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1.
Utilizing data from NCEP/ NCAR reanalysis, the summertime atmospheric diabatic heating due to different physical processes
is investigated over the Sahara desert, the Tibetan Plateau, and the Bay of Bengal. Atmospheric circulation systems in summer
over these three areas are also studied. Thermal adaptation theory is employed to explain the relationship between the circulation
and the atmospheric diabatic heating.
Over the Sahara desert, heating resulting from the surface sensible heat flux dominates the near-surface layer, while radiative
cooling is dominant upward from the boundary layer. There is positive vorticity in the shallow boundary layer and negative
vorticity in the middle and upper troposphere. Downward motion prevails over the Sahara desert, except in the shallow near—surface
layer where weak ascent exists in summer. Over the Tibetan Plateau, strong vertical diffusion resulting from intense surface
sensible heat flux to the overlying atmosphere contributes most to the boundary layer heating, condensation associated with
large—scale ascent is another contributor to the lower layer heating. Latent heat release accompanying deep convection is
critical in offsetting longwave radiative cooling in the middle and upper troposphere. The overall diabatic heating is positive
in the whole troposphere in summer, with the most intense heating located in the boundary layer. Convergence and positive
vorticity occur in the shallow near—surface layer and divergence and negative vorticity exist deeply in the middle and upper
troposphere. Accordingly, upward motion prevails over the Plateau in summer, with the most intense rising occurring near the
ground surface. Over the Bay of Bengal, summertime latent heat release associated with deep convection exceeds longwave radiative
cooling, resulting in intense heating in almost the whole troposphere. The strongest heating over the Bay of Bengal is located
around 400 hPa, resulting in the most intense rising occurring between 300 hPa and 400 hPa, and producing positive vorticity
in the lower troposphere and negative vorticity in the upper troposphere. It is also shown that the divergent circulation
is from a heat source region to a sink region in the upper troposphere and vice versa in lower layers.
This work was jointly supported by “ National Key Program for Developing Basic Sciences” G1998040904 by NSFC projects 49805003,
49635170, 49823002, and 49825504. 相似文献
2.
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
3.
本文利用NCAR开发的CAM5.1(Community Atmosphere Model Version 5.1)模式,针对我国东部大规模城市下垫面发展对南海夏季风爆发的影响进行了数值模拟研究。结果表明我国东部大规模城市群发展可能使得南海夏季风提前1候爆发;机理分析表明:在南海夏季风爆发之前,中国东部城市群发展引起的陆面增温,使得南海及其附近地区南北温差提前逆转、中国东部区域海平面气压降低,导致中南半岛到南海地区西南气流加强,中南半岛到南海地区降水增加,而凝结潜热垂直变化强迫出的异常环流,促进了南亚高压的加强及提前北跳,相伴随的高层抽吸作用有助于季风对流的建立和西太平洋副高的减弱东撤,从而形成了有利于南海夏季风爆发的高低层环流条件,导致南海夏季风提前爆发。另外,观测结果表明1993年之后南海夏季风爆发的日期相对上一个年代明显提前约2候,城市化快速发展阶段与南海夏季风爆发的年代际变化存在时间段的吻合,表明城市下垫面发展可能是南海夏季风提前爆发的原因之一。 相似文献
4.
通过理论分析和数值模拟,研究了降水所致凝结潜热影响副热带高压带断裂的物理机制。基于全型垂直涡度方程的尺度分析指出,强的对流凝结加热的垂直梯度的变化,导致副热带地区对流层高层和中低层的高低压分布呈现出反位相。数值试验证实凝结潜热是决定东半球夏季副热带高压位置和强度的关键因素：东亚季风降雨所致凝结潜热加热使高层南亚高压位于加热中心西侧,中层西太平洋副热带高压位于加热中心东侧。通过定常波的传播,副热带地区的凝结潜热加热对中高纬天气的形成和维持有一定影响。 相似文献
5.
Condensation heating of the Asian summer monsoon and the subtropical anticyclone in the Eastern Hemisphere 总被引：27，自引：0，他引：27
The effects of condensation heating on the formation of the subtropical anticyclone in the Eastern Hemisphere (EH) are studied
by means of theoretical analysis and numerical simulation. The complete vorticity equation is employed for the analysis. It
is found that, due to the vertical gradient of strong condensation heating, the distribution of cyclone and anticyclone in
the upper troposphere is out of phase with that in the middle and lower troposphere. This is confirmed by a series of numerical
experiments. The horizontal gradient of the condensation heating also affects the configuration of the subtropical anticyclone.
