低高度角地基GPS联合反演大气折射率廓线   总被引：1，自引：0，他引：1  

廖麒翔  石汉青  俞宏  汪彪 《气象科学》2016,36(1):128-133

为充分利用电磁波在大气中传播所携带的信息反演大气折射率廓线,提高低高度角地基GPS反演折射率廓线的精度,本文通过多目标优化反演算法NSGA-II,基本实现了GPS电磁波传播损耗和相位延迟观测量的最优联合反演。数值试验表明,联合反演效果明显优于传统的GA(Genetic Algorithm)单目标反演算法,加噪试验进一步证明了最优联合反演算法在反演折射率廓线方面的可行性及优越性。  相似文献   

APPLICATIONS OF THE CLOUDSAT TROPICAL CYCLONE PRODUCT IN ANALYZING THE VERTICAL STRUCTURE OF TROPICAL CYCLONES OVER THE WESTERN PACIFIC     

李冠林  严卫  韩丁  王蕊  叶晶 《热带气象学报(英文版)》2017,23(1):1-14

Cloud profiling radar (CPR) onboard CloudSat allows for deep penetration into dense clouds/precipitation. In this study, tropical cyclones (TCs) are classified into three stages as developing, mature, and decaying. The circular TC area with the radius of 500 km is divided into five regions. The vertical structure characteristics of 94 Western Pacific TCs at different stages in different regions from June 2006 to February 2014 are statistically quantified using the CloudSat tropical cyclone overpass product (the CSTC Product). Contoured frequency by altitude diagrams (CFADs) of radar reflectivity show an arc-like feature and exhibit opposite distributions with a boundary at 5 km. Bright bands are found at this altitude, indicating melting layers. Deep convective (DC) clouds have the largest occurrence probability in the inner region, while Ci clouds occur more frequently in the outer region at 10-15 km. As clouds have the second largest vertical scale after DC clouds. Distributions of Ac, Cu, and Ns clouds at different stages have few distinctions. As the altitude increases, the ice effective radius and the distribution width parameter decrease while the particle number concentration increases. Moist static energy (MSE), cloud thickness (CT), liquid water path (LWP), ice water path (IWP), water vapor (WV), and rain rate (RR) all diminish along the radial direction and are significantly larger at the mature stage. The average value of MSE at the developing stage is larger than that at the decaying stage.  相似文献   

一次伴有雷暴大风的飑线天气过程分析及数值模拟研究   总被引：1，自引：1，他引：0  

崔强  王春明  张云  黄泓  岳甫璐 《气象科学》2017,37(5):673-682

利用NCEP/NCAR(1°×1°)的逐6 h再分析资料、WRF中尺度预报模式,对2014年7月30—31日发生在江淮地区的一次强飑线天气过程进天气学分析和数值模拟研究。研究结果表明,此次飑线过程是在高空槽后有强冷空气输送、中层阶梯槽引导干冷空气南下并叠加在低层暖湿气流之上的有利背景条件下产生的,低空切变线是此次飑线过程的重要触发机制。在飑线成熟阶段,气流下沉速度极大值区在高(低)层与霰(雨水)混合比极大值区有很好的对应关系,水凝物粒子下落时对周围空气的拖曳作用是下沉气流形成的关键。雨水蒸发率影响飑线维持期间地面冷池的强度和分布,雨水蒸发率越大,地面冷池强度越强、范围越广;雨水蒸发率越小,地面冷池越弱,甚至消失。雨水蒸发率与地面风速也有很好的正相关性,增大雨水蒸发率可使地面风速增大,使模拟的地面最大风速更接近实况。  相似文献   

一次飑线过程的云微物理参数化方案数值试验及其成因分析   总被引：2，自引：1，他引：1  

许广  费建芳  黄小刚  姜勇强  程小平 《气象科学》2017,37(3):283-292

利用WRF模式6种适合高分辨率且包含多种固态水成物粒子的云微物理参数化方案,分别对2012年5月16日江苏北部一次飑线过程进行数值试验,结果表明:LIN方案模拟的飑线回波反射率、强降水TS评分、结构和强度等均要优于其余5种微物理参数化方案。分析不同参数化试验结果中不同水成物粒子占比随时间的变化特征,并针对LIN方案采取敏感性试验和水成物转化微物理过程分析指出,在此次飑线过程中的各水成物粒子中,霰/雹粒子占比最大,是降水过程中最重要的粒子;地面降水直接来源是雨水,雨水主要来源于中层霰/雹粒子的融化,小部分来源于云水的自动转化;中层霰/雹粒子最主要来源是通过雨霰转化过程中的雨水撞冻冰雹微物理过程,其次是霰撞冻云水的微物理过程,而冰相物质雪晶和云冰的碰并、撞冻和自动转化过程微乎其微。  相似文献   

