强暴雨中尺度系统发展结构和机理的非静力数值模式模拟研究
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摘要
本文利用观测分析、数值模拟以及动力学诊断相结合的方法,对我国两类中尺度强暴雨系统发展结构和机理进行了较深入研究,其中主要包括以下八个方面的研究成果。
     1.台风登陆变性低压暴雨和典型梅雨锋暴雨的对比研究
     台风登陆变性低压和典型梅雨锋是造成我国暴雨洪涝灾害的两类重要天气系统。为此,我们选取了“96.8”台风登陆变性低压暴雨过程和“98.7”梅雨锋低涡切变线暴雨过程。观测分析、数值模拟和热力、动力诊断结果指出,这两次暴雨过程都与α-中尺度对流系统(MαCS)和β-中尺度对流系统(MβCS)的生成和强烈发展直接相关。但其发生、发展及结构演变并不尽相同。
     2.“96.8”台风登陆变性低压暴雨的α中尺度系统结构及发展机理研究
     卫星云图分析可以看出,造成我国晋、冀、豫严重内陆灾害的“96.8”台风登陆变性低压暴雨的产生和台风低压中形成的强α-中尺度对流系统密切相关。
     天气观测事实分析可以得知,“96.8”特大暴雨是在大、中尺度天气系统和高、中、低纬环流系统相互作用而形成的有利环流形势下产生的。稳定的大型鞍形场和北移台风低压与其东侧副热带高压的相互作用是“96.8”特大暴雨发生的大、中尺度环流条件;而北移的α-中尺度台风低压及其特有的动力热力结构与该暴雨的发生和持续直接相关。
     成功的非静力中尺度数值模式模拟结果分析揭示:发展的台风低压具有气旋性涡柱的暖心高湿结构,在涡柱低空是湿对流不稳定和负湿位涡结构;强垂直上升运动与高空强辐散、低空强辐合及对流云团的发展互耦;与台风低压相伴的强南风急流不仅是台风低压和对流云团发展与维持的互伴互耦条件,而且也是暴雨产生与维持的必备条件。
     3.“98.7”梅雨锋低涡切变线暴雨的β-中尺度系统结构及发展机理研究
     大、中尺度天气系统和云图分析指出,“98.7”特大暴雨过程不仅与500hPa短波槽和700hPa低涡切变线以及地面梅雨锋系的生成和发展密切相关,而且与沿低涡切变线相继生成和强烈发展的MαCS与MβCS直接关联。
     双向相互作用的二重、三重和具有2km水平分辨率的四重嵌套细网格域D04的模拟结果揭示:(1)中-β尺度切变线在鄂东沿江低空强烈发展及辐合中心的出现与其中-β低涡的形成和发展直接关联。(2)中-β切变线强烈发展的垂直结构:强辐合层和强辐散层复式迭置并与强上升运动耦合发展;强涡度层和强位涡度层与强辐合层互伴发展;低空湿位温中心与中空饱和水汽带共存。(3)中-β低涡生成的垂直结构:散度和上升运动均呈双支柱状发展;涡度和位涡度均呈单支柱状发展;高湿能柱呈双支耦合发展,水汽通道呈阶梯斜升状。(4)中-β低涡发展的垂直结构:V字型散度柱和上升运动柱互耦发展;涡度和位涡度呈双支柱状;双支高湿能拄强烈发展,阶梯斜升水汽通道变宽增厚。至此低涡发展达最强,其结构具有典型性。模拟结果还指出,发展时空分辨率更高的多重嵌套网格模拟技术和应用四维资料同化方法,将有助于更细致的了解中-β强对流系统发生和发展的结构及其演变,并能进一步提高对暴雨落区及雨强的预报水平。(5)低涡云水和雨水的发生发展场结构是由带状向柱状发展,雪和云冰的发生发展场结构在高空呈带状发展。(6)强降水雨带和暴雨中心与700hPa高值θ。带和中心以及强风中心有相当好的对应关系,强暴雨中心位于强急流中心的北侧;低层位涡的分布与模拟的降水量分布几乎重合,这表明中尺度系统的发展与低层高PV带形成相联系。
The structure and mechanisms of two types of heavy rainfall mesoscale systems occurred in China have been studied in details by using observational analyses, numerical simulations and thermodynamic-dynamic diagnoses. The following eight issues have been mainly discussed and studied in this dissertation:1. The research on two types of heavy rainfall systems with a landing typhoon metamorphic low and typical Mei-Yu frontLanding typhoon metamorphic low and typical Mei-Yu front, two important types of the heavy rainfall synoptic systems, always result in severe floods in China. Therefore, we selected two related heavy-rainfall cases ( "96.8" landing typhoon metamorphic low and "98.7" Mei-Yu front with the low vortex-shear line) to investigate and study in this thesis. The results from observational analyses, numerical simulations and thermodynamic-dynamics diagnoses for the two heavy rainfall events indicated that the heavy rainfall were directly related to the genesis and intensive development of the MaCS and MpCS. However, there were still some large differences in the genesis, development and its structure evolution of the two types of heavy rainfall systems.2. The study on the structure and developing mechanisms of the meso-α scale heavy rainfall systems of the "96.8" landing typhoon metamorphic lowA heavy rainfall event occurred in Henan, Hebei and Shanxi Provinces during the period from 3 to 5 August 1996, resulted in severe flood catastrophe in China. Satellite cloud image analyses showed that the event was directly related to the genesis and intensive development of the MaCS formed in landing typhoon metamorphic low.Synoptic observational analyses showed that "96.8" rainstorm occurred under a favorable circulation pattern formed by the interactions between the large- and mesoscale synoptic systems as well as the high-, middle- and low latitude circulation systems. The stable gross col field and the interaction between a northward moving typhoon-low and its eastern lateral Pacific subtropical high were the large- and meso-scale circulation conditions. The unique dynamical and thermodynamical structures of the MaCS formed in landing typhoon metamorphic low were directly responsible for this rainstorm event.We have successful simulated this event using a nonhydrostatic numerical model MM5.V3 with a two-way interactive nesting mesh method. Results from the simulations revealed that: the developing typhoon-low had α structure of the cyclonic vorticity column with warm center and high humidity. At the lower levels, the vorticity column was the moist convective instability and the moist potential vorticity was negative;Strong vertical ascending motion, strong divergence at upper levels, strong convergence at the
