共查询到20条相似文献，搜索用时 343 毫秒
1.
2.
青藏高原东坡高原草甸近地层气象要素与能量输送季节变化分析 总被引：1，自引：0，他引：1
本文简要介绍了青藏高原东坡理塘大气综合观测站的情况。利用该站2007~2008年观测资料,分析比较了青藏高原东坡地区高原草甸下垫面情况下近地层气象要素及能量输送的季节变化特征。结果表明：理塘地区近地层气象要素及能量输送的季节变化显著,具有明显的水热同期特点。各个季节近地层气象要素和湍流通量,如风、气温、感热通量、潜热通量等,日变化显著。风速、动量通量、摩擦速度等要素的平均日最大值和最小值分别出现在下午和日出前。比湿的峰值出现在日出前。辐射和热平衡分量的日均最大值与最小值分别出现在正午及日出前。地表热源强度分析表明,理塘白天为热源,在春夏秋三季夜间为弱的热源与冷源交替出现。在雨季,潜热输送在陆气间热量交换过程中占主导作用,感热输送是次要的;干季的结果与雨季相反,感热是首要的。 相似文献
3.
青藏高原东坡高原草甸近地层气象要素与能量输送季节变化分析 总被引：1，自引：0，他引：1
本文简要介绍了青藏高原东坡理塘大气综合观测站的情况。利用该站20072008年观测资料, 分析比较了青藏高原东坡地区高原草甸下垫面情况下近地层气象要素及能量输送的季节变化特征。结果表明:理塘地区近地层气象要素及能量输送的季节变化显著, 具有明显的水热同期特点。各个季节近地层气象要素和湍流通量, 如风、气温、感热通量、潜热通量等, 日变化显著。风速、动量通量、摩擦速度等要素的平均日最大值和最小值分别出现在下午和日出前。比湿的峰值出现在日出前。辐射和热平衡分量的日均最大值与最小值分别出现在正午及日出前。地表热源强度分析表明, 理塘白天为热源, 在春夏秋三季夜间为弱的热源与冷源交替出现。在雨季, 潜热输送在陆气间热量交换过程中占主导作用, 感热输送是次要的;干季的结果与雨季相反, 感热是首要的。 相似文献
4.
本文分析了用IAP两层大气环流模式模拟的海表动量和热量通量,并将其同Han等和Esbensen等的气候资料比较.模拟的热量通量与观测估计值有类似的水平分布和季节变化,但在中低纬地区有偏多的热量由海洋向大气输送,尤其1月北半球中纬大气需要从海洋获得过分多的热量;模拟的海表动量通量和气候估计值也类似,但模拟的北半球冬季中高纬西风动量通量中心位置偏东,赤道中西太平洋和大西洋的东风动量通量偏弱,南半球环绕南极的西风带模拟得过分弱(尤其在7月份).本文还检验了基本变量的日变化和日际变化对计算海表动量和湍流扩散热量通量的影响,结果表明用月平均,日平均和每小时的基本量计算的动量和湍流扩散热量通量依次增大,尤其在中高纬地区更明显. 相似文献
5.
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
6.
文中分析和模拟了森林冠层上下动量、热量和水汽传输的特征。结果表明：冠层对动量的吸收十分明显,非局地扩散通量在冠层上下的动量传输中起着很大的作用;白天在冠层下层结稳定,但冠层下观测的感热通量向上传输;夜晚冠层下层结不稳定,但冠层下观测的感热通量向下传输,白天和晚上都出现了热量的反梯度传输现象,从而证明在热量输送中,非局地扩散通量不可忽视。同时对冠层上下的水汽交换特征的分析表明：非局地扩散通量是冠层内水汽向冠层上传输的主要机制。 相似文献
7.
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
8.
1986年东海与南海的海-气界面热量交换 总被引：1，自引：0，他引：1
采用实测资料计算1986年7—12月东海和南海观测海域海-气界面热量交换。结果表明：7—9月上旬,大气向观测海域输送热量是主要现象,因为这时的气温比水温高,潜热通量与感热通量出现反相变化,天气晴好,海洋大量吸热;9月中旬—12月,观测海域向大气输送热量是主要现象,东海表现得比南海更为明显,主要贡献来自潜热通量和感热通量。受冷空气影响时,感热通量重要;在热带辐合带和热带气旋系统内海-气界面热量交换强烈,大气对海洋的响应为主。 相似文献
9.
10.
一个确定大气近地层湍流输送的计算方案 总被引：1，自引：0，他引：1
在相似理论的基础上,提出了一个确定大气近地层湍流输送特征(包括气象要素风、温度的垂直分布廓线,以及大气和下垫面之间的动量和热量通量交换)的计算方案.并与Businger(1971)的迭代计算方案进行了比较.该方案计算结果较好,应用方便. 相似文献
11.