It is concluded that condensation heating is a key factor for the formation and location of the summer subtropical anticyclone
in the EH. The latent heating released by the Asian monsoon rainfall contributes to the formation of the 200 hPa South Asian
anticyclone on the western side of the heating center and the 500 hPa western Pacific subtropical anticyclone on the eastern
side of the center. Such configurations are modified to some extent by surface sensible heating and orography. The circulation
in mid-latitudes is also affected by the latent heating in the subtropical area through the propagation of Rossby waves.
Received: 10 September 1999 / Accepted: 5 June 2000 相似文献
6.
通过对四川盆地西部一次持续性暴雨过程的半理想数值模拟,研究了青藏高原热力作用对四川盆地持续性暴雨过程的影响。研究表明,高原的热力作用对于下游地区有着显著的影响,主要表现为:（1）关闭高原地面感热和潜热后,高原地区和四川盆地西部的降水明显减弱,而盆地中东部降水却有所加强,且四川盆地降水的日变化特征稍有减弱;（2）500 hPa青藏高原上的短波槽减弱,位于四川盆地中西部的背风槽强度、范围有所减弱,但低层盆地东部的气旋性涡旋加强;（3）涡度收支的定量分析发现,关闭高原热力作用后,盆地东部对流层低层垂直风切变的增强使得夜间倾斜项的正贡献增强,从而使该区域涡旋发展加强,盆地东部降水增强。 相似文献
7.
针对2020年8月11—12日四川盆地西部特大暴雨过程中尺度系统演变特征和维持机制,利用欧洲中心ERA5逐小时再分析资料以及FY-4A的云顶相当黑体温度TBB资料进行诊断分析。(1) 本次过程发生在500 hPa巴湖长波槽分裂短波和高原低槽东移发展在四川盆地停滞,副高加强西伸形成阻挡的形势下,同时200 hPa有南亚高压和高空分流区配合。(2) 在上述有利的背景条件下,中尺度系统活动经历了中尺度辐合扰动-西南涡生成发展-低空急流影响-西南涡再次发展增强等4个阶段,西南涡两个阶段的发展对降水影响最大,初生发展阶段雨强最强,再次发展阶段强降雨范围最大。(3) 西南涡在暖区内初生发展,对流不稳定性强,地面潜热和感热加热以及500 hPa层以下水汽凝结潜热加热均十分显著,在较强暖湿平流作用下,配合低层涡度拉伸项和扭转项的动力作用加强,西南涡迅速发展,但低层辐合相对较弱,正涡度柱高度仅发展至500 hPa。(4) 西南涡再次发展阶段冷平流入侵,大气斜压性增强,中高层感热和凝结潜热加热作用加大,“低层辐合-中高层辐散”的动力机制显著加强,配合垂直向上输送正涡度和涡度拉伸项的动力发展作用,西南涡发展旺盛,正涡度柱中心强度和发展高度较初始发展阶段均明显增强。 相似文献
8.
通过数值试验研究了孟加拉湾季风爆发期间该地区旺盛的对流凝结加热对南海季风爆发和副热带高压“撤出”南海的影响,结果证明在孟加拉湾地区引入模拟的对流凝结潜热使该地区出现了强烈的上升运动,引起了孟加拉湾季风的爆发。同时由于对凝结加热的非对称Rossby响应,在南海北部导致西风出现和增强及垂直上升运动。因低层水汽平流的共同作用下,在南海北部引起了对流的发展。而正是南海北部的凝结加热促使南海地区温度经向梯度逆转,使副热带高压脊面的倾斜从冬季型转为夏季型,即低层的副热带高压减弱南移。最后当对流在南海地区发展起来时,副热带高压移出南海地区。 相似文献
9.
亚洲夏季风建立前后对流层温度场演变特征及其热力成因 总被引：5，自引：1，他引：4
对１９９６年亚洲夏季风爆发前后（３～６月）印度及南海季风区对流层温度演变特征及其热力成因作了比较分析。结果表明：印度和南海夏季风的爆发与各季风区对流层中上层南北温差逆转密切相关,而南北温差逆转是由１０～３０°Ｎ之间纬度带对流层的季节性增暖引起的。夏季风爆发前期,南海季风区的增温主要由暖平流及非绝热加热过程（主要为凝结潜热）共同作用所致。春季在印度季风区大陆上空存在显著的下沉绝热增温,使得对流层中上层的增温率比华南大陆及邻近地区上空的增温率显著得多。但印度季风区冬末春初的南北温差（南暖北冷）也非常明显,以至该地区对流层中上层增暖到引起南北温差发生逆转的时间较迟,而南海季风区对流层中层南北温差发生逆转的时间相对要早,因而印度夏季风比南海夏季风迟爆发。 相似文献
10.