    lower levels and the development of the convective cloud cluster were intercoupling;the intensive southern wind jet accompanied by the typhoon-low was not only the necessary interaccompanying and intercoupling conditions on the development and maintenance of the typhoon-low and convective cloud cluster, but it also transported the moisture source and heat energy essential prerequisite for the "96.8" extraordinary rainstorm.3. The study on the structure and developing mechanisms of the meso-p scale heavy rainfall system of the, 'j'98.7" Mei-Yu front with the low vortex-shear lineLarge-, meso- scale synoptic systems and cloud image analyses indicated that the "98.7" extraordinary heavy rainfall event was closely related to the genesis, development of a short wave trough on 500 hPa, a low vortex-shear line on 700 hPa and a Mei-Yu front system on surface, but it also directly related to the successive genesis and intensive development of MaCS and MpCS along the low vortex-shear line.Simulations using MM5.V3 with full moist physics schemes, four-dimensional data assimulation (FDDA) of analysis nudging and two way interactive nesting mesh method in two- or triple- or quartet- nest grid, especially in a very high horizontal resolution (nest subdomain D04 with 2km horizontal resolution) revealed that: (1) The intensive development of a meso-p shear line at low levels along the Changjiang River in the east Hubei and the occurrence of a convergence center were in directly relationship with the genesis and development of a meso-P low vortex;(2) The vertical structure of the intensive development on the meso-p shear line showed that the intensive convergence and divergence layers were reiteration and coupling with strong ascending motion. The strong vorticity, potential vorticity and convergence layers were inter-adjointing while the moist potential temperature center at low levels and the saturated vapor belt at middle levels were coexistence;(3) The vertical structural features of the genesis on the meso-p low vortex indicated that the divergence and ascending motion developed in double-branches column while the vorticity and potential vorticity developed in one branch column;the high moist energy column had a coupling double-branches development while the moisture channel had a step slantwise ascending development;(4) The vertical structures of the developing meso-p low vortex revealed the intercoupling development between the V-letter columns of the divergence and strong ascending motion;the vorticity and potential vorticity had double-branches columns;the band of the step slantwise ascending moisture channel became wider and deeper during the period of intensive double-branches column of high moisture energy. Meanwhile, the low vortex extremely developed and reached its strongest with its typical structure. (5) The genesis and developing field structure of the low vortex cloud water and rain water were developed from belt to column while the snow and cloud ice at upper levels exhibited a belt development. (6) There were considerable consistent corresponding relationship among the belt, centers of heavy rainfall and high value 6e on 700 hPa. The centers of heavy rainfall located the north side of the jet stream;the distribution of potential vorticity (PV) at lower levels was almost coincidence with the distribution of the simulated precipitation, suggesting the development of mesoscale system was related to the genesis of PV belt.
