青藏高原对其东北侧干旱形成的数值试验

应用再分析资料，指出高原边界层内存在北高南低偶极子型涡旋对的独特气候现象。根据当雄站1998年5月31日至6月4日感热通量的连续观测资料，确定了高原热力作用的时变特征，分别用不同的理想高原初始涡度场加定常热源强迫和时变热源强迫代入正压准地转涡度模式，研究了高原东北侧干旱的形成。认为有三种过程在起着重要作用，它们是：基流对上游反气旋涡旋的平流输送、南侧气旋涡旋的能量频散以及高原热力强迫引起的频散生成高值系统的增强。     

Dynamical and Thermal Problems in Vortex Development and Movement. Part I: A PV–Q View

Based on the Lagrangian change equation of vertical vorticity deduced from the equation of threedimensional Ertel potential vorticity(PV e),the development and movement of vortex are investigated from the view of potential vorticity and diabatic heating(PV-Q).It is demonstrated that the asymmetric distribution in the vortex of the non-uniform diabatic heating in both vertical and horizontal can lead to the vortex’s development and movement.The theoretical results are used to analyze the development and movement of a Tibetan Plateau(TP) vortex(TPV),which appeared over the TP,then slid down and moved eastward in late July 2008,resulting in heavy rainfall in Sichuan Province and along the middle and lower reaches of the Yangtze River.The relative contributions to the vertical vorticity development of the TPV are decomposed into three parts:the diabatic heating,the change in horizontal component of PV e(defined as PV 2),and the change in static stability θ z.The results show that in most cases,diabatic heating plays a leading role,followed by the change in PV 2,while the change of θ z usually has a negative impact in a stable atmosphere when the atmosphere becomes more stable,and has a positive contribution when the atmosphere approaches neutral stratification.The intensification of the TPV from 0600 to 1200 UTC 22 July 2008 is mainly due to the diabatic heating associated with the precipitation on the eastern side of the TPV when it uplifted on the up-slope of the northeastern edge of the Sichuan basin.The vertical gradient of diabatic heating makes positive(negative) PV e generation below(above) the maximum of diabatic heating;the positive PV e generation not only intensifies the low-level vortex but also enhances the vertical extent of the vortex as it uplifts.The change in PV e due to the horizontal gradient of diabatic heating depends on the vertical shear of horizontal wind that passes through the center of diabatic heating.The horizontal gradient of diabatic heating makes positive(negative) PV e generation on the right(left) side of the vertical shear of horizontal wind.The positive PV e generation on the right side of the vertical shear of horizontal wind not only intensifies the local vertical vorticity but also affects direction of movement of the TPV.These diagnostic results are in good agreement with the theoretic results developed from the PV-Q view.     

青藏高原上中尺度对流系统(MCS)的数值模拟

A mesoscale convective system (MCS) developing over the Qinghai-Xizang Plateau on 26 July 1995 issimulated using the fifth version of the Penn State-NCAR nonhydrostatic mesoscale model (MM5). Theresults obtained are inspiring and are as follows. (1) The model simulates well the largescale conditionsin which the MCS concerned is embedded, which are the well-known anticyclonic Qinghai-Xizang PlateauHigh in the upper layers and the strong thermal forcing in the lower layers. In particular, the modelcaptures the meso-α scale cyclonic vortex associated with the MCS, which can be analyzed in the 500 hPaobservational winds; and to some degree, the model reproduces even its meso-β scale substructure similarto satellite images, reflected in the model-simulated 400 hPa rainwater. On the other hand, there aresome distinct deficiencies in the simulation; for example, the simulated MCS occurs with a lag of 3 hoursand a westward deviation of 3-5° longitude. (2) The structure and evolution of the meso-α scale vortexassociated with the MCS are undescribable for upper-air sounding data. The vortex is confined to thelower troposphere under 450 hPa over the plateau and shrinks its extent with height, with a diameter of4° longitude at 500 hPa. It is within the updraft area, but with an upper-level anticyclone and downdraftover it. The vortex originates over the plateau, and does not form until the mature stage of the MCS. Itlasts for 3-6 hours. In its processes of both formation and decay, the change in geopotential height fieldis prior to that in the wind field. It follows that the vortex is closely associated with the thermal effectsover the plateau. (3) A series of sensitivity experiments are conducted to investigate the impact of varioussurface thermal forcings and other physical processes on the MCS over the plateau. The results indicatethat under the background conditions of the upper-level Qinghai-Xizang High, the MCS involved is mainlydominated by the low-level thermal forcing. The simulation described here is a good indication that itmay be possible to reproduce the MCS over the plateau under certain large-scale conditions and with theincorporation of proper thermal physics in the lower layers.     