对惯性重力内波方程组分别通过线性和非线性求解探讨造成2010年10月海南岛一次特大暴雨中一类热带中尺度涡旋生成发展的动力、热力机制,研究发现:（1）在副热带高压和大陆冷高压南侧反气旋性纬向水平风切变大值区、静力不稳定大气层结、积云对流潜热释放、低空急流、适当强度的冷空气有利于热带中尺度涡旋的形成和发展;（2）非线性惯性重力内波的孤立波解与这类热带中尺度涡旋有很好的联系,在静力不稳定的大气层结下,热带中尺度涡旋的形态主要由对流凝结潜热加热所决定,即潜热加热下的孤立波解要求热带中尺度涡旋在垂直方向是一个浅薄的涡旋系统;另外强盛的对流凝结潜热对热带中尺度涡旋垂直运动振幅的增强起主要作用,更有利于涡旋的发展和维持。基于天气事实分析的理论研究为深化影响海南的热带中尺度涡旋乃至南海中尺度对流系统的机理认识进行了探索。 相似文献
11.
2003年夏季梅雨期一次强气旋发展的位涡诊断分析 总被引：10，自引：2，他引：8
通过位涡诊断和回推轨迹分析, 对2003年夏季梅雨期间一次强江淮气旋的发展过程进行了研究。结果表明: 气旋发展初期, 非绝热加热在气旋的低层发展中起了主要作用, 随后由于高层水平平流的增强, 通过垂直平流使高低层大值位涡耦合在一起, 从而使气旋迅速发展。从中、 高、 低层对位涡柱形成所起的作用来看, 低层主要是非绝热加热, 中层是垂直平流, 而高层主要是水平平流; 从构成气旋的气流来说, 在气旋迅速发展阶段, 低层主要以西南暖湿气流为主, 高层 (500 hPa以上) 主要以沿急流轴下降的高层干冷气流和对流层底层流向气旋东北部并迅速上升的暖湿气流为主。高低层冷暖空气的相互作用主要发生在600 hPa及以上层次, 因凝结加热引起的垂直运动通过垂直平流可能在冷暖气流相互作用和上下大位涡的垂直耦合中发挥了重要作用。 相似文献
12.
13.
利用可分辨云模式及中国南海北部试验区加密探空的平均水平风场、位温场和水汽场模拟分析了1998年5月15日至6月11日中国南海北部地区中尺度对流系统(Mesoscal Convective System,简称MCS)中冰相相变潜热对云和降水、辐射传输以及大尺度环境场的影响作用。研究表明,冰相相变潜热总体上不会引起明显的大气辐射通量的变化,但会引起较明显的下垫面热通量的变化。凝华潜热释放显著地增加了大气稳定度,造成对流和下垫面热通量的减弱,从而导致地面降水减小10.11%。碰冻潜热释放也使得大气稳定度增加,不利于中尺度对流系统对流的发展,区域累积降水量减小2.2%。融化潜热的冷却效应,使得融化层以下的大气降温,从而增加了低层大气的不稳定性,有利于海面热通量的输送,导致MCS降水增加4.1%。因此,冰相相变潜热对降水的影响主要是通过影响大气环境稳定,进而影响洋面感热通量和潜热通量的垂直输送和对流的发展,导致区域降水改变。 相似文献
14.
