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1.
通过对一个明显后向传播雷暴和一个无明显传播特征雷暴的环境场进行对比,分析环境场条件对雷暴传播运动的影响。结果表明:二者高空均受冷涡后部西北气流控制,有中空急流,低层受暖温度脊影响,气温较高,傍晚前后受短波槽影响,在鲁西北地区产生对流天气;后向传播雷暴的环境场水汽条件较好,大气斜压特征明显,近地面层高温高湿,θse锋区位于对流层中层,中层干空气与低层冷空气入侵,二者共同作用是雷暴的产生机制;无明显传播特征雷暴的环境场水汽条件较差,θse锋区位于850 hPa以下,对流层低层干冷空气与暖湿空气交绥是雷暴的产生机制;雷暴易发生在水汽通量散度中心北侧梯度较大的区域,主回波后部大气为不稳定层结且具有辐合中心、相对湿度较大的特征,这是产生新对流单体的关键;若雷暴区有湿平流,雷暴的下游方向有水汽辐合中心,且辐合中心具有斜压特征,有利于雷暴新生,反之,则不利于雷暴新生。  相似文献   

2.
利用常规资料、NCEP 1°×1°再分析资料、高分辨率可见光卫星云图资料,描述了2011年2月22-24日持续性海雾的发生范围、演变过程,分析了海雾发生前、发生时大气背景和物理量场;并利用环黄海北部的探空站、气象自动站资料对海雾发生时低层大气的温度、风、逆温特征进行了分析.结果表明:环黄海北部4个气象站中,各站出现海雾的特征不尽相同,既有以平流雾为主的、也有辐射雾为主的、还有平流雾和辐射雾共存的.对流层低层暖平流有助于保持逆温层、维持大气层结稳定;对流层低层偏南气流形成的水汽输送带和中层偏西气流水汽输送带的共同作用为大雾的形成和维持提供了水汽条件;夜晚低层辐合、高层辐散的动力分布有助于逆温层内弱的上升气流维持,对水汽凝结有利;白天低层辐散、高层辐合的动力分布有助于气流下沉,对稳定度和逆温的维持有利;负(冷)温度平流南下是大雾消散的动力热力因子.  相似文献   

3.
利用常规观测资料、自动站加密观测资料、NCEP1°×1°再分析资料、卫星FY-2E的TBB资料、多普勒天气雷达观测资料等,对2011年7月25日山东乳山强降水进行分析研究,结果表明:(1)这次强降水主要影响系统是高空槽、低层暖式切变线和副高边缘的低空急流。强降水产生在850h Pa和925h Pa切变线附近,低层850h Pa以下有较强的西南气流向北输送大量的水汽,强降水的水汽来源于低层近海面的水汽输送和辐合。(2)强降水产生在高温高湿区,强降水期间,低层有明显的暖平流,高层有明显的冷平流,低层暖平流增强或高层冷平流增强时,降水强度也明显增强。(3)强降水期间,乳山的特殊海岸线地形抬升作用产生的上升运动与中高层入侵的干冷空气(伴有下沉运动)相遇,从而触发对流不稳定能量释放,降水强度增大,产生强降水。(4)乳山出现短时强降水主要是由中-β尺度对流云团造成的,此次强降水的TBB在-63~-52℃,云团发展迅速,高度较高,在云团发展阶段,其反应的云顶温度比实际的云顶温度偏高。(5)风暴低层逆风区和中-γ尺度气旋性涡旋,及风暴顶的强烈辐散,利于回波发展与维持,同时使高值区维持在风暴中层及以下高度,在环境因子有利的情况下产生降水效率较高的强降水风暴。  相似文献   

4.
本文主要利用1973~1989年逐月全球热带200hPa及850hPa层经、纬向格点风及1980年以来1000,850,700,500,200,100,50hPa各层经纬向格点风,确定了热带对流层高、低(200,850hPa)层具有气候意义的越赤道气流通道,并分析了各越赤道气流通道强度的时、空变化特征。指出东半球比西半球越赤道气流强且稳定,季节变化也较明显。文章还指出,低层东半球向夏半球输送,高层夏半球向冬半球输送,且高、低层各相应通道强度变化趋势基本一致。高层与低层相比较,低层通道强且稳定,季节变化规律也较明显。文章还讨论了越赤道气流与大气环流系统的密切关系,指出各通道强度的年际变化是南、北两半球大尺度海-气相互作用的重要组成部分,是全球大气环流异常变化的重要信息。  相似文献   

5.
齐庆华 《海洋科学》2009,33(9):35-41
基于长时间序列的大气资料,计算了西北太平洋地区的水汽输送通量,分析了水汽输送通量场的时空变化特征,并给出了西北太平洋水汽输送通量与中国夏季降水异常的耦合模态.结果显示:西北太平洋水汽输送通量场具有显著的经向型、辐散型和纬向型3个主要的空间型,这三种模态的年循环特征都很显著.夏季,西北太平洋水汽输送通量异常以辐散型为主,且具有显著的准两年周期振荡特征和明显的年代际变率;在西北太平洋水汽输送通量与中国夏季降水异常前三类主要的耦合模态中,水汽输送通量异常以纬向型和辐散型为主.分析表明,西北太平洋水汽输送通量变化是影响中国东部降水异常的重要因素之一,而西太平洋暖池区、黑潮流域和中国近海尤其是南海海域则是向中国输送水汽的关键区域.这可为西北太平洋海气相互作用过程及其对中国气候的影响研究提供了必要的科学依据.  相似文献   