台风活动对青藏高原东北侧干旱的影响

应用１９５９￣１９９６的青藏高原东北侧５８个站历年逐月降水量资料,历年（１９５０￣１９９６年）逐月西太平洋台风资料及５００ｈＰａ高度格点资料,分析了台风活动对高原东北侧干旱的影响。结果指出：少台风活动年与干旱环流流型及高原东北侧干旱之间,多台风活动年与多雨环流流型及高原东北侧多雨之间,均存在着对应关系。     

华南持续性强降水期间低频非绝热加热对低频环流的影响

利用站点降水资料和再分析资料针对华南地区5—8月的持续性强降水过程,分析了低频异常非绝热加热的时空分布特征及其对低频大气环流的可能反馈作用。得到如下结论:5—6月和7—8月华南持续性强降水期间10—30 d低频非绝热加热的演变特征有所不同,5—6月持续性强降水发生前低频非绝热加热大值区从30°N(107°—115°E)以北向南传播发展至华南地区,而在7—8月降水前非绝热加热大值区从中国南海中部向西北方向传播,并在降水最强盛期到达华南。异常环流型控制着持续性强降水的强度和位置,从而决定异常凝结潜热的演变特征。异常凝结潜热则是通过影响涡度倾向变化而对大气环流有一个反馈作用。对于发生在华南5—6月和7—8月的这2组持续性强降水过程,当降水处于发展阶段,在低频非绝热加热作用项和低频涡度平流项的共同作用下,华南上空中层存在显著的10—30 d低频正涡度倾向变化,有利于低频气旋式环流的进一步发展。非绝热加热作用项主要由加热率的垂直梯度决定,涡度平流项则与气候背景风场有密切关系。5—6月持续性强降水期间涡度平流项位于非绝热加热项东侧,而7—8月持续性强降水期间涡度平流项位于非绝热加热项北侧。在持续性强降水的衰亡期,由于非绝热加热项和涡度平流项转为负值,华南被负涡度倾向变化控制,低频气旋式环流迅速消亡。     

非绝热加热对热带气旋非对称结构影响的数值试验

利用含非绝热加热强迫的正压涡度方程。将非绝热加热作适当的参数化处理。对初始对称 热带气旋作了一系列数值试验,结果表明：不仅β项、平流项在热带气旋非对称结构的形成中有重要作用,而且非绝热加热对热带气旋的非对称结构亦有重要影响,从而验证了非绝热加热是热带气旋非对称结构形成的一种可能机制的结论。     

青藏高原大地形作用下的Rossby波

在对青藏高原大地形的动力和热力作用物理分析的基础上,着重分析了青藏高原地形坡度和非绝热和非绝热加热对二维Ｒｏｓｓｂｙ波的影响。研究指出：高原地开坡度对Ｒｏｓｓｂｙ波的作用与Ｒｏｓｓｂｙ参数的作用相当,而且其相速度和群速度之间存在一个圆的关系：（ｃｇｘ－ｃｘ）＾２＋ｃｇｙ＾２＝Ｒ＾２;高原加热作用与水平辐合作用相当。地形坡度和非绝热加热都有使二维Ｒｏｓｓｂｙ波向低频发展的的趋向。     

赤道反气旋的合成结构和涡度收支

本文通过普查1979—1983年7—9月在10°S—15°N、90°E—140°E范围内的赤道反气旋活动情况,从中选出15个强度和范围较接近的赤道反气旋进行综合分析,得到它们的平均三维结构特征。结果表明,赤道反气旋是一个暖性的中低层系统。反气旋环流与涡度、散度及垂直运动有较好的配合。在赤道反气旋的低层,环流中心为负涡度区和辐散区,并与下沉运动区相对应,四周为正涡度和辐合区,以及上升运动区。高层正好相反。加热场与垂直运动场有较好的对应关系,中心区是干绝热下沉增温区。对涡度收支的计算表明,中低层有负涡度积累,上层有正涡度积累,局地涡度变化主要决定于散度项、平流项和垂直输送项。      

