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1.
近海层大气湍流通量系数研究   总被引:1,自引:0,他引:1  
根据1994年9月18~30日南沙群岛海域渚碧礁的近海面大气湍流观测实验资料,分别计算了该海域光滑海面和粗糙海面上的空气动力粗糙度(z0 )、中性曳力系数( C D N)。利用 Butsaert 的假定,推导了求取标量粗糙度(z T、z Q)、整体输送系数(感热交换系数 C H N、水汽交换系数 C E N )的一组公式。在此基础上,分别计算和分析了该海域光滑海面和粗糙海面上空气动力粗糙度(z0 )、标量粗糙度(z T、z Q )、中性曳力系数( C D N)、整体输送系数(感热交换系数 C H N、水汽交换系数 C E N)及其关于水平风速分量的分布,并得到了一些有益的结论。  相似文献   

2.
厄尼诺与东亚暖冬的数值模拟   总被引:4,自引:1,他引:4  
陈受钧 《气象学报》1995,53(3):380-384
应用全球大气环流谱模式(ECHAM3),根据实际观测的海面温度资料,从1979年1月1日长期积分至1992年。模拟了厄尼诺年的东亚暧冬和弱冬季风现象。对于模拟的结果进行了初步讨论。  相似文献   

3.
TOGACD-ROM资料介绍(续)国家自然科学基金委员会地球科学部南京气象学院大气资料服务中心资料通讯第2卷第4期(总第7期)1995年10月4GEOSAr海面高度资料这些资料由NOAANationalService提供。原始资料是GEOSAT(Ge...  相似文献   

4.
本根据“实验3号”科学考察船在TOGA-COARE(1992年11月-1993年2月)定点(2°15'S,158°00'E)连续观测的大气,海洋资料,利用考虑风速和大气层结影响的整体输送动力学公式,计算给出了在西太平洋热带海域强对流天气过程中动量、感热和潜热等湍流通量垂直交换和水平输送的一些特性,并与该海域其它天气过程湍流通量交换和输送的特性作了比较,此外,中还讨论了更接近实际的曳力系数,感热  相似文献   

5.
资料通讯     
资料通讯国家自然科学基金委员会地球科学部南京气象学院大气资料服务中心第4卷第1期(总第10期)1997年12月ECMWF数值模拟资料CD┐ROM和CMAP降水资料介绍1ECMWFCD┐ROM这些CD-ROM上存放着选自ECMWF(欧洲中期预报中心)“...  相似文献   

6.
陆面上总体输送系数的特征   总被引:7,自引:4,他引:7  
苗曼倩  钱峻屏 《气象学报》1996,54(1):95-101
利用气象铁塔的风、温梯度资料,对陆面上近地层湍流拖曳系数CD和总体输送系数CH(或CE)的大小和日变化规律进行研究。发现陆面上较粗糙的地表,CD和CH可以比海面上大一个量级左右。而且存在着明显的日变化。它们对地表面动力粗糙度变化的反应较敏感。本工作为气候及大气环流模式研究中陆面参数化过程提供了重要依据。  相似文献   

7.
南沙海域大气湍流通量输送特征分析   总被引:23,自引:1,他引:23  
利用1994年9月在南沙群岛的渚碧礁(10°52′N,114°04′E)观测的湍流资料,采用涡旋相关法计算,给出了南沙海域的曳力系数,动量通量,感热通量和潜热通量,并与其它海气相互作用实验及HEIFE的结果作了比较,结果表明,该海域的曳力系数CD=(1.54±0.24)×10^-3。大气向海洋输送动量通量与水平风速挟方成正比,该海区无论白在还是晚上都是将其贮存的热量以潜热或感热的形式输送到大气中。  相似文献   

8.
西太平洋暖池区的海气通量及整体交换系数   总被引:3,自引:1,他引:2  
根据西太平洋海域弱风、高温、潮湿的大气状态特征,提出了在光滑面存在粘性副层气流中的廓线的层结订正方案。用此模式对西太平洋暖池区TOGACOAREIOP期间,在向阳红5号船(2°S,154°E)获取的海面风、温、湿梯度资料进行了处理。计算结果显示西太平洋暖池区贴水层气流中不稳定层结占50%-80%,其中很不稳定的占10.3%;该海区海气通量和整体交换系数受层结影响远大于受风速的影响;海气通量和整体交换系数随不稳定程度增加而增大,在相同风速下量值可相差4倍以上;其变化范围为0.3×10-3—3.2×10-3。由此可见,层结的影响使它们的变化大于其它海区的结果。在u10=0-10m/s范围内,中性化整体交换系数平均为CDN=1.2×10-3,CHN=1.14×10-3,CEN=1.19×10-3,与Large和Pond(1981,1982)不稳定条件的研究结果相差无几。  相似文献   