    4. Thermodynamic diagnoses of the heat and moisture budgets on the genesis and development of the "98.7" meso-fi scale heavy rainfall systemAnalyses of diagnostic apparent heat sources Qi and apparent moisture sink Q2 showed that the regions of high value of the total latent heat plus surface fluxes were consistent with the corresponding intensive regions of "98.7" heavy rainfall;The deep and thick heating layer in the mjdtlle troposphere was the mainly thermodynamic mechanism for the cumulus convective activation, the persistent genesis and development of severe rainstorm;The relative cool layer in the upper troposphere provided a favorable thermodynamic unstable condition for intensive cumulus convection over the heavy rain areas. The condensation latent heating of cumulus convective in the lower and middle troposphere was not only heating the middle troposphere atmosphere, but also heating the upper environment atmosphere through transporting heat to upper levels;the double-peak structure of Q2 at the early stage of heavy rainfall was relevant to drying associated with convective condensation of both stratocumulus in the lower levels and cumulus in the middle levels;the peak value of Q2 in the middle levels was basically corresponding with that of Qi;the deep and thick drying layer of Q2 was consistent with the deep and thick condensation heating layer of Qi.5. Dynamic diagnoses on change-rate of vorticity and divergence for the genesis and development of the "98.7" meso-fi scale heavy rainfall systemThe results from the diagnostic vorticity and vorticity change-rate (vorticity sources) indicated that one of the mainly physical mechanism of the persistent development of the low vortex-shear line was the superposition and coupling of positive vorticity centers over the upper and lower of the regions of Wuhan periphery;diagnoses of the total vorticity sources revealed that there was an almost vertical volume of high positive vorticity sources value generating and maintaining from low to upper levels over Wuhan periphery during the intensive genesis and development of the abrupt heavy rainfall. The vertical structure and evolution of the positive vorticity centers of the formation and development of the vorticitiy were consistent with that of the total vorticity sources, suggesting that the total vorticity sources played important roles in the genesis and development of the mesoscale low vortex, which was also a key dynamic mechanic of the persistent of the mesoscale system of the heavy rainfall. As for the contributions to the vortictiy change-rate, the divergence term was very important below 650hPa, but from 650hPa to 200hPa, vertical vorticity advection term was bigger than divergence term, the value of the horizontal advection was also positive. The divergence term was negative between 450hPa-250hPa, but the twisting term was negative through all the troposphere. Near the surface level, the factors of vertical vorticity and horizontal advection had almost no contribution to the vortictiy change-rate. The time-mean and perturbation of vorticity change-rate played important roles in the genesis of the low vortex at the beginning stage;The relative numeric of the nonlinear interactive vorticity change-rate was the most important component during the intensive development of the rainfall.The results from diagnostic divergence change-rate showed that the genesis and development of strong convergence centers and belt were related to the genesis and