雷达回波强度与雨滴谱参数的相关性研究   总被引：2，自引：2，他引：0  

张欢  濮江平  苑海燕  刘广超 《气象科学》2017,37(6):797-807

在雷达定量探测降水方面,目前大都采用雷达回波强度与降水强度的相关性来定量估算,但雷达回波强度与降水强度并非一一对应。本文利用从庐山和南京收集到的雷达观测资料和同步Parsivel观测到的雨滴谱数据,建立雷达回波强度与不同雨滴谱参数的函数关系,将由确定的函数关系式拟合后的雷达回波强度与雷达实测的回波强度作对比,以检验假定函数关系式的合理性,同时通过对比两地两类云降水拟合值的相对误差,给出了函数关系式中的最优y选项,为雷达定量估算降水量寻找新的途径。研究结果表明:庐山和南京两地两类云降水的雨滴谱参数对雷达回波强度的拟合普遍较好,其中对流云降水的拟合都明显好于层状云降水。两地层状云降水中各个雨滴谱参数对雷达回波强度的拟合曲线都大体相近,而对流云降水中,不同雨滴谱参数对雷达回波强度的拟合曲线差异较大。南京两类云降水拟合的相对误差要小于庐山两类云降水拟合的相对误差。除庐山对流云降水外,DV是两地两类云降水拟合公式中最优的y选项。而庐山对流云降水拟合式中,以N和DP的拟合最佳。  相似文献   

Contribution of tropical cyclones to abnormal sea surface temperature warming in the Yellow Sea in December 2004     

《Dynamics of Atmospheres and Oceans》2017

Unusual sea surface temperature (SST) warming occurred over the Yellow Sea (YS) in December 2004. To identify the causes of the abnormal SST warming, we conducted an analysis on atmospheric circulation anomalies induced by tropical cyclones (TCs) and their impacts on upper ocean characteristics using multiple datasets. With the analysis of various datasets, we explored a new aspect of the relationship between TC activity and SST. The results show that there is a significant link between TC activity over the Northwest Pacific (NWP) and SST in the YS. The integrated effect of consecutive TCs activity induces a large-scale atmospheric cyclonic circulation anomaly over the NWP and consequently anomalous easterly winds over the YS and East China Sea. The mechanism of the unusually warm SST in the YS can be explained by considering TCs acting as an important source of Ekman heat transport that results in substantial intrusion of relatively warm surface water into the YS interior. Furthermore, TC-related circulation anomalies contribute to the retention of the resulting warm SST anomalies in the entire YS.  相似文献   

风浪状态对海面拖曳系数的影响     

史剑  赵栋梁 《海洋湖沼通报》2007,(2):1-6

通过对四种参数化方法的比较,认为风海雷诺数RB较风速、波龄和波陡能更好地描述拖曳系数CDN。利用分组平均法对CDN与RB关系进行处理,得到最佳的CDN参数化方案。利用COARE3算法测试了四种依赖海况的粗糙长度,与实测结果进行了比较,结果表明CDN与RB的关系式更真实地反映了海-气界面动量交换过程。  相似文献   

江苏沿海近35年冷水块的特征分析     

朱首贤  何占元  张文静  谢石建  徐宇程 《海洋学报(英文版)》2018,37(11):19-25

The daily and monthly-mean characteristics of cold water patches(CWPs) off the Jiangsu coast in 35 a of1982–2016 are examined based on advanced very high resolution radiometer(AVHRR) data. Most of the CWPs are found to occur in the warm and hot months(May–September), with some CWPs in the cool and cold months(October–April). The average radius and intensity of the monthly-mean CWPs are about 81 km and 0.6°C,respectively. The average difference in the sea surface temperature(SST) between the centers of the CWPs and the nearshore is about 2.0°C. The correlation analysis between the CWPs, winds and tides indicates that most of the CWPs occurred during the southerly winds, with some CWPs occurring during the northerly winds. The average intensity of the CWPs during spring tides is slightly stronger than that during neap tides in the warm and hot months, and the difference is very small in the cool and cold months.  相似文献   