9.
1985年6月14日,在中部风暴试验俄克拉何马-堪萨斯初步区域试验(PRE-STORM)外场阶段生成了一个很强的夜间中尺度对流复合体(MCC)。它出现在美国气候上中部暖季降水夜间最大中心附近。本文应用专门的无线电深空测风资料和地面中尺度站网资料研究了支持MCC生成的环境条件在夜间如何演变的。这里所研究的MCC是一个MCC系列中的第4个,是在准静止地面锋以北100-300公里处向东方向传播的三个MC  相似文献   

10.
利用1993年ENSO事件(4月)爆发前酝酿阶段,TOGA/COARE关键区强化期(1992年11月-1993年2月)立体观测实验“向阳红五号”科学考察船定点(155°E,2°S)高空大气探测资料,分析了西太平洋暖海域上空对流上升区西侧风的垂直变化,指出:对流层上、下部各有一强风带,随着海-气ENSO异常的发展,高空强东风带和低空强西风带均呈增强趋势,最强时分别连续14天和18天达到急流标准,占相  相似文献   

11.
利用珠海凤凰山陆气相互作用观测塔站2014年11月至2016年5月的观测数据,对比分析了干湿季森林下垫面能量通量和气象要素的变化特征,分析了在不同稳定度下3个风向范围(315°~45°、45°~135°和135°~225°)的动量和感热交换系数随冠层表面风速的变化特征,并对动量和感热交换系数进行了参数化研究。结果表明:干季感热和潜热通量值相当,湿季潜热远大于感热。干季和湿季的夜晚都出现负感热现象,感热从大气向森林输送。相对湿度的变化幅度大,与该地气象状况密切相关,相对湿度的垂直梯度夜晚较大,白天较小。干季的气温垂直梯度比湿季的明显。风速在冬季变化平缓,夏季变化剧烈,低层风速随高度变化梯度明显,高层较紊乱。各高度风向差异不大。中性和近中性状态下,在风向为315°~45°、45°~135°和135°~225°时,动量交换系数Cdn分别为0.05、0.0055和0.022,感热交换系数Chn分别为0.0055、0.003和0.004。在稳定和不稳定状态下,动量交换系数Cd、感热交换系数Ch随冠层表面风速v明显发生变化,稳定条件下,Cd、Ch随v的增大而增大;不稳定条件下,Cd、Ch随v的增大而减小。分不同风向对森林冠层Cd、Ch在稳定和不稳定条件下与v的关系进行了拟合,得到了参数化公式。  相似文献   

12.
Both mean and wave-induced motions generate turbulence in the air flow above sea waves. Assuming a local balance between production of turbulent kinetic energy and its dissipation, an explicit relation for the heat exchange coefficient CH is obtained. It is shown that CH follows a square-root dependence on the drag coefficient CD. However, the proportionality coefficient appears to depend on the sea state, expressed in terms of the coupling parameter. Dependence on the sea state suppresses the CD1/2 wind-speed dependence, and results in a marginal increase of CH with increase in the wind speed.  相似文献   

13.
在计算海-气感热通量、潜热通量和动量通量时,因气象要素的测量高度不一致而带来的热交换系数cT、蒸发系数cE和摩擦系数 cυ的偏差,给计算结果带来一定的影响。文章介绍一种高度订正方法,对cT、cE、cυ的值加以订正,从而提高了计算准确性。计算结果表明,系数订正后的误差可减小9%—11%。  相似文献   

14.
Recent studies have shown that surface fluxes and exchange coefficients are particularly important to models attempting to simulate the evolution and maintenance of hurricanes or typhoons.By using an advanced research version of the Weather Research and Forecasting(ARW)modeling system,this work aims to study the impact of modified exchange coefficient on the intensity and structures of typhoon Saomai(2006)over the western North Pacific.Numerical experiments with the modified and unmodified exchange coefficients are used to investigate the intensity and structure of the storm,especially the structures of the boundary layer within the storm.Results show that,compared to the unmodified experiment,the simulated typhoon in the modified experiment has a bigger deepening rate after 30-h and is the same as the observation in the last 12-h.The roughness is leveled off when wind speed is greater than 30 m/s.The momentum exchange coefficient(CD)and enthalpy exchange coefficient(CK)are leveled off too,and CD is decreased more than CK when wind speed is greater than 30 m/s.More sensible heat flux and less latent heat flux are produced.In the lower level,the modified experiment has slightly stronger outflow,stronger vertical gradient of equivalent potential temperature and substantially higher maximum tangential winds than the unmodified experiment has.The modified experiment generates larger wind speed and water vapor tendencies and transports more air of high equivalent potential temperature to the eyewall in the boundary layer.It induces more and strong convection in the eyewall,thereby leading to a stronger storm.  相似文献   

