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1.
The atmospheric heat source strength over western Tibet has been computed for the period beginning with the last ten days in May, 1979 and extending through August, 1979. Our results show a significantly smaller heat source than that obtained by other authors. The discrepancy is mainly due to adjustments in the dray, coefficient suggested by observations and numerical modeling experiments. We subdivided western Tibet into northern and southern parts. In the north sensible heating, SH, provides the dominant input into the atmospheric heat source, whereas in the southern part latent heat, LP, offers a significant contribution after the start of the rainy season.Detailed heat budget calculations were also carried out over limited regions of southwestern Tibet which hau good station coverage. During periods with area-averaged rainfall ≤1 mm/day an atmospheric heat source maximum was located over southwestern Tibet near the 500 hPa level, while a heat sink dominated the upper troposphere in a layer of subsidence. When rainfall exceeded 4 mm/day, ascending motions and heal sources prevailed throughout the troposphere with maxima near 400 hPa. Time series analyses of the heat sourcs components show that the total atmospheric heat source is strongly modulated by the release of latent heat. Atmospheric radiational cooling reveals a phase shift in its relation with precipitation. During the first part of the observation period a correlation of that cooling exists mainly with the net radiation at the top of the atmosphere, during the last part with the net radiation at the ground.  相似文献   

2.
采用南京气象学院(NIM)5层陆面过程模式,利用1979年5-8月“青藏高原气象科学实验”资料模拟和分析了夏季青藏高原不同地区的陆面特征和地表能量特征。并将模拟值与根据观测资料计算得到的感热和潜热以及观测得到的净辐射、土壤温度、土壤热通量进行了对比。结果表明,NIM5层陆面过程模式可以模拟青藏高原夏季不同下垫面情形下的能量交换过程。  相似文献   

3.
根据NCEP/DOE再分析资料的地面感热通量和潜热通量以及MICAPS天气图资料识别的高原低涡资料集,研究了近30年来青藏高原夏季地面热源和高原低涡生成频数的气候学特征,分析了高原地面加热与低涡生成频数的时间相关性及其物理成因.得到如下认知:夏季高原地面感热通量的气候均值为58 W m-2,近30年地面感热总体呈微弱的减小趋势.其中在1980年代初期和21世纪前10年的大部分时段,地面感热呈增大趋势,而中间时段呈波动式下降.地面感热具有准3年为主的周期振荡,1996年前后是其开始减弱的突变点.高原夏季地面潜热通量的气候均值为62 W m-2,近30年呈波动状变化并伴有增大趋势.地面潜热的周期振荡以准4年为主,地面潜热增大的突变始于2004年前后.夏季高原地面热源的气候均值为120 W m-2,其中地面感热与地面潜热对地面热源的贡献在夏季大致相当.地面热源总体呈幅度不大的减弱趋势,其中1980年代到1990年代末偏强,21世纪前6年明显偏弱,随后又转为偏强.地面热源亦呈准3年为主的周期振荡并在1997年前后发生由强转弱的突变.根据MICAPS天气图资料的识别和统计,近30来夏季高原低涡的生成频数整体呈现一定程度的线性减少趋势,低涡高发期主要集中在1980年代到1990年代中后期.低涡生成频数有准7年为主的周期振荡现象,自1990年代中期开始的低涡生成频数的减少态势在1998年前后发生了突变.夏季高原低涡生成频数与同期高原地面感热呈高度正相关,与地面潜热呈一定程度的负相关,但与同期地面热源仍呈较显著的正相关.因此,在气候尺度上,高原地面热源偏强特别是地面感热偏强的时期,对应高原低涡的多发期.本研究从气候统计的时间相关性角度揭示了高原地面加热作用对催生高原低涡乃至高原对流活动的重要性.  相似文献   

4.
应用NCEP地面热通量资料, 研究了青藏高原地面感热、潜热的气候状况及其与初夏东亚大气环流之间的关系。发现高原地面热通量的异常将影响高原地区上空的垂直运动与辐散辐合运动, 从而引起东亚地区高度场及风场的异常。同时, 青藏高原地区地面热通量与后期东亚地区的环流变化也有密切关系, 这种关系可为预测东亚地区初夏环流异常提供有意义的指标。  相似文献   