Stephan R. de Roode Harm J. J. Jonker Peter G. Duynkerke Bjorn Stevens 《Boundary-Layer Meteorology》2004,112(1):179-196
Large-eddy simulations of a clear convective boundary layer (CBL)and a stratocumulus-topped boundary layer are studied. Bottom-upand a top-down scalars were included in the simulations, and theprinciple of linear superposition of variables was applied toreconstruct the fields of any arbitrary conserved variable.This approach allows a systematic analysis of countergradient fluxesas a function of the flux ratio, which is defined as the ratio betweenthe entrainment flux and the surface flux of the conserved quantity.In general, the turbulent flux of an arbitrary conserved quantityis counter to the mean vertical gradient if the heights where thevertical flux and the mean vertical gradient change sign do notcoincide. The regime where the flux is countergradient is thereforebounded by the so-called zero-flux and zero-gradient heights. Becausethe vertical flux changes sign only if the entrainment flux has anopposite sign to the surface flux, countergradient fluxes arepredominantly found for negative flux ratios. In the CBL the fluxratio for the virtual potential temperature is, to a good approximation,constant, and equal to -0.2. Only if the moisture contribution to thevirtual potential temperature is negligibly small will the flux ratio forthe potential temperature be equal to this value. Otherwise, theflux ratio for the potential temperature can have any arbitrary(negative) value, and, as a consequence, the fluxes for thepotential temperature and the virtual potential temperature willbe countergradient at different heights. As a practical application ofthe results, vertical profiles of the countergradient correction termfor different entrainment-to-surface-flux ratios are discussed. 相似文献
12.
13.
14.
A total of 52 years of data (1949–2000) from the NCEP/NCAR reanalysis are used to investigate mechanisms involved in forcing and damping of sea surface temperature (SST) variability in the South Atlantic Ocean. Organized patterns of coupled ocean–atmosphere variability are identified using EOF and SVD analyses. The leading mode of coupled variability consists of an SST pattern with a strong northeast–southwest gradient and an SLP monopole centered at 15°W, 45°S. The anomalous winds associated with this monopole generate the SST pattern through anomalous latent heat flux and mixed layer deepening. Other heat flux components and anomalous Ekman transport play only a secondary role. Once established, the SST pattern is attenuated through latent heat flux. The higher SST modes are also induced by anomalous winds and destroyed by latent heat flux. It thus appears that the coupled variability in the South Atlantic Ocean consists of atmospheric circulation anomalies that induce SST anomalies through anomalous latent heat fluxes and wind-induced mixed layer deepening. These SST anomalies are destroyed by latent heat flux with no detectable systematic feedback onto the atmospheric circulation. Atmospheric variability in the South Atlantic is found to be largely independent of that elsewhere, although there is a weak relation with ENSO (El Niño-Southern Oscillation). 相似文献
15.
南海季风建立前后珠江三角洲的陆气热量交换与热力边界层结构特征 总被引：4，自引：0，他引：4
根据动力与热力指标,2004和2005年南海季风建立前后可分成明显的4个阶段——季风建立前的雨期、非雨期;季风建立后的活跃期与非活跃期。对2004和2005年南海季风建立前后的广州番禺综合外场观测资料进行分析,得到了这4个阶段陆气热量交换与热力边界层的主要特征:净辐射与净短波辐射的变化趋势基本一致,净短波辐射与净长波辐射之比为3.49—4.81,净短波辐射是净辐射的主要贡献项,云量与降水是控制净短波辐射与净辐射的直接因素;季风活跃期间午间对流云系对太阳辐射衰减显著,造成了辐射各分量以及热通量的峰值区变窄,量值急剧变小;季风建立前后感热与潜热均是净辐射的主要消耗项,占净辐射的90%以上,潜热明显大于感热,2005年较2004年潜热的分配额有明显的增加,其原因可能与近地层的风速较大,总是维持向上的湿度梯度有关;季风建立前后除季风活跃期外边界层位温结构均具有明显的日变化特征,午间混合层可发展至1070m,而季风活跃期间午间混合层发展受到对流云释放潜热的抑制,导致季风活跃期混合层消失的现象,分析还发现季风建立前后各阶段夜间残余混合层均不明显。分析表明引起陆气能量过程及边界层热力结构差异的关键因素之一是云系与降水,加强边界层过程与降水宏微观过程相互作用的研究是深入认识陆气过程与边界层结构特征的关键。 相似文献
16.