15.
The surface flux exchange associated with the exchange coefficients and upper ocean conditions is essential to the development of tropical cyclones (TCs). Using the Weather Research and Forecasting (WRF) model, the present study has investigated the impact of exchange coefficients and ocean coupling during Super Typhoon Saomai (2006). Firstly, two experiments with different formula of roughness are conducted. The experiment with the Donelan formula for drag coefficient (Cd) and ramped formula for enthalpy coefficient (Ck) can simulate stronger intensity compared to other experiments due to the increased surface wind and enthalpy fluxes. That is because the new formulas allows for a smaller Cd and larger Ck in the high wind regime than the former formulas did. Moreover, two coupled simulations between WRF and a one-dimensional ocean model are conducted to examine the feedback of sea surface cooling to the TC. In the experiments with a horizontal uniform mixed layer depth of 70 m, the sea surface cooling is too weak to change the evolution of TC. While in the experiment with an input mixed layer calculated using the Hybrid Coordinate Ocean Model (HYCOM) data, the significant sea surface cooling induces obvious impact on TC intensity and structure. Under the negative feedback of sea surface cooling, the sensible and latent heat fluxes decreases, especially in the right part of Saomai (2006). The negative feedback with coupled ocean model plays a vital role in simulating the intensity and structure of TC.  相似文献   

16.
Using monthly mean of surface turbulent heat exchange coefficients calculated based on datafrom four automatic weather stations(AWS)for thermal equilibrium observation in July 1993—September 1996 and of surface conventional measurements,an empirical expression is establishedfor such coefficients.With the expression,the heat exchange coefficients and the components ofsurface thermal source are computed in terms of 1961—1990 monthly mean conventional data from148 stations over the Qinghai-Xizang(Tibetan)Plateau(QXP)and its adjoining areas,and the1961—1990 climatic means are examined.Evidence suggests that the empirical expression is capable of showing the variation of the heatexchange coefficient in a climatic context.The monthly variation of the coefficients averaged overthe QXP is in a range of 4×10~(-3)-5×10~(-3).The wintertime values are bigger in the mountainsthan in the valleys and reversal in summer.Surface effective radiation and sensible heat are thedominant factors of surface total heat.In spring surface sensible heat is enhanced quickly,resulting in two innegligible regions of sensible heat,one in the west QXP and the other innorthern Tibet.with their maximums emerging in different months.In spring and summersensible heat and surface effective radiation are higher in the west than in the east.The effectiveradiation peaks for the east in October—December and the whole QXP and in June and October forthe west.The surface total heat of the plateau maximizes in May.minimizes in December andJanuary,and shows seasonal variation more remarkable in the SW compared to the eastern part.Inthe SW plateau the total heat is much more intense than the eastern counterpart in all the seasonsexcept winter.Under the effect of the sensible heat,the total heat on the SW plateau starts toconsiderably intensify in February,which leads to a predominant heating region in the west,withits center experiencing a noticeable westward migration early in summer and twice pronouncedweakening in July and after October.However,the weakening courses are owing to differentcauses.The total heat over the north of QXP is greatly strengthened in March.thus generatinganother significant thermal region in the plateau.  相似文献   

17.
强风天气条件下海气动量交换参数的观测分析   总被引:4,自引:3,他引:4  
利用近岸海上气象平台对登陆台风“黑格比”近海层风廓线观测资料,计算分析了近海层大气的湍流动量通量交换参数,以期认识高风速情况下的海气动量交换特征.数据分析结果显示,当海面上方 10 m处风速U10≤24 m/s时,摩擦速度(U*)随风速的增大而增大,当U10>24 m/s时,U*呈饱和趋势.海面粗糙度长度(Z0)、拖曳系数(Cd)在低风速( U10≤6 m/s)随风速的增大而减小,在U10处于6~24 m/s之间时,Z0、Cd随风速的增大而增大,当U10>24 m/s时,Z0、Cd达到极值后开始减弱.Z0、Cd极值出现在U10为24~28 m/s之间.并对高风速时拖曳系数衰减现象的对应机制进行了讨论.另外,还探讨了台风期间的阵风因子(G(t,T))等参数的演变特征.  相似文献   

18.
1.Introducti0nThemesoscaleoperationalmodel-whichisoftenused,isMM4orMM5'butMM4isusedfrequentlyonlO3kmscale.Thephysicalprocessesinthismodeldevelopconstantly.FororiginalMM4,thecomputationofsurfacefluxesisnotaccurate,andKmodelfortheturbu-lencefluxesbetweenany2levelsneedstobeimprovedbynewtreatment.Inordertostudytheinfluencesofboundarylayerparameterizationschemesonmesoscaleheavyrainsystem,sur-facefluxesandKmodelinoriginalMM4areimprovedbytherecentresearchinthispaPer.Theflux-profilerelationsforv…  相似文献   

19.
利用1961-2010年河北省周边7个太阳辐射观测站的资料,拟合得出相对精确的河北省太阳直接辐射经验公式,分析了河北省太阳直接辐射时空变化特征。结果表明:河北省近50 a来太阳直接辐射年总量总体呈明显的下降趋势。其中,下降幅度相对较大的石家庄为25%,下降幅度相对较小的唐山为11%。河北省水平面太阳直接辐射年总量近50 a平均值空间差异较大,<2540MJ·m-2 主要分布在邢台南部,>3510MJ·m-2 主要分布在张家口西北部,大部分地区介于2540-3300MJ·m-2 。河北省太阳能资源开发利用潜力比较大的区域主要在张家口的坝上地区。  相似文献   

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