5.
首先对青藏高原地表热通量再分析资料与自动气象站(AWS)实测资料进行对比, 结果表明: 相对于美国国家环境预报中心和国家大气中心20世纪90年代研制的NCEP/NCAR(Kalnay 等1996)和NCEP/DOE (Kanamitsu 等2002) 再分析资料, ECMWF(Uppala 等2004)资料在高原地区的地表热通量具有较好的代表性。进一步利用奇异值分解(SVD)方法分析了ECMWF资料反映的高原地面热源与我国夏季降水的关系, 发现前期青藏高原主体的冬季地面热源与长江中下游地区夏季降水量呈负相关, 与华北和东南沿海地区的夏季降水量呈正相关。而长江中下游地区夏季降水量还与春季高原南部的地面热源存在负相关、与高原北部的地面热源存在正相关。高原冬、春季地面热源场的变化是影响我国夏季降水的重要因子。  相似文献   

6.
The surface and atmospheric heating fields over the Qinghai-Xizang Plateau are computed by using theobservational data of solar radiation during 1982—1983.The mian results are as follows:The central andnorthern parts of the Plateau act as heat sinks in winter from November to January.Both eastern and south-ern parts of the Plateau are of heat sources.In summer,the main part of the Plateau acts as a strong heatsource,and the center of the heating field is in the southeastern Plateau.However the main part of thePlateau acts as a heat sink for the atmospheric heating fields from October to March.The maximum intensityof the atmospheric heat sink over the central Plateau appears in December and January.From April toSeptember,the main part of the Plateau acts as a heat source for the atmospheric heating fields.  相似文献   

7.
Using monthly mean of surface turbulent heat exchange coefficients calculated based on datafrom four automatic weather stations(AWS)for thermal equilibrium observation in July 1993—September 1996 and of surface conventional measurements,an empirical expression is establishedfor such coefficients.With the expression,the heat exchange coefficients and the components ofsurface thermal source are computed in terms of 1961—1990 monthly mean conventional data from148 stations over the Qinghai-Xizang(Tibetan)Plateau(QXP)and its adjoining areas,and the1961—1990 climatic means are examined.Evidence suggests that the empirical expression is capable of showing the variation of the heatexchange coefficient in a climatic context.The monthly variation of the coefficients averaged overthe QXP is in a range of 4×10~(-3)-5×10~(-3).The wintertime values are bigger in the mountainsthan in the valleys and reversal in summer.Surface effective radiation and sensible heat are thedominant factors of surface total heat.In spring surface sensible heat is enhanced quickly,resulting in two innegligible regions of sensible heat,one in the west QXP and the other innorthern Tibet.with their maximums emerging in different months.In spring and summersensible heat and surface effective radiation are higher in the west than in the east.The effectiveradiation peaks for the east in October—December and the whole QXP and in June and October forthe west.The surface total heat of the plateau maximizes in May.minimizes in December andJanuary,and shows seasonal variation more remarkable in the SW compared to the eastern part.Inthe SW plateau the total heat is much more intense than the eastern counterpart in all the seasonsexcept winter.Under the effect of the sensible heat,the total heat on the SW plateau starts toconsiderably intensify in February,which leads to a predominant heating region in the west,withits center experiencing a noticeable westward migration early in summer and twice pronouncedweakening in July and after October.However,the weakening courses are owing to differentcauses.The total heat over the north of QXP is greatly strengthened in March.thus generatinganother significant thermal region in the plateau.  相似文献   

8.
The heat exchange between ocean and atmosphere over cold water is studied by calculating all terms in the energy balance twice each day for the year 1971 for the Sable Island region.

The atmospheric long‐wave radiation is relatively constant because of frequent overcast and low clouds. The surface long‐wave balance is markedly negative in winter but slightly positive for a short time in summer, due to strong advection of warm moist air over the cold water. In winter, the turbulent fluxes are directed upwards and are strong, the upward fluxes beginning after the middle of August and lasting until mid‐March. The maximum daily values of latent heat flux are 400 to 500 ly day?1 (194 to 242 W m?2), about a third or a quarter of the magnitude over the warmer Gulf Stream water. The summer fluxes are fairly constant and directed downward.

The water of the Labrador Current in the Sable Island region warms substantially from March to September and conversely cools intensely in the period November‐January.

A comparison of the energy exchange for a current and for water without motion shows that the surface temperatures would be similar in summer, and the temperature drop would be about equal until November. From that time on, the surface temperature would level off for a water body with no current, but in actual conditions the surface temperature continues to drop to a late winter minimum of about 1°C.