    development of mesoscale vortex along shear line during the heavy rainfall. It indicated that the centers and their belt of the negative divergence change-rate in the lower level was in direct related to the genesis and development of mesoscale vortex along shear line by calculating the divergence equation. Moreover, the velocity advection divergence term was very important to the convergence for low level divergence, then the next large contribution was from ageostrophic vortictiy, and their negative belt was corresponding with the rainfall belt. At the same time, the p term in the divergence equation plays minor contribution to the divergence change-rate of the factors, which can be neglected.6. Dynamic diagnoses on frontogenesis and MPV for the genesis and development of the "98.7" Mei-Yu front with the low vortex-shear lineThe diagnoses from the frontogenetical function showed that the existence of frontogenesis nearby the north side of Wuhan-Huangshi played an important dynamic role in the maintenance and development of Meiyu front. Above the surface, the diabatic term was very crucial for the frontogenesis and the deformation and convergence of wind field was important too.The diagnoses of Moist Potential vorticity (MPV) showed that the low level negative MPV was correspondence with the rainfall belt, which indicated the moist symmetric instability was one of the possible mechanism of the convective along the Meiyu front precipitation belt. The heavy rain would be easily happened when the low level pressure was moist static instability and triggered vertical motion induced by moist symmetric instability.o7. A conceptual model of the meso-fi scale heavy rainfall system and study f Quantitative Precipitation Forecast (QPF)MM5.V3 with full moist physics scheme run in two-way interactive triple nest grid domains was used to simulate "98.7" heavy rainfall. Obviously, the simulations improved and the results was better than using two nest grid domains, especially the nest subdomain D03 with 6.6km horizontal resolution better revealed the four dimension thermodynamic and dynamic structure during the genesis and development of meso-p heavy rainfall system, and was able to successful reproduce maximum accumulated precipitation at 60hr and 72hr. We formed a conceptual picture based on to the simulations.The similar model run in two way with quartet nest grid as well as FDDA of analysis nudging was also used to simulate "98.7" heavy rainfall event. It showed that the simulation largely improved than previous simulations in two- and triple- nest grid, especially, the nest subdomain D04 with 2km horizontal resolution was able to simulate more correct heavy rainfall area and precipitation. It further revealed the structures and evolution of the genesis and development on meso-p systems producing intensive heavy rainfall. The simulative results also indicated that the development of a multiple nest technology with high temporal and spatial resolution and the application of FDDA method will be helpful to understand the structure and evolution of the genesis and development on the meso-P severe convective systems in more details, moreover, it will
    further enhance predictive capability for heavy rainfall area and precipitation as well as QPF.8. An investigation of probability on interlink mechanism between tropospheric precipitation and stratospheric ozoneA probability on interlink mechanism was investigated based on a correlation analysis of some observational fact between tropospheric precipitation and stratospheric ozone. Also we showed some relative modeled results using a 3D chemical transport model (CTM) SLIMCAT which is a power tool and world widely used to study ozone in the high- and middle- latitude regions. Furthermore, we made some possible explanations between the connection between tropospheric precipitation and stratospheric ozone. Further studies need to be done on this issue.
引文
[1] Godwin O. P. Obasi, WMO-服务的50年,2000,中国气象局图书馆文献资料通讯,2:1-5。
    [2] 陶诗言,倪允琪,赵思雄等,夏季中国暴雨的形成机理与预报研究,2001,北京,气象出版社.184pp.
    [3] 程麟生,中尺度大气数值模式和模拟,1994,气象出版社,358-359。
    [4] 张国华,“96. 8”河北大暴雨的时空分布特征,1997,河北气象,16(2);9-11。
    [5] 周月华、刘敏、陈淑明,湖北省1998年气候影响评价,1999,湖北气象,No.1,45-48。
    [6] 姚学祥,徐晶,2003年淮河流域大水期间体积降水量的研究,2004,气象学报,62(6):803-813。
    [7] 陶诗言,张小玲,张顺利,长江流域暴雨灾害研究。见:倪允琪,周秀骥主编 国家重点基础研究发展规划项目 (我国重大天气灾害形成机理与预测理论研究)研究专著系列丛书之二。北京,气象出版社,2004,192pp。
    [8] Convey, B. J. , 1987, FRONTIES: an operational system for nowcasting, NOWCASTING, 17-19 Aug. Vancouver.
