共查询到18条相似文献，搜索用时 305 毫秒
1.
2.
在位涡的基础上,考虑散度效应,把水平风矢量旋转90°后的旋度在广义位温梯度方向上的投影定义为位势散度,并把其二阶扰动量定义为位势散度波作用密度,该波作用密度代表扰动热量的扰动输送,与位势稳定度的发展演变有关.登陆台风Morakot(2009)的诊断分析表明,在台风登陆台湾岛,进入台湾海峡和登陆大陆三个阶段,波作用密度高值区与大陆和台湾降水区相重叠,扰动热量的扰动输送显著;在前两个阶段,大陆和台湾降水区波作用密度逐渐增大,扰动热量的扰动输送逐步增强;在台风登陆福建霞浦市后,大陆地区波作用密度减小,扰动热量的扰动输送减弱.在影响波作用密度局地变化的诸多物理因素中,扰动非地转风位涡项是主要强迫项.统计分析表明,波作用密度与观测降水有一定的相关性,据此发展了位势散度波作用密度降水预报方程,其本质是数值模式预报资料的动力延伸释用,预报应用表明,利用24 h模式预报场计算的波作用密度降水能够较好地再现观测降水的落区,对台风Morakot引发的暴雨有一定的预报技巧. 相似文献
3.
《中国科学:地球科学》2020,(9)
文章回顾了近年来发展的全球大气环流的三型分解理论,主要包括全球大气环流三型分解模型及全球大尺度水平型环流、经圈型环流和纬圈型环流的动力学方程组理论.与传统二维环流分解方法的对比表明:全球大气环流三型分解将垂直涡度中由水平涡旋运动与辐合辐散运动引起的垂直涡度分量有效地分解开来,也将垂直速度中的经向垂直环流与纬向垂直环流分量分解开来,为研究辐合辐散过程对垂直涡度场的演变作用及局地垂直环流的准确描述问题提供了新的方法.全球大气环流的三型分解是一种基于实际大气运动特征的三维环流分解方法,其分解后的水平型、经圈型以及纬圈型环流可分别看作是中高纬度Rossby波及低纬度Hadley和Walker环流在全球的推广.因此,新的环流分解模型及其动力学方程组为中高纬度大气环流与低纬度大气环流之间的相互作用问题研究以及全球变暖背景下大尺度环流异常演变的物理机制问题研究提供了新的理论与方法. 相似文献
4.
5.
2006年7月19-24日,东北地区出现一次明显的冷涡发展导致强降水的过程.对这次东北冷涡过程的天气形势分析表明,该东北冷涡的维持和发展与冷涡东部阻塞高压的建立与消亡有关.本文根据500 hPa环流形势演变特征,将东北冷涡发生发展过程分为4个阶段,并借助调和-余弦谱展开方法,对东北冷涡各阶段850 hPa水平风和水汽通量进行无辐散和无旋转分量分解,分析各阶段无旋转风动能和无辐散风动能之间的能量转化.研究结果表明,分解得到的无辐散风及其水汽通量清楚地展现出了东北冷涡的大尺度环流和水汽输送通道及水汽来源,而从无旋转风及其水汽通量上则可以直观地看到冷涡低层的中小尺度风场及水汽辐合辐散区,为分析东北冷涡内部对流提供帮助.东北冷涡发展的不同阶段其水汽来源有所不同,初始阶段的水汽主要来自黄海和渤海地区,发展阶段水汽主要来自日本海,而到成熟阶段和减弱阶段,水汽输送通道被破坏,冷涡的水汽供应大大减少,与同时期暴雨减弱一致.同时,无旋转风辐合强值区和无旋转风水汽通量大值区的重合区域有利于强对流的发生发展,表现为重合区与TBB(Temperature of Black Body,黑体辐射温度)强对流云带的形状和位置对应良好,与降水落区也较为一致,可为预报东北冷涡引发的强降水落区这一预报难点问题提供参考.从动能转化上看,无旋转风和无辐散风的动能转化项能很好地反映东北冷涡整个生命史过程中各阶段强度的变化特点,对冷涡强度预报具有一定的指示意义. 相似文献
6.