Atmospheric advection of latent heat was calculated by assuming that the daily precipitation was always caused first by condensation of all locally evaporated water with any remainder being supplied by water‐vapour advection. The main cause for atmospheric heating in the Sable Island area was found to be condensation of imported water vapour. The region is, in summer, a marked sink for atmospheric heat and water content. For water it remains a sink even in winter. For sensible heat it becomes a source from November to March. The warming of the atmosphere is caused by release of latent heat of advected water vapour in the period February‐August. During the months September‐January the heat sources are both water‐vapour advection and surface turbulent terms.  相似文献   

9.
春季青藏高原地区大气热源的气候特征分析   总被引:1,自引:0,他引:1  
利用1948-2009年NCEP/NCAR逐日再分析资料采用倒算法计算了青藏高原地区大气热量源汇的值,分析了春季青藏高原地区大气热源的水平和垂直气候分布特征及时空变化特征.结果表明:春季青藏高原上空,大气热量源汇的整层积分为正值,即高原上空大气为热源,但在高原上空大气高层存在局部为冷源的分布.与周边地区相比较,高原对其上空大气的加热作用在三月份最为显著.春季3、4、5月青藏高原区域大气的加热存在一个自西向东逐渐扩展的过程.春季青藏高原东部和西部为大气热源年变化较大的区域,且高原东部和西部大气热源表现出反位相分布的特征.  相似文献   

10.
利用第三次青藏高原大气科学观测试验数据,对高原不同地区感热、潜热交换等湍流输送特征进行了分析,并进一步对比研究了其与气象环境因子的相关关系。结果表明:(1)高原各站之间感热和潜热的差异性较大,但大多在雨季潜热会大于感热。干燥的狮泉河站属于高寒荒漠地区,降水极少,全年感热都远大于潜热,波文比年平均值可达到20.0;湿润的比如站和嘉黎站潜热在4~10月均显著大于感热,波文比在4~10月的数值范围在0.27~0.88。(2)高原感热和潜热通量的季节变化与高原季风所处的地理位置有密切关系,高原中部的感热通量在3~5月达到最大值,而高原西部则在4~6月最大,可能与高原季风的活动有关。(3)通过与气象要素的相关分析表明,高原西部狮泉河站感热与地气温差的正相关关系最为显著,全年的相关系数可以达到0.905,在4个季节相关系数也均大于0.79,这可能与下垫面是裸地有关;高原中部安多站和那曲站感热与风速的正相关在夏季最为显著,比如站感热与风速的正相关在冬季最为明显,而狮泉河站感热与风速在春、夏季均有着十分显著的正相关。  相似文献   

11.
本文用1979年夏季6—8月青藏高原地区17个站资料(包括青藏高原科学实验资料),通过直接法求得长波辐射、短波辐射、凝结潜热和感热输送等四项加热分量,在此基础上求出高原地区的平均大气热量输送,并和国内外其它作者所估计的高原大气热源情况进行比较。计算结果表明,对高原大气热源的主要贡献是长波辐射,文中还探讨了青藏高原地区大气加热场与高原季风爆发前后以及高原季风活跃和中断时期环流的关系。  相似文献   

12.
In this study, a parameterization methodology based on Advanced Very High-Resolution Radiometer (AVHRR), Moderate Resolution Imaging Spectroradiometer (MODIS), and in situ data is proposed and tested for deriving the regional surface heating field, sensible heat flux, and latent heat flux over a heterogeneous landscape. In this case study, this method is applied to the whole Tibetan Plateau (TP) area. Four sets of AVHRR data and four sets of MODIS data (collected on 17 January 2003, 14 April 2003, 23 July 2003, and 16 October 2003) were used in this study to make comparisons between winter, spring, summer, and autumn values. The satellite-derived results were also validated using the “ground truth” as measured in the stations of CAMP/Tibet (Coordinated Enhanced Observing Period (CEOP) and Asia–Australia Monsoon Project on the Tibetan Plateau). The results show that the surface heating field, sensible heat flux, and latent heat flux in the four seasons across the TP are in close accordance with its land surface status. These parameters range widely due to the strongly contrasting surface features found within the TP region. Also, the estimated surface heating field, sensible heat flux, and latent heat flux all agree with the ground truth data, and usually, the absolute percentage difference between the two sets of data is less than 10 % at the validation stations. The AVHRR results were also in agreement with the MODIS data, with the latter usually displaying a higher level of accuracy. We have thus concluded that the proposed method was successful in retrieving surface heating field, sensible heat flux, and latent heat flux values using AVHRR, MODIS, and in situ data over the heterogeneous land surface of the TP. Shortcomings and possible further improvements in the method are also discussed.  相似文献   