    [9] 周秀骥,1989,京津冀灾害性天气监测与超短期预报实验基地建立的进展,京津冀中尺度气象试验基地文集。1989.3。
    [10] Ma Henian, Tang Xu, 1999, China's four major meteorological scientific experiments, ACTA METEOROLOGICA, 13(2): 129-140.
    [11] 薛纪善,海峡两岸及邻近地区暴雨试验研究进展,1999,海峡两岸灾害学术研讨会论文摘要总编,84-89。
    [12] Orlanski L. A rational subdivision of scales for atmospheric processes. Bull Amer Meteor Soc, 1975, 56: 527-530.
    [13] Maddox R A. Mesoscale convective complexes. Bull Amer Meteor Soc, 1980, 61: 1374-1387.
    [14] Shibagaki Y, Yabanaka M D, Shimizu S, et aL. Meso-β to meso-γ -scale wind circulations associated with precipitating clouds near Beiu front observed by the MU and meteorological radars. J Meteo Soc Japan, 2000, 78: 69-91.
    [15] 国家气象中心,国家卫星中心.'98中国大洪水与天气预报。北京:气象出版社,1999。
    [16] Changnon S A, Kunkel K E. Record flood-producing rainstorms of 17-18 July 1996 in the Chicago Metropolitan area. Part Ⅰ: Synoptic and mesoscale features. J Appl Meteor, 1999, 38: 257-265.
    [17] JST-CREST: Studies on structure and formation/development mechnisms of mesoscale convective systems. MRI-HP, 2000, No. 3: 1-8.
    [18] Gray M E B, The impact of mesoscale convective system potential vorticity anomalies on numerical weather prediction forecasts. Q. J. R. Meteo. Soc. , 2001, 127 (Part A): 73-88.
    [19] Ninomiya, K. , T. Akiyama and M. Ikawa, Evolution and fine structure of a long-lived Meso-α scale convective system in Baiu front zone. Part Ⅰ: Evolotion and Meso β scale characteristics, J. Meteo. Soc. . Japan, 1988, 66;331-350.
    [20] Ninomiya, K. , T. Akiyama and M. Ikawa, Evolution and fine structure of a long-lived Meso-α scale convective system in Baiu front zone. Part Ⅱ : Evolotion and Meso-γ-scale characteristics of precipitation, J. Meteo. Soc. . Japan, 1988, 66;351-371.
    [21] Laing A G, Fritsch J M. The large-scale environments of the global populations of mesoscale convective complexes. Mon Wea Rev, , 2000, 128: 2756-2776.
    [22] Parker M D, Johnson R H. Organizational modes of midlatitude mesoscale convective systems. Mon Wea Rev, 2000, 128: 3413-3436.
    [23] McAnelly R L, Nachamkin J E, Cotton W R, et al. . Upscale evolution of MCSs: Doppler radar analysis and analytical investigation. Mon Wea Rev, 1997, 125: 1083-1110.
    [24] McAnelly R L, and Cotton W R. Early growth of mesoscale convective complexes: A meso--β -scale cycle of convective precipitation? Mon Wea Rev, 1992, 120: 1851-1877.
    [25] Nachamkin J E, Cotton W R. Interactions between a developing mesoscale convective system and its environment. Part Ⅱ: Numerical Simulation. Mon Wea Rev, 2000, 128: 1225-1244.
    [26] Nachamkin J E, McAnelly R L, and Cotton W R. Interactions between a developing mesoscale convective system and its environment. Part Ⅰ: Observational analysis. Mon Wea Rev, 2000, 128: 1205-1224
    [27] Grasso L D. The dissipation of a left-moving cell in a severe storm environment. Mon Wea Rev, 2000, 128(8): 2797-2815.
    [28] 伍志方,张沛源,张春良,714CD多普勒天气雷达和714测雨雷达探测雹云的对比分析。高原气象,2000,19(1):1-8。
    [29] Houze R A, Rutledge S A, and Smull B F, Interpretation of Doppler weather radar displays of midlatitude mesoscale convective systems. Bull Amer Meteo Soc, 1989, 70: 608-619.