夏季南亚高压多中心特征及其热力影响因子分析

采用美国NCEP/NCAR I、NCEP/DOE II和日本气象厅JRA-55（Japanese 55-year Reanalysis Project）的月平均环流场和非绝热加热场资料,分析了夏季南亚高压多中心结构特征,探讨了不同区域高压中心的动力和热力结构,及其与不同地区热源的关系。结果表明:（1）夏季南亚高压存在显著多中心特征,可达5～6个,其中双中心类和三中心类占比例最多,约70%～80%,其次,单中心类和四中心类分别约占10%左右。（2）无论中心个数的多或少,不同区域的南亚高压中心的动力结构和热力结构不同,大致可以分为三个区域20°～70°E、80°～120°E和120°～160°E。20°～70°E伊朗高原及其以西上空南亚高压中心中层对应伊朗副高的东北侧,低层对应印缅槽的西北部,整层为下沉运动;80°～120°E青藏高原到我国东部上空南亚高压中心低层对应印缅槽中部,低层正涡度高层负涡度,整层为强上升运动;120°～160°E西太平洋地区南亚高压中心中低层都对应西太平洋副热带高压的西部,整层负涡度,对应上升运动。（3）三个区域的高压中心都对应着暖中心结构,20°～70°E区域以下沉增温加热为主导,80°～120°E和120°～160°E区域以深对流加热为主导。（4）当20°～70°E、80°～120°E和120°～160°E区域存在高压中心时,对应区域的南亚高压环流的增强,对局地环流、深对流和降水有着显著的影响。     

利用空间均匀网格对中国夏季降水异常区域特性的初步分析

用方差极大正交转动ＥＯＦ（Ｖａｒｉｍａｘ　ＥＯＦ）及点相关图法分析了夏季总降水（６、７、８月降水之和）及逐月降水的区域特性。使用的资料为全国范围４７个５°×５°经纬度网格上的降水资料，分析时段为１９５９—１９９４年。分析结果表明，由于采用了空间均匀的格同资料，本分析除进一步证实了中国东部地区降水异常的区域特性外，也揭示了西部地区降水异常的区域特性及沿长江流域东西方向上降水异常的相互关系。夏季总降水异常最显著的区域特性是江淮流域与河套及华南反相关。另外沿长江流域，四川盆地的降水异常与青藏高原东部及江淮流域的降水异常也存在着反相关联系。西部地区的区域特性为青藏高原中东部南北两侧为负相关，并且青藏高原中东部南侧的降水异常与华北东部及东北南部为正相关。上述的空间模都有准２—３ａ及１０ａ左右的周期。逐月降水的分析表明，６月份，江淮流域、华北东部及东北大部分地区为正相关。７月，河套地区与江淮流域的降水异常呈现一定的负相关联系，８月份降水异常的区域特性与夏季总降水异常的区域特性极其一致。     

北半球冬季副热带高压带维持的涡度机制

本文利用涡度平衡方程讨论北半球冬季副热带高压的维持,计算发现,30°N副热带高压带地区,大型扰动所造成的涡度输送的辐散是维持这地区反气旋涡度的主要因子,这种辐散作用所造成的反气旋涡度主要发生在对流层上层,平均经圈环流对地转祸度的输送可以把它引导到对流层下层来。此外,我们还根据涡度输送的计算,讨论了西风急流的维持。向北的扰动涡度输送在45°N上空达极大值,因此它对中纬度西风和纬向平均急流的维持起着重要作用。但30°N上空,扰动的涡度输送为零,而平均经圈环流对地转涡度和相对涡度的输送都比较大,因此,可以认为副热带急流是在平均经圈环流作用下维持的。     

MAIN HEATING MODES OVER THE TIBETAN PLATEAU IN JULY AND THE CORRELATION PATTERNS OF CIRCULATION AND PRECIPITATION OVER EAST ASIA*