本文分析长时间强度维持"菲特"台风不同发展阶段的位涡分布特征发现：台风内核区中尺度高值PV带及其变化与台风强度变化具有伴随关系,即高值PV区与内核区强对流不仅具有对应关系;而且其生命史与台风强盛维持期一致;此外在眼墙区附近位涡梯度最大.分析还指出：垂直剖面上的高值PV呈现由单极位涡态（台风发展加强期）向中空位涡态（台风强盛维持期）的转变,到台风快速衰减期,又形成PV量值较小的单极位涡态.位涡收支方程诊断表明：内核区域水平平流、垂直输送和凝结加热的初始增强和大值收支带不仅对台风内中尺度高值位涡分布及长时间强度维持具有重要影响,而且具有伴随关系.此外,位涡收支各项对位涡态的转变起着不同的作用,其中凝结加热在台风强盛期中空位涡塔的建立中作用明显,水平平流项则在眼墙区的位涡塔中上层有着正贡献,垂直输送在高值PV分布的再分配中起中介作用. 相似文献
7.
8.
本文利用中尺度模式WRF V3.9对2016年7月16日成都一次污染天气下的城市热岛环流个例进行了数值模拟,分析了城市热岛环流的三维结构及演变特征.并通过设计减少气溶胶光学厚度的敏感性试验,研究了污染对城市热岛环流的可能影响.结果表明:当地时间17∶00城市热岛环流开始形成.随着热岛强度增强,环流增强,城乡边界处的城市风锋不断向城市中心推进.19∶00热岛环流结构最显著.21∶00环流结构被破坏,仅低层存在微弱的乡村风.在热岛环流结构最显著时刻,近地面风场由郊区向城市辐合,地面以上2.0km处风场由城市向乡村辐散,辐散中心与辐合中心位置大致对应.此时城市风锋在城市处合并,环流的水平尺度约为城市尺度的2～2.5倍.当气溶胶光学厚度减小后,城市热岛环流尺度和强度以减小为主.特别是在热岛环流最显著时刻,低层乡村风风速减小,城市风锋最大上升速度降低,环流的水平尺度在西、南、北三个方向均减小,且高空回流高度降低.可能的影响机制是,气溶胶光学厚度减小后,净辐射通量增大,城乡地表能量通量差异增大,城市边界层高度升高.但城市边界层高度升高对城市热岛的抑制作用超过了城乡地表能量通量差异增加对城市热岛的增强作用,最终造成城市热岛减弱,环流减弱. 相似文献
9.
地面摩擦和大尺度流场是影响锋面气旋结构演变的重要因子,本文使用WRF模式并采用湿物理方案,通过理想化试验,综合考虑陆面摩擦、气旋式扰动相对于急流位置和大尺度流场对锋面气旋结构变化的影响.结果表明：当仅考虑单一因子时,气旋式扰动位于急流南侧和辐合流流场有利于气旋形成Shapiro-Keyser（S-K）模型结构.当同时考虑地面摩擦和大尺度辐合时,气旋式扰动位于急流北侧的气旋发展整体向经典的挪威气旋模型转变;扰动位于急流南侧的的气旋发展则整体呈现S-K模型结构,此时辐合流场有利于S-K模型结构出现.当同时考虑地面摩擦和大尺度辐散时,扰动处于急流北侧的气旋呈现挪威气旋模型结构;由于气旋式扰动穿越急流和辐散流场同时有利于暖锋后弯发展以及冷暖锋距离加大和锋消,扰动处于急流南侧的气旋呈现典型S-K气旋模型结构.这个结果解释了在东亚大陆地区辐散场形势下出现的S-K模型结构气旋个例. 相似文献
10.
观测的大气流场可以物理分解为气候流场、行星尺度纬圈平均扰动流场和天气尺度扰动流场.低层大气的天气尺度扰动流场中的切变线、南方气旋、北方气旋、冷锋槽线、西南涡暖切变线、热带气旋、倒槽切变线、东风波切变线等对区域暴雨具有指示意义.扰动流场中的环流系统更适合天气分析的原理.中国的暴雨带多为扰动辐合线两侧气流对峙的结果.观测流场中,暴雨带出现在低空急流的左侧,是因为气候流场掩盖或削弱了天气尺度扰动流场的作用.对切变线暴雨,天气尺度扰动流场有99%的诊断能力,而原始流场只有66%的指示能力. 相似文献
11.