13.
青藏高原地面-对流层系统的能量收支   总被引:3,自引:3,他引:3  
利用CCM3中的辐射模式CRM,计算了1月和7月地-气系统、地面-对流层系统和地面辐射能收支,研究了青藏高原地面-对流层系统辐射能收支的冬、夏季节特征及其与地面和地-气系统辐射能收支的关系,并与东部平原地区和高原北侧干旱地区比较。文中还讨论了云和高原冬季地面积雪对辐射能收支的影响,比较了大气辐射加热和地面感热通量对夏季高原对流层大气加热的贡献。  相似文献   

14.
西藏高原夏季旱涝年OLR分布差异   总被引:10,自引:0,他引:10       下载免费PDF全文
根据美国NOAA卫星观测得到的射出长波辐射资料(Outgoing Longwave Radiation,简称OLR),分析了西藏高原及其附近地区各月的辐射气候特征,指出:高原冬、春季节OLR主要反映了高原下垫面温度的季节变化,高原夏季为雨季,OLR与降水之间存在较好的负相关。印度季风爆发前后的OLR演变特征反映出中、低纬大气环流调整对高原雨季形成及降水分布的影响。旱涝年OLR合成分析表明:高原夏季降水与赤道印度洋反Walker环流强弱、印度季风槽、副热带高压及西太平洋暖池区对流强度、位置变化有密切的关系。  相似文献   

15.
青藏高原作为世界第三极,其热力强迫作用不仅对亚洲季风系统的发展和维持十分重要,也会对大气环流场产生深远影响。利用欧洲中期天气预报中心(ECMWF)的ERA-Interim中1979-2016年3-10月青藏高原及其周边地区的地表热通量月平均再分析资料,通过分析得出以下结论:3-5月青藏高原主体由感热占据,感热强度快速上升且呈西高东低的分布态势,潜热强度较小但随时间而增强。季风爆发后的6-8月,青藏高原感热强度减弱,潜热强度迅速增强且呈东高西低的分布特征。季风消退后的9-10月,感热与潜热强度相当,但感热呈现出西高东低的分布特征。过去38年,青藏高原地表感热总体呈现微弱下降趋势,潜热呈较弱上升趋势。青藏高原西部地区感热呈微弱下降趋势,潜热呈上升趋势。东部感热呈较为明显的下降趋势且近年来变化趋势增强,东部潜热通量则呈现较为明显的上升趋势,分析结论与近期全球变暖条件下青藏高原气候变暖变湿这一变化状况一致,通过对青藏高原地表热通量的变化分析为下一步运用第三次青藏高原大气科学试验所获资料分析青藏高原上空大气热源的变化以及地表加热场如何影响大气环流奠定基础。   相似文献   

16.
青藏高原地面热源对亚洲季风爆发的热力影响   总被引:23,自引:4,他引:23  
利用多年NCEP/NCAR再分析全球逐候平均气象场资料和逐旬感热、潜热资料,对亚洲夏季风爆发期间青藏高原及其邻近地区地面加热场的特征进行分析。着重讨论了高原和邻近地区感热加热对亚洲夏季风爆发的影响,具体分析了高原感热加热对亚洲夏季风推进的影响机制,以及对热带低层西风气流的作用。结果发现,中纬度主原的感热加热所造成的经、纬向热力差异是导致亚洲夏季风爆发的原因。亚洲夏季风建立区域和时间的差异与高原感热加热的区域性有关。高原感热加热在南海夏季风爆发前后对南海地区低层西风所流所起的作用不同,在季风爆发前是加速低层西风,在季风爆发后起削弱西风气流的作用。对亚洲夏季风爆发早年和晚年的感热加热进行了对比分析,发现亚洲夏季风爆发时间的年际变化与热源的年际变化有关。  相似文献   