In spring over the southern Bay of Bengal (BOB), a vortex commonly develops, followed by the Asian summer monsoon onset. An analysis of relevant data and a case study reveals that the BOB monsoon onset vortex is formed as a consequence of air–sea interaction over BOB, which is modulated by Tibetan Plateau forcing and the land–sea thermal contrast over the South Asian area during the spring season. Tibetan Plateau forcing in spring generates a prevailing cold northwesterly over India in the lower troposphere. Strong surface sensible heating is then released, forming a prominent surface cyclone with a strong southwesterly along the coastal ocean in northwestern BOB. This southwesterly induces a local offshore current and upwelling, resulting in cold sea surface temperatures (SSTs). The southwesterly, together with the near-equatorial westerly, also results in a surface anticyclone with descending air over most of BOB and a cyclone with ascending air over the southern part of BOB. In the eastern part of central BOB, where sky is clear, surface wind is weak, and ocean mixed layer is shallow, intense solar radiation and low energy loss due to weak surface latent and sensible heat fluxes act onto a thin ocean layer, resulting in the development of a unique BOB warm pool in spring. Near the surface, water vapor is transferred from northern BOB and other regions to southeastern BOB, where surface sensible heating is relatively high. The atmospheric available potential energy is generated and converted to kinetic energy, thereby resulting in vortex formation. The vortex then intensifies and moves northward, where SST is higher and surface sensible heating is stronger. Meanwhile, the zonal-mean kinetic energy is converted to eddy kinetic energy in the area east of the vortex, and the vortex turns eastward. Eventually, southwesterly sweeps over eastern BOB and merges with the subtropical westerly, leading to the onset of the Asian summer monsoon. 相似文献
15.
In this study, we first show that tropical cyclone (TC) Usagi evolved from a mid-level vortex over the South China Sea (SCS) in August 2001. The initial disturbance of TC Usagi had a maximum potential vorticity (PV) near 500 hPa, and an anticyclonic circulation with a cold core near the surface. The cyclonic circulation and its warm core of the mid-level vortex developed gradually downward toward the surface when environmental easterly and dry air intruded from the upper troposphere; finally, the mid-level vortex evolved into TC Usagi under favorable environment conditions such as weak vertical wind shear, deep moist layer, etc. To investigate the dynamic and thermodynamic processes during TC Usagi genesis, the technique of piecewise PV inversion is employed. The results show that the actions of upper-layer PV and potential temperature anomalies were not important in TC Usagi genesis. Surface-layer thermal anomalies mainly produced negative disturbances of temperature at the vortex center below 800 hPa, which was unfavorable to the genesis of a cyclonic circulation near the surface. Middle-to-lower-layer latent heat played a key role in TC Usagi genesis and downward development of dynamic and thermodynamic processes. The actions of dry air intrusion from the upper troposphere, environmental westerly changing into easterly in the middle and lower troposphere, and baroclinic structure of the vortex were also important. The cyclonic circulation of the mid-level vortex could develop downward quickly from the middle troposphere toward the surface. However, whether the warm core of the vortex developed near the surface depended on the combined actions of surface-layer thermal anomaly and middle-to-lower-layer latent heat. Finally, we present a conceptual model of TC Usagi genesis induced by a mid-level vortex over the SCS. 相似文献
16.
使用二维云分辨模式研究冰晶增长过程(云水到冰晶的冻结增长和通过水汽凝华冰晶到雪的增长)对热量收支的影响。采用4种冰晶增长参数化方案模拟了热带到中纬度地区的4个降水个例。研究发现:(1)高冰核浓度的ZENG方案和SHEN方案引起对流层中上层辐射加热增多,这与它们模拟的冰晶在对流层中上层增多有关。(2)高冰核浓度的ZENG方案导致模拟区域—平均的局地温度变化在对流层上层出现异常减小值,这与它在热带个例中导致垂直热量通量辐合减少和在中纬度个例中导致潜热加热减少有关。(3)尽管高冰核浓度的ZENG方案引起质量加权平均的辐射加热增多,但是它在热带个例中引起地表感热通量减少和在中纬度个例中引起潜热加热减少,最终导致4种参数化方案计算的模拟区域—质量加权平均的局地温度变化基本一致。 相似文献
17.
The studies in China on the formation of the summertime subtropical anticyclone on the climate timescale are reviewed. New insights in resent studies are introduced. It is stressed that either in the free atmosphere or in the planetary boundary, the descending arm of the Hadley cell cannot be considered as a mechanism for the formation of the subtropical anticyclone. Then the theories of thermal adaptation of the atmosphere to external thermal forcing and the potential vorticity forcing are developed to understand the formation of the subtropical anticyclone in the three-dimensional domain. Numerical experiments are designed to verify these theories. Results show that in the boreal summer, the formation of the strong South Asian High in the upper troposphere and the subtropical anticyclone over the western Pacific in the middle and lower troposphere is, to a great extent, due to the convective latent heating associated with the Asian monsoon, but affected by orography and the surface sensible heating over the continents.On the other hand, the formation of the subtropical anticyclone at the surface over the northern Pacific and in the upper troposphere over North America is mainly due to the strong surface sensible heating over North America, but affected by radiation cooling over the eastern North Pacific. Moreover, in the real atmosphere such individual thermal forcing is well organized. By considering the different diabatic heating in synthesis, a quadruple heating pattern is found over each subtropical continent and its adjacent oceans in summer. A distinct circulation pattern accompanies this heating pattern. The global summer subtropical heating and circulation may be viewed as “mosaics” of such quadruplet heating and circulationpatterns respectively. At last, some important issues for further research in understanding and predicting the variations of the subtropical anticyclone are raised. 相似文献
18.