Using the improved CCM1 dynamic climate model, the impact of abnormal heat source and sink over the Tibetan Plateau in winter on the abnormal zonal wind over the Pacific Ocean is studied in this paper. The following new-findings are obtained: (1) When the at mospheric cold source during January—March on the Tibetan Plateau gets intensified, an abnormal anticyclone around the Tibetan Plateau will appear in lower troposphere. Abnormal northerly wind at the coastal area of the mainland of China and an abnormal cyclone will appear on the West Pacific in the following months. Then, abnormal west wind will appear over the equator of the West Pacific and extends to the East Pacific. (2) When the atmospheric cold source during January—March over the Tibetan Plateau is unusually weak, an abnormal cyclone around the Tibetan Plateau will appear at lower levels first, then abnormal anticyclone will appear on the West Pacific and move to the south and result in abnormal easterly wind over the equator of the West Pacific, which will extend to the east. Furthermore, abnormal changes of zonal wind on equatorial Indian Ocean can be caused by the intensity change of atmospheric cold source in winter and early spring over the Tibetan Plateau.
相似文献12.
本文应用欧洲中期预报中心（ECMWF,European Centre for Medium\|Range Weather Forecasts—ERA\|40）资料和美国国家环境预测中心和国家大气研究中心(NCEP/NCAR, National Centers for Environmental Prediction/National Center for Atmospheric Research)资料,研究了青藏高原雪深变化对南海夏季风爆发的影响和ENSO对青藏高原降雪的影响.结果表明：（1）ECMWF的雪深资料是可信的,可以用来研究青藏高原雪深变化对南海夏季风爆发的影响;（2）青藏高原的积雪异常影响到500 hPa以上的温度异常和印度洋与大陆间的气温对比,一方面使上层的南亚高压移动速度发生变化,另一方面也影响到低层大气的运动和东西向风异常,在青藏高原少雪年,东印度洋产生西风异常和一个气旋对,而在青藏高原多雪年,东印度洋产生东风异常和一个反气旋对;（3）ENSO与青藏高原春季积雪关系密切.东太平洋SST正异常时,东印度洋和南海气压偏高,从而导致该区海陆经向压强梯度增强和西风异常.另外,此时青藏高原北部气压偏高,北风偏强,副热带锋面增强,同时,印度洋的SST偏高,为青藏高原降雪提供了水汽保障,这些都有利于青藏高原的降雪. 相似文献
13.
14.
采用有限元方法模拟了近20万年来青藏高原岩石圈形变演化过程，探讨了印度-欧亚大陆的碰撞对中国大陆岩石层形变和应力场的影响以及它们与强地震活动性的关系.结合现代GPS、地震和地质学观测的结果，对比分析了中国大陆在百万年、十万年和十年尺度上的形变和构造应力场的基本格局.研究表明：（1）印度-欧亚大陆的碰撞以及印度大陆的持续向北推进、挤压所产生的应力环境，一直主导了以青藏高原为核心的我国西部地域岩石圈构造、运动和演化，但其影响随着远离青藏高原地区而逐渐变小.（2）断层滑移和重力势作用对于青藏高原东西部以及塔里木盆地的影响相当大，它们导致青藏高原岩石层东西向形变速率增大，对青藏高原的中南部地区产生拉张效应，同时导致塔里木盆地出现整体的右旋趋势.（3）青藏高原区域水平方向形变速率和GPS观测结果吻合较好.但在垂直方向上，一些地区计算结果与观测数据相差较大，这说明单纯的挤压作用不是现代青藏高原隆升的惟一机制.现代青藏高原的隆升可能与其他驱动机制，如地幔对流、重力均衡以及剥蚀作用等有关.（4）印度板块的挤压作用基本上决定了中国大陆西部的主压应力场分布.（5）印度板块的碰撞对中国大陆的强地震活动性有重要影响，但华北地区是个例外，该地区的地震活动性很强而印度板块的挤压在该区域产生的影响却很小，说明其他的驱动力在一定程度上活化了华北地块. 相似文献
15.