17.
春夏东亚大气环流年代际转折的影响及其可能机理   总被引:2,自引:0,他引:2  
本文通过多变量联合经验正交分解(MV-EOF)方法揭示了近30年(1979~2010年) 春季和夏季东亚大气环流所发生的年代际转折及其与中国南方降水年代际季节反相变化的内在联系,探讨了局地性大气热源年代际变化影响东亚大气环流年代际转折的可能机理.结果表明:(1)东亚大气环流春季第一模态和夏季第二模态在90年代中期都发生了明显的年代际转折;(2)与春季大气环流第一模态和夏季大气环流第二模态年代际转折相对应的是中国南方降水明显的年代际季节反相变化,即春季降水年代际减少,夏季降水年代际增多;(3)春季青藏高原和夏季贝加尔湖地区大气热源年代际变化对东亚大气环流年代际转折有一定贡献,是造成中国南方降水年代际季节反相变化的直接原因;(4)春季青藏高原大气热源的年代际减弱,使得高原东南侧的西南风减弱,导致中国南方上空水汽输送不足,春季降水减少.夏季贝加尔湖大气热源偶极型分布由“南负北正”转变为“南正北负”,由此在贝湖上空激发高压异常,使得夏季雨带北进受阻而停滞南方,造成中国南方夏季降水增多.  相似文献   

18.
1.IntroductionTopreciselyestimatethevaluesofalbedosatsurfaceandatmospherictop.surfacetotalradiationandearth--atmosphereoutgoinglongwaveradiationiscrucialtocalculatingradiationbalanceatsurfaceandatmospherictopandexploringoftheeffectoftheQXPatmosphericheatsourcesonatmosphericcirculations.Using1958--1960observationsofsurfacetotalradiation,albedoandsurfacemeteorologicalobservationsoverChina.ChenandGongetal.(1964.1965)investigated,throughanatmosphericradiationcalculationscheme.thedistributionchar…  相似文献   

19.
利用NCEP/NCAR (National Centers for Environmental Prediction/National Center for Atmospheric Research)2001-2010年再分析资料,检验了全球气候系统模式CESM中大气模块CAM (Community Atmosphere Model)对亚洲夏季风和大气热源的模拟能力。结果显示,模式可以再现亚洲夏季风和大气热源的主要特征。通过敏感试验探讨人为气溶胶影响亚洲夏季风的机理,分析、讨论了气溶胶引起的非均匀加热的变化对辐散风和无辐散风强度的影响,在机理上解释了亚洲夏季风减弱的原因。结果表明,人为气溶胶浓度的升高使东亚夏季风强度在中国东南地区、中南半岛北部和印度半岛北部减弱。而中国东南部季风的减弱促使中国内陆降水减少,沿海降水增多。进一步分析人为气溶胶浓度升高的作用发现,其改变了大气热源的分布,造成阿拉伯海、孟加拉湾和中国南海大气热源增强,中国东部地区和中南半岛大气热源减弱,其中气溶胶通过影响凝结潜热来改变大气热源,主要是对对流过程的影响。此外,大气热源分布的变化改变了季风区的热力结构,使中国东南地区、中南半岛北部的加热减弱,从而减少了全位能的产生,使得全位能向辐散风的转换减小,辐散风减弱;同时,中国东南部、中南半岛北部季风由于辐散风向无辐散风转换的减弱,无辐散风减弱,最终导致了夏季风强度的减弱。而且,人为气溶胶对亚洲夏季风的影响主要通过大气热力和动力过程的响应产生作用。  相似文献   

20.
亚——非季风区非绝热加热与夏季环流关系的诊断研究   总被引:4,自引:0,他引:4  
基于热力适应理论,本文利用 NCEP/ NCAR再分析资料对撒哈拉沙漠、青藏高原和孟加拉湾地区的非绝热加热与夏季环流进行了诊断研究。在非洲撒哈拉沙漠地区,以感热输送为主的加热仅局限于近地面层,边界层以上的大气则以辐射冷却占优势。因而除了边界层内存在着浅薄的正涡度和微弱的上升运动以外,整个对流层几乎都维持负涡度并盛行下沉运动。对于青藏高原地区,强大的表面感热通量引起的垂直扩散是近地面大气加热的主要分量,与大尺度上升运动相关的凝结潜热对低层大气的加热也有一定的贡献。长波辐射造成的对流层中、上层大气的冷却则主要由深对流潜热释放来补偿。夏季高原地区总非绝热加热是正值,且最大加热率出现在边界层内。低空大气辐合产生正涡度,而中、高层大气辐散伴有较强的负涡度。因而高原盛行上升运动,最大上升运动位于近地面层。夏季孟加拉湾地区的深对流凝结潜热释放远大于长波辐的冷却作用,因而整个对流层几乎都保持较强的非绝热加热。400hPa层附近的最大加热率引起300-400hPa最强的上升运动。对流层上层是负涡度区,而中、低层为正涡度区。结果还表明,垂直和水平辐散环流与大气的热源和热汇区密切相联:在高层,辐散气流从热源区流向热汇区;在低层则相  相似文献   

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