1983 年梅雨期前后亚洲季风区水汽输送的分析          下载免费PDF全文

费建芳  乔全明  高太平 《应用气象学报》1993,4(1):65-72

分析了1983年江淮流域入梅前、梅雨期以及出梅后垂直积分的水汽输送和水汽通量散度分布,计算了南海和中国东部地区的水汽收支。结果指出:江淮流域入梅前,华南地区降水的水汽主要来自印度西南季风和东南季风气流;梅雨期降水的水汽主要来自印度西南季风气流;出梅后华北雨季则主要受中低纬水汽输送气流汇合的影响。分析表明,江淮流域梅雨期是印度西南季风气流加强并东进北上,西太平洋高压东撤所造成的;而梅雨结束则是由于西南季风气流减弱西退和西太平洋高压西进北上所造成的;此外,还讨论了水汽输送、水汽通量辐合与云量及我国东部降水的关系。  相似文献   

Research Status and Progress of Balloon-borne Cloud and Precipitation Particles Probe     

Peng Wang  Lei Liu  Xichuan Liu  Shuai Hu  Shijun Zhao  Wenming Ji  Taichang Gao 《地球科学进展》1986,35(7):704-714

The accurate observation of the microphysical structure of cloud and precipitation plays an important role in understanding the formation of clouds and precipitation. In-situ measurement using measuring instruments carried by meteorological balloons is an effective way to obtain the microphysical properties of cloud and precipitation particles, which is a supplementary means for aircraft to observe cloud and precipitation particles. This observation method plays a more and more important role in in-situ measurement. According to the difference of the working principle of the existing balloon-borne cloud and precipitation particles probes, the detectors can be divided into particle impact-sampling sensors, particle imaging sensors, light-scattering sensors, light intensity attenuation sensors and charge measurement sensors. The working principles, key technologies and main advantages and disadvantages of typical instruments were summarized, and their applications to detailed cloud structure acquisition, cloud remote sensing method establishment, cloud and precipitation physical process research and parameterization, and scientific observation of thunderstorm clouds were briefly introduced. Finally, the development trend of balloon-borne cloud precipitation particle detectors was prospected, which will provide reference for related technical research and equipment development.  相似文献   

热带海气耦合距平模式中的ENSO循环及其形成机制     

杨修群  谢倩 《气象科学》1995,15(4):134-157

本文研制设计了一包含海洋表面边界层和大气辐合反馈过程的热带太平洋海气耦合异常模式。进而利用该模式对ＥＮＳＯ循环进行了成功的模拟。通过对模式ＥＮＳＯ循环的演变特征及其形成机制的细致分析，揭示了ＥＮＳＯ暖位相的一种机制。  相似文献   

下击暴流的数值模拟研究   总被引：10，自引：3，他引：10  

许焕斌  魏绍远 《气象学报》1995,53(2):168-176

下击暴流是危害飞行安全的一种重要天气现象，特别是尺度为１—４ｋｍ的微下击暴流。为了了解下击暴流的发展过程，以及大气环境条件和云－降水微物理结构对下击暴流发生演变的影响，利用我们设计发展的非静力全弹性中尺度－γ模式，以一次发生了下击暴流的大气的温、湿、风实测资料为算例进行了数值模拟研究。计算结果给出了下击暴流发生发展的过程，以及在发展过程中各种物理量的变化，得出一些大气环境条件及水凝物粒子微结构对下击暴流发展的影响机理，有助于台站预报员掌握这种天气现象的出现和演变。  相似文献   

EFFECTS OF TOPOGRAPHY ON PROPAGATION AND DEVELOPMENT OF INERTIA GRAVITY WAVE          下载免费PDF全文

Wang Xingbao 《Acta Meteorologica Sinica》1995,9(4):488-500

Effects of topography on the propagation and development of inertia gravity waves areinvestigated by means of WKBJ method.The equation of wave action conservation is obtained.It isfound that the inertia gravity wave tends to propagate to the higher elevation area,meanwhile theamplitudes of the waves increase.While the inertia gravity waves propagate to a lower elevation area,their amplitudes decrease.  相似文献   

-种等压面上流场的可视化方法          下载免费PDF全文

李妍  黄峰  陈希  沙文钰 《大气科学学报》2001,24(2):286-290

结合等压面上高度场及其气象要素矢量场数据的空间分布特征,设计了-种能客观反映大气在等压面上的运动规律的可视化方法表面场线映射,它在气象上有较好的实用价值  相似文献   