6.
殷嘉晗  张林 《海洋预报》2020,37(3):72-81
利用我国第六次—第九次北极科学考察雪龙船走航探空数据,计算北极太平洋扇区和白令海的夏季对流层高度,分析对流层内的风速、温度、水汽廓线,从而确定对流层结构,并分析各要素的垂直分布和经向分布特征。结果表明:夏季北极太平洋扇区和白令海的递减率对流层顶、冷点对流层顶平均值分别为10 003 m、10 116 m,对流层高度随纬度增加而降低。夏季北极大气对流层低层和对流层顶存在逆温,对流层顶的逆温高度和厚度随纬度增加而降低。大气可降水量与纬度呈负相关,且集中于对流层中低层。近地面的风速受地表摩擦力的影响较明显,对流层内的风速随高度增加而增大,高空急流的强度和高度随纬度增加而减小,风廓线和急流易受天气尺度过程的影响。研究结果揭示了夏季北极太平洋扇区和白令海的对流层结构,并可用于检验数值预报模式对北极大气垂直结构的预报效果、评估再分析资料描述北极大气垂直结构的能力。  相似文献   

7.
2017年1月1—5日,山东出现了一次大范围的平流辐射雾过程。利用山东地区自动气象站观测资料、青岛探空站资料、风廓线雷达资料和NCEP/NCAR再分析资料,通过分析此次连续大雾过程的大尺度环流背景场、温湿场特征,地面、高空气象要素条件,揭示了其形成原因、维持机制和消散机理。结果表明:中高纬度平直的大气环流、静稳的垂直结构是此次大雾形成的背景条件;水汽输送阶段变化造成的低层水汽浓度变化是大雾阶段变化的原因;两次弱低槽冷锋过程显著增加了雾的强度和范围,也使雾的性质由平流雾变为辐射雾。当低层水汽持续减少,中低层东风气流增强并破坏了大气的稳定层结时,大雾逐渐消散。  相似文献   

8.
基于近40 a NCEP/NCAR再分析月平均高度场、风场、涡度场、垂直速度场以及NOAA重构的海面温度(sea surface temperature,SST)资料和美国联合台风预警中心(Joint Typhoon Warning Center,JTWC)热带气旋最佳路径资料,利用合成分析方法,研究了前期春季及同期夏季印度洋海面温度同夏季西北太平洋台风活动的关系。结果表明:1)前期春季印度洋海温异常(sea surface temperature anomaly,SSTA)尤其是关键区位于赤道偏北印度洋和西南印度洋地区对西北太平洋台风活动具有显著的影响,春季印度洋海温异常偏暖年,后期夏季,110°~180°E的经向垂直环流表现为异常下沉气流,对应风场的低层低频风辐散、高层辐合的形势,这种环流形势使得低层水汽无法向上输送,对流层中层水汽异常偏少,纬向风垂直切变偏大,从而夏季西北太平洋台风频数偏少、强度偏弱,而异常偏冷年份则正好相反。2)春季印度洋异常暖年,西北太平洋副热带高压加强、西伸;而春季印度洋异常冷年,后期夏季西北太平洋副热带高压减弱、东退,这可能是引起夏季西北太平洋台风变化的另一原因。  相似文献   

9.
利用热带海洋和全球大气试验(TOGA)期间(1980~1996年)热带大气海洋观测阵(TAO)的长期浮标资料,分析了赤道行星波对西赤道太平洋暖池热传播的作用。结果表明,西赤道太平洋暖池纬向热传播主要出现在次表层水体中,并沿温跃层向东传播;而向西传播的季节热结构变化主要出现在中、西赤道太平洋的混合层中;驻波型传播在西赤道太平洋主要出现于温跃层,在中赤道太平洋主要出现于混合层和温跃层,在东赤道太平洋主要出现于混合层。在平均条件下,赤道太平洋上层水温纬向热传播信号以驻波型和东传型较强,西传型较弱。赤道Kelvin波压力分量贯穿西、东赤道太平洋并向东输送暖池热能,纬向流分量的热输送主要出现在西赤道太平洋;Rossby波压力分量的热输送主要出现在东、中赤道太平洋;混合Rossby重力波激发纬向流的热输送作用比相应温跃层扰动强。在平均条件下,赤道太平洋上层水温的驻波型变化制约了西赤道太平洋暖池热量的持续向东输送,因此形成了赤道太平洋水温的正常季节变化形态。当水温的驻波型变化减弱而东传型变化加强时,随后将形成厄尔尼诺现象。  相似文献   