热带太平洋-印度洋海温异常综合模的数值模拟 总被引：1，自引：0，他引：1
通过数值模拟及结果的合成分析,对热带太平洋-印度洋异常海温综合模态的三维热力结构、动力结构及其发生发展的可能机制进行了研究.数值模拟结果的分析表明,太平洋、印度洋海温异常的综合模态在表层、次表层的表现都很明显,即在赤道西印度洋、中东太平洋的海温偏高(低)时,赤道西太平洋、东印度洋的海温偏低(高),该模态还存在着显著的年变化特征、年际变化特征以及年代际变化特征.数值模拟的合成分析结果表明,异常的海表风应力引起表层洋流异常,表层洋流异常及由其引起的海表高度异常可导致次表层海水环流的异常,海洋环流异常导致的平流热输送异常是海温形成异常综合模态的主要原因之一,垂直输送是形成次表层海温综合模态的主要原因.平流热输送过程对海表温度变异的贡献是:在事件发生到盛期阶段促进了次表层海温异常综合模态的形成,在盛期到消亡阶段次表层的平流过程阻碍其进一步发展;短波辐射是海洋的主要热力来源,海表面异常的净短波辐射通量、潜热通量是表层海温形成异常模态的主要热力学原因,异常的海表面净短波辐射通量、潜热通量、感热通量在到达盛期阶段后抑制其进一步发展. 相似文献
19.
七月中、低纬地区定常波动和加热场的模拟特征 总被引：1，自引：0，他引：1
本文利用P-σ混合坐标原始分程球带模式的最新版本,对七月中、低纬地区的定常波动及非绝热加热场进行了数值模拟。结果表明,模式成功地模拟出了北半球夏季对流层中波数为2的定常波动。高层波峰出现在大陆,波谷出现在海洋上,低层则相反。南半球的副热带高压带也模拟出来了。降水量的模拟也是成功的,特别是位于ITCZ中的积云对流性降水。加热场的模拟结果指出,七月份的热源区除了主要分布在北半球的几个主要大陆上,还分布在热带海洋上ITCZ所在区;其余的广大洋面则显示出冷源的性质。其中热带海洋的热源以潜热加热为主(主要分布于大气的中高层),大陆上的热源有的以感热为主(主要分布于大气的低层),有的仍以潜热加热贡献较大。海洋的冷源是由长波辐射冷却造成的。 相似文献
20.
夏季我国干旱、半干旱区陆面过程能量平衡及其局地大气环流 总被引：28，自引：10，他引：18
利用NCEP资料分析得出,夏季我国干旱,半干旱区在整个欧亚大陆上是陆面感热通量最强的地方,与此对应的陆面潜热通量则最弱.陆面所接收的太阳短波辐射主要以感热和长波辐射的能量形式释放.该区降水量很少,降水量的年际变率也很弱;因此,该区的陆面热量通量都显出很弱的年际变率;然而,这些通量的年代际变率信号则比较显著.我国干旱、半干旱区大气环流的热力过程与其陆面过程特征密切相关.该区对流层大气的辐射冷却很强,达-3 K d-1.由于缺乏水汽和上升运动,大尺度凝结加热率、深对流加热率、浅对流加热率都非常弱.因此,600hPa以上的大气以绝热下沉加热来平衡辐射冷却;600hPa以下,陆面感热引起的垂直扩散加热率非常强,多达8 K d-1,它除了平衡辐射冷却以外还制造对流层低层的对流运动,以绝热上升冷却来平衡多余的垂直扩散加热.总之,我国干旱、半干旱区的陆面过程特征决定了该区大气运动的特殊垂直结构,即对流层低层对流上升运动及其上层的下沉运动.我国干旱、半干旱区陆面能量平衡及其局地大气环流的年代际变率,是全球气候系统年代际变率的必然结果. 相似文献