a passive scalar in a rough wall turbulent boundary layer has been studied using wind-tunnel experiments. The surface roughness was varied using different sizes of roughness elements, and different spacings between the elements. Vertical profiles of average concentration were measured at different distances downwind of the source, and the vertical spread of the plume was computed by fitting a double Gaussian profile to the data. An estimate of the integral length scale is derived from the turbulence characteristics of the boundary layer and is then used to scale the measured values of plume spread. This scaling reduces the variability in the data, confirming the validity of the model for the Lagrangian integral time scale, but does not remove it entirely. The scaled plume spreading shows significant differences from predictions of theoretical models both in the near and in the far field. In the region immediately downwind of the source this is due to the influence of the wake of the injector for which we have developed a simple model. In the far field we explain that the differences are mainly due to the absence of large-scale motions. Finally, further downwind of the source the scaled values of plume spread fall into two distinct groups. It is suggested that the difference between the two groups may be related to the lack of dynamical similarity between the boundary-layer flows for varying surface roughness or to biased estimates of the plume spread.  相似文献   

17.
Surface Flux Parameterization in the Tibetan Plateau   总被引:9,自引:1,他引:9  
This study investigates some basic aspects related to surface-flux parameterization in the Tibetan Plateau, based on the measurement at three sites. These sites are essentially flat and covered by very sparse and short grasses in the monsoon season. The main contributions include: (1) an optimization technique is proposed to estimate aerodynamic roughness length based on wind and temperature profiles. The approach is not sensitive to random measurement errors if the number of data samples is large enough. The optimized values reasonably vary with surface characteristics. (2) At the three sites, kB-1 (the logarithm of the ratio of aerodynamic roughness length to thermal roughness length) experiences seasonal and diurnal variations in addition to a dependence on surface types. The mean values for the individual sites vary over a range of 2.7 to 6.4 with large standard deviations. (3) A formula for estimatingthe value of kB-1 isproposed to account for the effect of seasonal variation of aerodynamic roughness length and diurnal variation of surface temperature. With the formula, the flux parameterization with surface temperature estimates sensible heat flux better than profile parameterization for all the sites.  相似文献   

18.
The effects of abrupt streamwise transitions of the aerodynamic roughness length ( $z_\mathrm{o}$ z o ) on the stable atmospheric boundary layer are evaluated using a series of large-eddy simulations based on the first Global Energy and Water Cycle Experiment Atmospheric Boundary Layer intercomparison study (GABLS1). Four $z_\mathrm{o}$ z o values spanning three orders of magnitude are used to create all possible binary distributions with each arranged into patches of characteristic length scales equal to roughly one-half, one, and two times the equivalent homogeneous boundary-layer height. The impact of the heterogeneity on mean profiles of wind speed and temperature, on surface fluxes of heat and momentum, and on internal boundary-layer dynamics are considered. It is found that $z_\mathrm{o}$ z o transitions do not significantly alter the functional relationship between the average surface fluxes and the mean profiles of wind speed and potential temperature. Although this suggests that bulk similarity theory is applicable for modelling the stable boundary layer over $z_\mathrm{o}$ z o heterogeneity, effective surface parameters must still be specified. Existing models that solve for effective roughness lengths of momentum and heat are evaluated and compared to values derived from the simulation data. The existing models are unable to accurately reproduce both the values of the effective aerodynamic roughness lengths and their trends as functions of patch length scale and stability. A new model for the effective aerodynamic roughness length is developed to exploit the benefits of the other models tested. It accurately accounts for the effects of the heterogeneity and stratification on the blending height and effective aerodynamic roughness length. The new model provides improved average surface fluxes when used with bulk similarity.  相似文献   

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