Based on the 1958-1999 monthly averaged NCEP/NCAR reanalysis data,the REOF analysis is applied to obtain the main spatial modes of normalized atmospheric heating source over the Tibetan Plateau(TP) in July.Results show that the four leading modes are located over the northeast TP,southwest TP.Kashmir and southeast TP respectively,and the cumulative variances are no more than one third of the total.It indicates that the heating source distribution is very complicated over the TP in July.In other words.it is difficult to depict the heating spatial distribution with a few modes.By using wavelet analysis,a 2-4-year variation period is identified in these modes.Moreover,correlation coefficients between each RPC and zonal wind U, meridional wind V.zonal moisture flux Q_v,meridional moisture flux Q_v,and precipitation rate over East Asia are calculated to construct correlation fields,Results show that different heating modes over the TP correspond to different circulation,moisture flux as well as precipitation patterns,Precipitation over North China(or Kashmir) is negatively(or positively) correlated with REOF1.Similarly.notable negative(or positive) correlation can be found between the rainfall over south part of Southwest China.South China,and the Philippines(or Japan) and the REOF3. Due to high localization of diabatic heating over the TP.it is not enough to study the influence of TP thermal forcing on the climate with an area averaged heating index.     

青藏高原动力和热力作用对季节转换期全球大气环流影响的数值研究

利用ＣＣＭ１（Ｒ１５Ｌ７）－ＬＮＷＰ模式,以１９９６年３月１７日的国家气象中心客观分析资料为初始场,分别采用有、无青藏高原两种方案,数值研究了青藏高原对５月份全球大气环流季节转换的影响。试验结果表明：北半球初夏,青藏高原区域用同纬度地区的一个中空热源,其作用可以在２００ｈＰａ层形成一个２２４Ｋ的暖中心,使大气增暖７Ｋ以上。高原地形的动力和非绝热作用使得南极大陆２００ｈＰａ层大部分地区降温６Ｋ左右,最大负中心可达－８．２８Ｋ,这对于南半球由夏至冬过程中,环极涡旋的强度加深和范围扩大是有利的。高原地形作用对北半球大气环流平均槽脊的形成和维持有十分重要的影响,它加强了高原所在纬度带北侧（减弱了南侧）由南向北的正温度梯度,同时也增强了３０°Ｓ附近由北向南的正温度梯度,从而有利于季节转换过程中全球中纬西风带的整体北移和初夏亚洲季风环流的形成。同时高原地形作用在赤道及低纬地区形成的位势增加区,有利于南半球热带高压脊的北退和北半球副高增强北移。此外,它还有利于南半球极地东风带的增强和５００ｈＰａ层环极低压带的强度减弱,同时增加了罗斯海附近的极涡强度,对赤道的索马里急流的形成也有重要影响     

IMPACT OF AIR-SEA INTERACTION ON THE GENESIS OF TROPICAL INCIPIENT VORTEX OVER SOUTH CHINA SEA: A CASE STUDY

Based on 6-hourly sensible heat flux and latent heat flux from the NCEP Climate Forecast System Reanalysis (CFSR) and circulation data from the Japanese 25-year Reanalysis (JRA-25), the initial developing process of tropical cyclone Mindulle (1005) in 2010 has been diagnosed to reveal the impact of air-sea interaction over the South China Sea (SCS) on the genesis of its incipient vortex. The results show that the incipient vortex first occurred east of the Luzon Island on 0000 UTC 20 August, suggesting that the topographic forcing of the Luzon Island for easterly winds over the western Pacific might be one of the factors responsible for the formation of the incipient vortex. During the formation stage of the incipient vortex, strong southeasterlies over the SCS caused warm water of the middle and eastern SCS to flow toward the Luzon Island due to Ekman transport resulting from wind stress, leading to an increase of the sea surface temperature and sensible heat flux into the atmosphere. Although the anomalous sensible heating favored surface pressure to reduce, it was not conducive to the increase of local vorticity associated with the vortex above the heating area because, according to the atmospheric thermal adaptation theory, the anticyclonic vorticity would be created in the lower troposphere due to the decreased vertical gradient of the sensible heating. However, the ascending motions occurred over the eastern area of the anomalous sensible heating due to the augmentation of the vorticity advection with increasing height, causing water vapor to condense in the middle and upper troposphere. In turn, cyclonic vorticity was generated in the lower troposphere due to the increased vertical gradient of the condensation latent heating, resulting in the formation and further growth of the incipient vortex. Therefore, the vorticity creation due to the condensation heating played a dominant role during the subsequent enhancing stage of the incipient vortex.     