    [30] Smull B F, and Augustine J A, Multiscale analysis of a mature mesoscale complex. Mon Wea Rev, 1993, 121: 103-131.
    [31] 周海光,王玉彬,2003年6月30日梅雨锋大暴雨β和γ中尺度结构的双多普勒雷达反演,气象学报,2005,63 (3):301-311。
    [32] 倪允琪,周秀骥,中国长江流域中下游梅雨锋暴雨形成机理以及监测与预测理论和方法研究,气象学报,2005,63(3):647-661。
    [33] Zhang, D. L. and J. M. Fritsch, Numerical sensitivity experiments of varying model physics on the structure evolution and dynamics of two mesoscale convective systems, 1988, J. Atmos . Sci. , 45, 261-293.
    [34] Stensrud D J, Bao J-W, and Warner T T. Using initial condition and model physics perturbations in short-range ensemble simulations of mesoscale convective systems. Mon Wea Rev, 2000, 128(7): 2007-2107.
    [33] Warmer T T, and Hsu H-M, Nested-model simulationof moist convection: The impact of coarse-grid parameterized convection on fine-grid resolved convection. Mon Wea Rev, 2000, 128(7): 2211-2231.
    [36] Kusaka, H。, A. Crook, K. Wada and H. Hirakuchi, NUMERICAL SIMULATION OF HEAVY RAINFALLS IN THE BAIU FRONT BY THE WRF AND MM5. The 6th WRF/15th MM5 Users' Workshop. 3. 4, NCAR , June 27-30, 2005。
    [37] Chen, S. -J. , Kuo Y. -H. , Wang W. , et. al. , A modeling case study of heavy rainstorms along the MeiYu front. Mon. Wea. Rev. , 1998, 126, 2330-2351.
    [38] 张庆红,刘启汉,王洪庆等.华南梅雨锋上中尺度对流系统的数值模拟。科学通报,2000,45(18):1988-1992.
    [39] Feng,W(冯伍虎),Cheng L(程麟生),Cheng M(程明虎).Nonhydrostatic numerical simulation for the "98. 6" extraordinary rainstorm and the developing structure of mesoscale system, ACTA Meteor. SINCA, 2002, 16: 423-440。
    [40] 程麟生,冯伍虎.“98.7”突发大暴雨及中尺度低涡结构的分析和数值模拟。大气科学,2001,25(4),465-478。
    [41] 程麟生,Kuo Y H,冯伍虎等.双向三重嵌套网格和“98.7”特大暴雨模拟。高科技研究中的数值计算,2000,第六卷,346-351。
    [42] 程麟生,冯伍虎,“98.7”暴雨β中尺度低涡生成发展结构演变:双向四重嵌套网格模拟。气象学报,2003,61 (4):385-395。
    [43] 徐亚梅,高坤.1998年7月22日长江中游中-β尺度低涡的数值模拟及分析。气象学报,2002.60(1)1 85-95。
    [44] Bei, N. , S. Zhao, and S. Gao, Numerical simulation of a heavy rainfall event in China during July 1998. Meteo. Atmos. Phys. 2002, 80: 153-164.
    [45] 隆霄,程麟生,“99.6”梅雨锋暴雨低涡切变线的数值模拟和分析.大气科学,2004,28(3):342-356.
    [46] 江晓燕,倪允琪,一次梅雨锋暴雨过程的中尺度对流系统发展机理的数值研究.气象学报,2005,63 (1):77-91。
    [47] 陈敏,郑永光,王洪庆等,一次强降水过程的中尺度对流系统模拟研究.气象学报,2005,63 (3):313-324。
    [48] 李鲲,徐幼平,宇如聪,梅雨锋上三类暴雨特征的数值模拟比较研究.大气科学,2005,29 (2):236-248。
    [49] Kuo. Y-H. , L. Cheng(程麟生) and R. A. Anthes, Mesoscale analyses of the Sichan flood catastrophe 11-15. July 1981. 1986, Mon. Wea. Rev. 114. 1984-2003.