Upper crustal deformation characteristics in the northeastern Tibetan Plateau and its adjacent areas revealed by GNSS and anisotropy data 
下载免费PDF全文
下载免费PDF全文 The northeastern part of the Tibetan Plateau is a region where different tectonic blocks collide and intersect, and large earthquakes are frequent. Global Navigation Satellite System (GNSS) observations show that tectonic deformation in this region is strong and manifests as non-uniform deformation associated with tectonic features. S-wave splitting studies of near-field seismic data show that seismic anisotropy parameters can also reveal the upper crustal medium deformation beneath the reporting station. In this paper, we summarize the surface deformation from GNSS observations and crustal deformation from seismic anisotropy data in the northeastern Tibetan Plateau. By comparing the principal compressive strain direction with the fast S-wave polarization direction of near-field S-wave splitting, we analyzed deformation and its differences in surface and upper crustal media in the northeastern Tibetan Plateau and adjacent areas. The principal compressive strain direction derived from GNSS is generally consistent with the polarization direction of fast S-waves, but there are also local tectonic regions with large differences between them, which reflect the different deformation mechanisms of regional upper crustal media. The combination of GNSS and seismic anisotropy data can reveal the depth variation characteristics of crustal deformation and deepen understanding of three-dimensional crustal deformation and the deep dynamical mechanisms underlying it. it. 相似文献
16.
Evidence from the eastern Indian Ocean implies a Greater India in Gondwanaland. Translated without distortion to Asia, the northeast part of Greater India is found to correspond in shape with the Tibetan Plateau. With geophysical evidence, this suggests that the northeast part of Greater India underlies, presumably by underthrusting, the Tibetan Plateau. 相似文献
17.
A comprehensive physical pattern of land-air dynamic and thermal structure on the Qinghai-Xizang Plateau 总被引：11，自引：1，他引：11
According to the boundary layer observations of three stations (Garze, Damxung and Qamdu) and relevant earth satellite, radiosonde and surface observations during the intensive observational period (IOP) of the second Tibetan (Qinghai-Xizang) Plateau Experiment of atmospheric science (TIPEX), the land-air physical process and dynamic model on the Tibetan Plateau were comprehensively analyzed in this study. The dynamic characteristics of boundary layer and the rules of turbulent motion on the plateau were illustrated. The characteristics of distributions of wind speed and direction with mutiple-layer structure and deep convective mixed layer on the plateau, the strong buoyancy effect in turbulent motion on the plateau on which the air density is obviously smaller than on the plain, and the Ekman spiral and its dynamic pump effect of the plateau deep boundary layer have been found. The local static distribution of water vapor and the horizontal advection of water vapor in the plateau boundary layer were studied. The abnomal thermodynamic structure on the plateau surface and boundary layer, including the plateau strong radiation phenomenon and strong heating source characteristics of the middle plateau, was also analyzed. The authors synthesized the above dynamic and thermodynamic structures of both surface and boundary layers on the plateau and posed the comprehensive physical model of the turbulence and convective mixture mechanism on the plateau boundary layer. The characteristics of formation, development and movement for convective cloud cluster over the plateau influencing floods in the Yangtze River area of China were studied. The conceptual model of dynamic and thermodynamic structures of turbulent motion and convective plume related to the frequent occurrence of "pop-corn-like" cloud system is given as well. 相似文献
18.
A simple model of fluid particle advection induced by the interaction of a point vortex and incident plane flow occurring near a curved boundary is analyzed. The use of the curved boundary in this case is aimed at mimicking the geometry of an isolated bay of a circular shape. An introduction of such a boundary to the model results in the appearance of retention zones, where the vortex can be permanently trapped being either stationary or periodically oscillating. When stationary, it induces a steady velocity field that in turn ensures regular advection of nearby fluid particles. When the vortex oscillates periodically, the induced velocity field turns unsteady leading to the manifestation of chaotic advection of fluid particles. We show that the size of the fluid region engaged into chaotic advection increases almost monotonically with the increased magnitude of the vortex oscillations provided the magnitude remains relatively small. The monotonicity is accounted for the fact that the frequency of the vortex oscillations incommensurable with the proper frequency of fluid particle rotations in the steady state. Another point of interest is that it is demonstrated that bounded regions, in which the vortex may be trapped, can appear even at a significant distance from the bay. Making use of a Lagrangian indicator, examples of fluid particle advection induced by the periodic motion of the vortex inside the bay are adduced. 相似文献