Dynamic and Numerical Study of Waves in the Tibetan Plateau Vortex简

In terms of its dynamics, The Tibetan Plateau Vortex （TPV） is assumed to be a vortex in the botmdary layer forced by diabatic heating and friction. In order to analyze the basic characteristics of waves in the vortex, the governing equations for the vortex were established in column coordinates with the balance of gradient wind. Based on this, the type of mixed waves and their dispersion characteristics were deduced by solving the linear model. Two numerical simulations with triple-nested domains--one idealized large-eddy simulation and one of a TPV that took place on 14 August 2006---were also carried out. The aim of the simulations was to validate the mixed wave deduced from the governing equations. The high-resolution model output data were analyzed and the results showed that the tangential flow field of the TPV in the form of center heating was cyclonic and convergent in the lower levels and anticyclonic and divergent in the upper levels. The simulations also showed that the vorticity of the vortex is uneven and might have shear flow along the radial direction. The changing vorticity causes the formation and spreading of vortex Rossby （VR） waves, and divergence will cause changes to the n~otion of the excitation and evolution of inertial gravity （IG） waves. Therefore, the vortex may contain what we call mixed ：inertial gravity-vortex Rossby （IG-VR） waves. It is suggested that some strongly developed TPVs should be studied in the future, because of their effects on weather in downstream areas.     

青藏高原地表热状况的卫星资料分析

在云辐射强迫→地表热力强迫→气候变化→云辐射强迫这一反馈过程中,地表热力过程是一个要环节。青藏高原地表热状况集中集现了青藏高热力作用的基本状态,因而 热力强迫作用下的气候变化如降水、季风等密切相关。因此,研究青藏高原地表热状况的变化,对深入了解青藏高原热力作用及其对周边气候环境的影响,进而对气候变化预测有重要意义。本文利用１９８３年７月至１９９０年１２月菜９０个月的ＩＳＣＣＰ－Ｃ２卫星观测地表温度     

7月青藏高原大气热源空间型及其与东亚大气环流和降水的相关研究

对1958～1999年的7月份NCEP/NCAR再分析资料中青藏高原区域大气热源强度(整层气柱的总非绝热加热率)做旋转经验正交函数分析,结果表明该区域内大气热源强度的空间分布特征复杂,各地差异显著。前4个REOF型的加热中心位于高原东北部、高原西南部、克什米尔地区以及高原东南部地区上空。小波分析还表明各空间型都有2～4a的变化周期。文中计算了前4个RPC与东亚中、低空纬向风(U)、经向风(V)、纬向水汽通量(Q_u)、经向水汽通量(Q_v)的相关系数,并用这些相关系数构造矢量,进而分析其流场和水汽通量散度场,发现高原不同区域的大气加热异常所对应的东亚大气环流形势及降水也大不相同,由此表明,在研究高原加热对中国气候的影响时,应注意加热的空间分布特征。     

冷空气对高原低涡移出青藏高原的影响

在对1998—2004年冷空气影响高原低涡移出青藏高原 (以下简称高原) 观测事实分析的基础上, 利用NCEP再分析资料对2002年8月12—14日托勒低涡移出高原的位涡进行诊断分析, 并通过数值试验揭示了托勒低涡移出高原的冷空气侵入特征和影响机理。结果表明:这次托勒低涡是受我国东北冷空气影响, 有高位涡空气伸入低涡区, 使冷空气迫近暖湿空气, 低涡处在斜压不稳定增强情况下移出高原的。在低涡区域没有冷空气或我国东北不存在冷温度槽情况下, 将会使伸向高原东北部的冷空气主力偏东、减弱, 使低涡受到我国东北冷空气影响减弱, 斜压不稳定减弱, 从而使高原低涡移出高原的速度减慢, 低涡强度减弱, 尤其是我国东北冷温度槽的影响更为明显, 在我国东北没有冷温度槽存在的情况下, 低涡24 h内西退, 在高原边缘徘徊。     

青藏高原东北侧干旱的数值试验

用谱方法（Ｔ４２）求解半球球面无辐散正压涡度方程,采用实际的干旱环流资料,分别在有地形和无地形的情况下,求出其对应的干旱环流型的强迫场,模拟了在强迫场的作用下干旱环流的形成、维持情况及在强迫场消失后干旱环流型的崩溃情况。结果表明：（１）强迫场在干旱环流型的形成、维持及崩溃过程中起重要作用;（２）青藏高原的存在使其东北侧干旱形成和崩溃均加快。