基于目标时域散射特性的土地覆盖类型分类研究

目标散射特性随时间变化的规律称之为目标时域散射特性。目标时域散射特征是利用多时相雷达遥感图像进行目标识别的基础。本研究以广东肇庆为试验区,利用多时相单参数雷达图像进行土地覆盖类型分类研究,分析了试验区内典型植被的结构、形态及其散射机理等特征,总结了各类目标的时域散射特性,区分识别了多种目标,制作了土地覆盖类型分类图.     

地球自转率潮汐变化尺度因子的确定

地球自转速率的潮汐变化与尺度因子成正比 ,影响尺度因子各种地球物理机制是复杂的 ,主要有液核、海洋动力学 (平衡海潮和非平衡海潮 )、大气、地幔滞弹性等。文中讨论了大气、地幔滞弹性 ,并对影响地球自转尺度因子的同一机制不同理论模型进行了对比分析     

9806号台风非对称结构形成及其高纬西折路径分析

对9806号台风在弱环境场中的向北移动，至强环境场中折向西行的物理机制进行了分析，得出在弱环境场中台风可形成不对称结构，其物理量如高度的变化在台风进入强环境场后与环境场叠加，从而改变台风移向，强弱环境场的更替，可能是9806号台风移向突变的重要原因。     

NUMERICAL SIMULATION OF ATMOSPHERIC METHANE TRENDS OVER THE LAST 150 YEARS

A global two-dimensional chemistry model is developed to study long-term trends of CH_4 sinceindustrial revolution.The sources of CH_4,CO and NO_x are parameterized as functions of latitudeand time.With two long-term emission scenarios,long-term trends of CH_4 are simulated.The resultshave a good agreement with observation from ice cores.The modeled CH_4 increased from 760 ppbvin 1840 to 1611.9 ppbv in 1991, while the modeled number concentration of tropospheric OHdecreased from 7.17×10~5 cm~(-3)in 1840 to 5.79×10~5 cm~(-3) in 1991.The increase of atmosphericCH_4 can be explained by the increase of emission of CH_4 and build-up because of decrease of OHradicals that remove CH_4 from the atmosphere.The model is also used to simulate the distribution of CH_4.Comparisons between the modelresults and observations show that the model can simulate both latitudinal distribution and seasonalvariation of CH_4 well.     

THE RELATIONSHIP BETWEEN THE MOVEMENT OF THE MEIYU/BAIU RAIN BELT AND THE PERIODIC NORTHWESTWARD PROPAGATION OF THE CONVECTIVE ACTIVITY FROM TROPICAL WEST PACIFIC

In order to investigate the effect of the factors in tower latitudes on Meiyu/Baiu front,adiagnostic analysis for the two cases during June to July of 1985 and 1986 was examined.We foundthat (1)when the tropical convective activity moves westward to 10.5-15.5′N/140°E from eastside of 10.5-15.5°N/160°E,the northward shifts of the Meiyu/Baiu rain belt occurs;(2)themain factor which results in the northward and southward shifts of Meiyu/Baiu rain belt is thoughtas the 8,18 and 30 day oscillations of the tropical convective activity around West Pacific.Meanwhile,the wave train propagating from Lake Baikal via Okhotsk Sea to the tropics couldsometimes shift Baiu rain belt southward;(3)the onsets of Meiyu in China of both cases tend totake place just when the convective activity around lower latitudes moves westward through about140°E with the 8,18 and 30 day oscillation periods firstly coming to June.     

INVESTIGATION ON GEOSTROPHIC ADJUSTMENT,FRONTOGENESIS AND OSCILLATIONS

Geostrophic adjustment and frontogenesis are examined by means of the 2-D ARPS model.The simulation shows that.without the large-scale forcing,both the frontogenesis and frontolysisare observed during the geostrophic adjustment process and the intensity of the front oscillates inthe case of no discontinuity.The convergence (divergence) induced by the secondary circulation isthe most important factor for frontogenesis (frontolysis) at the top and bottom boundaries.Theamplitude and period of oscillation are dependent on the initial atmospheric stratification and theCoriolis frequency,and they are related to the inertio-gravity wave.     

亚洲季风环流在20世纪70年代末之后的减弱(英文)

全球大气环流自２０世纪７０年代末之后的转变可以很清楚地在大气温度、风场等的变化上得到发现。子波分析的结果证实这次转变的时间尺度在２０年以上。本文的研究着重揭示：在对流层中层，亚洲中纬度区域的转变趋势同全球平均的转变趋势相反；更重要的是，在这次转变之后亚洲和非洲的季风环流变弱了，同时热带东太平洋区的贸易风环流也变弱了。而在降水的变化中也可以发现这次转变。     

中层大气中重力波饱和机制的数值分析

通过对向上传播的重力波波包在中层大气中的非线性传播过程进行数值模拟,讨论中层大气中重力波的饱和机制.数值模拟结果表明,向上传播的重力波波包的扰动振幅在接近波包的本征水平相速度之前随高度单调增长,而当波振幅接近本征水平相速度时,在对流不稳定区域出现等位温面的翻转,同时波振幅的增长达到饱和（波振幅随高度不发生变化）.小尺度对流在等位温面的翻转和波饱和发生后产生,随后波包开始破碎,这些非线性过程的最终结果产生湍流.表明导致重力波饱和的关键因素是等位温面的翻转而不是诸如波破碎、湍流、波-流相互作用等其他的一些物理过程.     

大别-苏鲁超高压变质带P-T-t轨迹的动力学模拟

综合现有的地质、地球化学资料以及同位素年龄等研究成果，同时结合新西兰南岛北端陆壳俯冲的最新发现，提出了超高压变质岩的形成四阶段演化模式：板片俯冲形成增生楔、板片俯冲驱动角落流、板片拆离浮力抬升至Moho深度和后期上地壳伸展阶段.以此为定量模拟的出发点，利用二维有限元对大别-苏鲁超高压变质带的形成演化进行了动力学和热演化模拟，追踪超高压变质岩形成演化过程中的质点路径以及对应的P-T-t轨迹.计算的P-T-t轨迹及其空间分布特征均能与实测结果较好吻合.     

平极长期漂移与地球平均下地幔黏性估计

利用9个国际纬度观测站的平纬长期变化序列,重新讨论并估计了平极的长期漂移,得到漂移的平均速率为(3.356“±0.142”)×l0-3/a,方向为西经78.7°±2.5°.进一步基于最新的ICE-4G冰期后地壳反弹模型,采用地球上8个冰盖的冰融参数,估计了理论的平极长期漂移方向为西经74.8°.由观测的平极长期漂移速率为约束,基于1066B地球模型,估计得到地球平均下地幔的黏性为vLM=(0.5-1.7)×1022Pa^.s,表明vLM应具有近1022Pa^.s量级,并认为地球平极的长期漂移很可能是由最近的21000年以来冰期后的地壳反弹所致.