黑潮延伸体邻近区域中尺度涡特征统计分析   总被引：7，自引：3，他引：4  

胡冬  陈希  毛科峰  滕军  李妍  彭旭东 《海洋与湖沼》2018,49(3):497-511

本文利用20年的卫星高度计资料,对黑潮延伸体邻近海区(25°—45°N,135°E—175°W)中尺度涡的统计特征以及季节变化进行了统计研究。基于涡旋自动识别方法,共识别出本区域3006个气旋涡轨迹和2887个反气旋涡轨迹,其平均周期分别为9.99周和11.00周,平均半径分别为69.5km和71.8km。长生命周期涡旋的平均半径、涡度、涡动能(EKE)和涡旋能量密度(EI)在生命周期内大致都经历了增大-基本保持不变-减小这三个阶段。绝大多数涡旋沿纬线向西移动,经向移动距离较小,气旋涡和反气旋涡在西向传播过程中都具有明显的向南(赤道)偏离趋势。涡旋的生成数量与总数量均在春夏季达到最多,且这一时期涡旋的平均涡度、EKE、EI处于较高水平。  相似文献   

Evaluation of the Momentum Closure Schemes in MPAS-Ocean     

Shimei Zhao  Yudi Liu  Wei Liu 《中国海洋大学学报(英文版)》2018,17(2):227-243

In order to compare and evaluate the performances of the Laplacian viscosity closure, the biharmonic viscosity closure, and the Leith closure momentum schemes in the MPAS-Ocean model, a variety of physical quantities, such as the relative reference potential energy(RPE) change, the RPE time change rate(RPETCR), the grid Reynolds number, the root mean square(RMS) of kinetic energy, and the spectra of kinetic energy and enstrophy, are calculated on the basis of results of a 3D baroclinic periodic channel. Results indicate that: 1) The RPETCR demonstrates a saturation phenomenon in baroclinic eddy tests. The critical grid Reynolds number corresponding to RPETCR saturation differs between the three closures: the largest value is in the biharmonic viscosity closure, followed by that in the Laplacian viscosity closure, and that in the Leith closure is the smallest. 2) All three closures can effectively suppress spurious dianeutral mixing by reducing the grid Reynolds number under sub-saturation conditions of the RPETCR, but they can also damage certain physical processes. Generally, the damage to the rotation process is greater than that to the advection process. 3) The dissipation in the biharmonic viscosity closure is strongly dependent on scales. Most dissipation concentrates on small scales, and the energy of small-scale eddies is often transferred to large-scale kinetic energy. The viscous dissipation in the Laplacian viscosity closure is the strongest on various scales, followed by that in the Leith closure. Note that part of the small-scale kinetic energy is also transferred to large-scale kinetic energy in the Leith closure. 4) The characteristic length scale L and the dimensionless parameter Г in the Leith closure are inherently coupled. The RPETCR is inversely proportional to the product of Г and L. When the product of Г and L is constant, both the simulated RPETCR and the inhibition of spurious dianeutral mixing are the same in all tests using the Leith closure. The dissipative scale in the Leith closure depends on the parameter L, and the dissipative intensity depends on the parameter Г. 5) Although optimal results may not be achieved by using the optimal parameters obtained from the 2D barotropic model in the 3D baroclinic simulation, the total energies are dissipative in all three closures. Dissipation is the strongest in the biharmonic viscosity closure, followed by that in the Leith closure, and that in the Laplacian viscosity closure is the weakest. Mesoscale eddies develop the fastest in the biharmonic viscosity closure after the baroclinic adjustment process finishes, and the kinetic energy reaches its maximum, which is attributed to the smallest dissipation of enstrophy in the biharmonic viscosity closure. Mesoscale eddies develop the slowest, and the kinetic energy peak value is the smallest in the Laplacian viscosity closure. Results in the Leith closure are between that in the biharmonic viscosity closure and the Laplacian viscosity closure.  相似文献