    [50] Li, Y-F, A. Huang and K. Gao. The role of convective heating in heavy rain system during Mei-Rains season. 1987, Scientia sinica (series B), 182-197
    [51] 丁一汇,高等天气学,1991,气象出版社。1-790。
    [52] 孙淑清,杜长萱,梅雨锋的维持与其上扰动的发展特征,1996,应用气象学报,7(2),153—159。
    [53] 冯伍虎,程麟生.“98.7”特大暴雨中尺度系统发展的热量和水汽收支诊断。应用气象学报,2001,12 (4),419-432.
    [54] 冯伍虎,程麟生,“98.7”突发性特大暴雨中尺度切变线低涡发展的涡源诊断。高原气象 2002,21 (5):447-456。
    [55] 冯伍虎,程麟生,“98.7”特大暴雨低涡切变线发展的散度变率诊断。暴雨·灾害,2001,5 (1):26-34
    [56] 冯伍虎,程麟生,“98.7”特大暴雨的动力学及能量诊断分析。兰州大学学报,2002,38 (4):131-137。
    [57] 隆霄,程麟生,“99.6”梅雨锋暴雨对流动量输送特征的诊断分析.气象学报,2004,62(4):439-448。
    [58] 柳艳菊,丁一汇,赵南,1998年南海季风爆发时期中尺度对流系统的研究:Ⅰ中尺度对流系统发生发展的大尺度条件.气象学报,2005,63(4):431-442。
    [59] 柳艳菊,丁一汇,1998年南海季风爆发时期中尺度对流系统的研究:Ⅱ 中尺度对流系统对大尺度场的作用.气象学报,2005,63 (4):443-454。
    [60] 黄永明,倪允琪,长江中下游一次非典型梅雨锋中尺度暴雨过程的分析研究.气象学报,2005.63 (1):100-113.
    [61] Hane C E, Jorgensen D P. Dynamic aspects of a distinctly three-dimensional mesoscale convective system. Mon Wea Rev, 1995, 123: 3194-3214.
    [62] Raymond D J, and Jiang H J. A theory for long-lived mesoscale convective systems. J Atmos Sci, 1990, 47: 3067-3077.
    [63] Kain J S, and Fritsch J M. Multiscale convective overturning in mesoscale convective systems: Reconciling observations, simulations and theory. Mon Wea Rev, 1998, 126: 2254-2273.
    [64] 程麟生,冯伍虎.,中纬度中尺度对流系统研究的若干进展。高原气象 2002,21(4):337-347。
    [65] Gao, S. , L. Ting, and Z. Yushu, Moisture potential vorticity anomaly with heat and mass forcing in torrential rain systems. Chin. Phys. Lett. , 2002, 19(6): 878-880.
    [66] Cui, X. , G Shoutting, and W. Guoxiong, Moisture potential vorticity and up-sliding slantwise vorticity development, Chin. Phys. Lett. , 2003, 20(1): 167-169.
    [67] 胡伯威,梅雨锋上MCS的发展、传播以及与低层“湿度锋”相关联的CISK惯性重力波,大气科学,2005,29(6).845-853。
    [68] 伍荣生,高守亭,谈哲敏等,锋面过程与中尺度扰动。见:倪允琪,周秀骥主编 国家重点基础研究发展规划项目 (我国重大天气灾害形成机理与预测理论研究)研究专著系列丛书之三。北京,气象出版社,2004,170pp。
    [69] 沈新勇,倪允琪,张明等,β中尺度暴雨系统发生发展的一种可能物理机制:Ⅰ.涡旋Rossby波的相速度,大气科学,2005,29 (5):727-733.
    [70] 沈新勇,倪允琪,沈桐立等,β中尺度暴雨系统发生发展的一种可能物理机制:Ⅱ.涡旋Rossby波的形成,大气科学,2005,29 (6):854-863。
    [71] Feng, W. (冯伍虎) , Fast Ozone Loss around the Polar Vortex during 2002/2003 Arctic Winter Deep Minihole Event, Water, Air & Soil pollution, in press.
    [72] Anthes, Global Weather Services in 2025, 1999, . http: //www. ucal: edu/ucargen/pres/2025/

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