斜压气流中波包的演变及其对外压不稳定波的激发     

王兴宝  吕克利 《气象学报》1996,54(1):2-17

把斜压气流中的短波槽看成波包，并把波包作为准地转模式的初值进行研究，发现波包的结构对其演变有重要影响，初始阶段急流轴下面向西倾斜的波包能够获得较快的发展，而向东倾斜的波包则是衰减的，这与ＷＫＢＪ方法得出的结论［１］是一致的，但是无论西倾还是东倾的波包，除了其自身随时间的演变外，还会激发出斜压不稳定波动，而且随着扰动的发展，不稳定斜压波会逐步在扰动中占主导地位。由此可以解释某些中纬度气旋的发生发展问题。  相似文献   

ENSO循环的数值模拟──Ⅰ:水平结构演变     

杨修群  谢倩 《气象学报》1996,54(1):42-52

利用发展的包含海洋表面边界展和大气辐合反馈过程的热带太平洋海气耦合距平模式，对ＥＮＳＯ循环进行了模拟。通过３０ａ积分，用合模式所展示的热带太平洋海气耦合系统的ＥＮＳＯ循环的水平结构演变特征和观测事实甚为一致，成功地模拟出了ＥＮＳＯ循环的冷暖态的发生发展、衰亡及相互转换等各个位相的动力和热力场的水平结构及其对季节循环的依赖性特征。本文数值模拟结果表明，ＥＮＳＯ循环的主要动力学过程可由热带海气相互作用系统自身所确定。ＥＮＳＯ循环的正确模拟是揭示其形成机制的前提。  相似文献   

ENSO循环的数值模拟(Ⅱ)──变化性及时间尺度选择机制     

杨修群  谢倩 《气象学报》1996,54(6):719-721

利用热带太平洋海气耦合异常模式的３０ａ模拟结果，对模式ＥＮＳＯ的变化性及多重时间尺度过程进行了细致分析，建立了一ＥＮＳＯ循环多重时间尺度过程相互作用的非线性相似（Ａｎａｌｏｇ）模型，并提出了ＥＮＳＯ循环主周期形成的一种可能机制。指出：和观测事实类似，模式ＥＮＳＯ过程确实涉及到三种时间尺度，即３—４ａ主周期振荡（ＬＦ）、准两年振荡（ＱＢ）和年循环（ＡＣ）；其中，ＱＢ过程是线性海气耦合系统的本征模态，年循环（ＡＣ）对其形成没有本质的影响；３—４ａ主周期振荡（ＬＦ）是一非线性系统的自激振荡现象，其形成是线性系统的本征模即ＱＢ过程通过非线性机制尤其是通过大气辐合反馈加热的“单向性”过程在ＱＢ的暖态产生的减频增幅所致；平均年循环（ＡＣ）虽然不能对ＥＮＳＯ循环形成有本质影响，但它可明显影响ＥＮＳＯ循环的具体振幅和位相，使得ＥＮＳＯ循环具有明显的不规则性并对季节循环具有明显的“锁相”特征；ＥＮＳＯ变化性确是ＬＦ、ＱＢ以及ＡＣ多重时间尺度相互作用形成的。本文提出的ＥＮＳＯ循环时间尺度选择机制不仅解释了主周期振荡的形成过程，而且也较好地解释了ＥＮＳＯ变化的谱，因此，这一机制更接近于观测事实。  相似文献   

ENSO cycle in a coupled ocean-atmosphere model and its negative feedback mechanism   总被引：1，自引：0，他引：1  

Assoc. Prof. Dr. X. -Q. Yang  Dr. Q. Xie  Prof. Y. -Q. Ni  Dr. S. -S. Huang 《Meteorology and Atmospheric Physics》1996,61(3-4):153-186

Summary A coupled ocean-atmosphere anomaly model has been developed for simulating ENSO cycle and its mechanism-study in this paper. After a long model run, the coupled model is successful in demonstrating ENSO-like irregular interannual variability and corresponding horizontal spatial structures. Based on the simulated results, the dynamics and the thermodynamics of the model ENSO cycle have been investigated, and in particular the negative feedback mechanisms that act to oppose instability of air-sea interaction, inducing termination of warm and cold events, have been examined. A detailed analysis of the oceanic wave dynamical properties and heat budget of the SST changes in a representative cycle suggest that the negative feedback mechanism to check the unstable growth of a warm event obviously differs from that of a cold event. The mechanism that induces decay and termination of a cold event is closely related to the negative, delayed feedback effect produced by the oceanic dynamical wave reflection at the western boundary. However, independent of the wave reflection effect, the negative feedback mechanism by which the coupled system returns from a warm event is associated with a slowly eastward-propagating coupling mode. Accompanied with the strong unstable development of the equatorial positive SST anomaly, the anomalous upwelling of cold water generated off the equator and the nonlinear anomalous meridional advection generated in the equator west of instability area jointly restrain the instability and finally plunge the system from a mature warm phase into a weak cold phase. A comparison between the results from the present model and the previous works is also discussed in this paper.With 16 Figures  相似文献