Four months of eddy correlation data collected over a grass field and a nearby sage brush community are analyzed to examine
the adjustment of the boundary-layer structure as it flows from the heated brush to the snow-covered grass. The grass site
includes a 34-m tower with seven levels of eddy correlation data. The midday heat flux over the snow-covered grass and bare
ground surfaces is often downward particularly with melting conditions, while the corresponding heat flux over the brush is
almost always upward. For most of these cases, a stable internal boundary layer over the snow is well defined in terms of
vertical profiles of the buoyancy flux over the snow-covered grass. The stable internal boundary layer is generally embedded
within a deeper layer of flux divergence corresponding to increasing upward heat flux with height above the internal boundary
layer. With thin snow cover, the surface heat flux over the grass is weak upward due to heating of grass protruding above
the snow so that the flow adjusts to a decrease of the upward surface heat flux in the downwind direction. This common case
of an adjusting boundary layer contrasts with the formation of an internal boundary layer due to a change of sign of the surface
heat in flux the downwind direction. The adjustment of the boundary layer to the decrease of the surface heat flux leads to
vertical divergence of the upward heat flux in contrast to the usual heated boundary layer over homogeneous surfaces. The
consequences of the cooling due to the vertical divergence of the heat flux are discussed in terms of the heat budget of the
adjusting and internal boundary layers. 相似文献
17.
18.
Ann-Sofi Smedman 《Boundary-Layer Meteorology》1988,44(3):231-253
Boundary-layer measurements conducted at the Marsta site in Sweden from a winter-time situation (23–25 Feb.) with stable stratification have been analysed. The data comprise wind and temperature profile measurements up to 30 m, turbulence measurements at 2, 6 and 30 m and Doppler acoustic sounder data up to about 150 m. The upwind fetch at the site is flat and free from obstacles to a distance of ca 5 km for the particular sector chosen for the experiment.During the night, a two-layer vertical structure developed. Analysis of power spectra, co-spectra and variances in a shallow and very stable turbulent boundary layer near the ground show that the turbulence is fully developed and follow the universal behaviour.Above, at a height of 30 m, another turbulent layer is produced by increased wind shear near a low-level jet. This turbulent upper layer can be regarded as a layer of free shear flow. At this height, there also exist wave-turbulence interactions at low frequencies which sometimes cause a countergradient heat flux. 相似文献
19.
The time and space variations of the ten-day mean surface sensible heat flux have beenanalyzed in this paper based on the data of NCEP/NCAR from January of 1979 to December of1995 in the South China Sea(SCS)monsoon region.It is found that large variations of the surfacesensible heat flux standard deviations exist in the northwestern Indochina Peninsula and the IndianPeninsula regions,and their locations and strength change significantly during the onset period ofSCS monsoon.The negative deviations appear evidently earlier in the Indocbina Peninsula than inthe Indian Peninsula but the deviation strength in the Indian Peninsula is stronger than that in theIndochina Peninsula.The appearance of the zonal negative mean deviations in the southern part ofthe Indochina Peninsula corresponds to the date of the SCS summer monsoon onset,while theoccurrence of the deviation decrease corresponds to the date of the South Asian monsoon onset.The sensible heat flux increases dekad by dekad before the onset of the summer monsoon in theIndian Peninsula and the Indochina Peninsula and decreases after the monsoon onset.Therefore,the surface sensible heat flux changes in the Indochina and the Indian Peninsula regions maybe havesome connections with the SCS monsoon onset and the Indian monsoon onset,and the IndochinaPeninsula maybe becomes the sensitive or key region to the SCS monsoon onset and the land maybeplays an important role in triggering summer monsoon onset. 相似文献
20.
P. Pettré M. F. Renaud R. Renaud M. Déqué S. Planton J. C. André 《Meteorology and Atmospheric Physics》1990,43(1-4):187-195
Summary A one dimensional analytical model of katabatic wind over the Antarctica has been developed. This parametric model is derived from the bulk two-layer model of Ball including the surface friction and taking into account the Earth's rotation and the geostrophic wind in the upper layer.This model is validated using the data set (70 soundings) collected during IAGO experiment at D47 (67°24S, 138°43E, altitude 1 564m), 110 km inland from the coast of Adélie Land.The parameteric model is then introduced into a GCM which is a spectral global version of the operational numerical weather prediction model used by the French weather service. The most significant effect of the parameterization is a 50 m increase of the geopotential height over the South Pole. The surface temperature at the South Pole increases (2°C) reducing the pole-midlatitude thermal gradient. The westerly circulation at 50° S is slowed down (4m/s at 850 hPa), and the surface pressure at the South Pole increases (4hPa). These results, consistent with an increase of katabatic winds, would however be improved by a better coupling between the parameterization and the GCM boundary layer.With 8 Figures 相似文献