10.
利用1974~1982年黄、东海海洋水文气象标准断面实测资料对近海面空气湿度的分布、变化进行了分析。讨论了冬、夏季海、气温与湿度的关系,并对冬、夏季近海面空气湿度进行了估算。结果表明,夏季,空气湿度为气温的函数;冬季,除了考虑空气本身平流的水汽外,还必须考虑海洋向大气的水汽输送。  相似文献   

11.
In this paper, effort is made to demonstrate the quality of high-resolution regional ocean circulation model in realistically simulating the circulation and variability properties of the northern Indian Ocean(10°S–25°N,45°–100°E) covering the Arabian Sea(AS) and Bay of Bengal(BoB). The model run using the open boundary conditions is carried out at 10 km horizontal resolution and highest vertical resolution of 2 m in the upper ocean.The surface and sub-surface structure of hydrographic variables(temperature and salinity) and currents is compared against the observations during 1998–2014(17 years). In particular, the seasonal variability of the sea surface temperature, sea surface salinity, and surface currents over the model domain is studied. The highresolution model's ability in correct estimation of the spatio-temporal mixed layer depth(MLD) variability of the AS and BoB is also shown. The lowest MLD values are observed during spring(March-April-May) and highest during winter(December-January-February) seasons. The maximum MLD in the AS(BoB) during December to February reaches 150 m (67 m). On the other hand, the minimum MLD in these regions during March-April-May becomes as low as 11–12 m. The influence of wind stress, net heat flux and freshwater flux on the seasonal variability of the MLD is discussed. The physical processes controlling the seasonal cycle of sea surface temperature are investigated by carrying out mixed layer heat budget analysis. It is found that air-sea fluxes play a dominant role in the seasonal evolution of sea surface temperature of the northern Indian Ocean and the contribution of horizontal advection, vertical entrainment and diffusion processes is small. The upper ocean zonal and meridional volume transport across different sections in the AS and BoB is also computed. The seasonal variability of the transports is studied in the context of monsoonal currents.  相似文献   

12.
This paper deals with the study of moisture budget of the typhoon No. 7507. The results show that the mass convergence produced by divergent wind has made the maximum contribution to precipitation, especially at the lower level, accounting for about 70% of the total precipitation, and that the advection term of water vapor is very small. The vertical flux term is to transport water vapor from the lower level to the middle and upper levels, resulting in the increase of water vapor accumulation at these levels. Evaporation term also plays an important role in precipitation, accounting for about 13% of the total precipitation and 23% of the horizontal moisture convergence. The moisture of the typhoon comes mainly from its southern boundary and the secondary inflow of moisture is from its western or eastern boundary. All the inflow layers of these three boundaries are very deep, reaching up to 300 hPa, while the strongest inflow occurs below 700 hPa. In the northern boundary of the typhoon, we obtained that  相似文献   

13.
Recent investigation suggests that volume transport through the Tsushima/Korea Strait often has double peaks during the summer to autumn period with decreasing transport in September. The satellite-observed wind changes from weak northwestward (across-strait) in summer to strong southwestward (along-strait) in early autumn (September) in the strait. Such a strong along-strait wind is related to tropical cyclones, which frequently pass through the East China Sea in September. The effect of the along-strait wind component on the transport variation is examined using a three-dimensional numerical model. The simulated volume transport through the Tsushima/Korea Strait shows realistic seasonal and intra-seasonal variations. According to sensitivity experiments on local winds, the transport variations in September are mainly generated by strong along-strait (southwestward) wind rather than weak across-strait wind. The strait transport responds to the along-strait wind (southeastward), which produces a sea level increase along the Korean coast, resulting in the geostrophic balance across the strait. The transport minimum through the Tsushima/Korea Strait in September can be determined by the combination of the across-strait geostrophic and along-strait ageostrophic balances. The Editor-in-Chief does not recommend the usage of the term “Japan/East Sea” in place of “Sea of Japan”.  相似文献   

14.
为了进一步揭示大气边界层低层动量通量逆梯度输运的观测事实,本文利用福建南部赤湖镇海边100m铁塔上观测得到的超声风温仪资料,采用诊断方法分析了2010年13号"鲇鱼"台风影响过程中近海面边界层大气中动量垂直通量逆梯度输送特征。结果表明:在逐小时时间尺度上台风近海面边界层大气中湍流动量垂直通量输送以沿梯度方向为主,但也存在一定比例的逆梯度方向输送现象,且越往高层该现象越明显,本文中其百分比最高不超过16%。并且这一现象出现的频率在台风环流的不同区域存在差别:在台风环流的内核区域最多,其次是登陆以后残余环流区,而在早期的台风外围环流中较少。湍流低频扰动的相干结构也是影响因素,当水平扰动与垂直扰动出现同位相变化时容易出现动量垂直通量逆梯度输送。大气动量通量逆梯度的水平和垂直平均空间尺度分别为258m和35m,平均时间尺度分别为123s和13s,均小于通常的顺梯度湍流低频扰动的时空尺度的1—3倍。  相似文献   

15.
Results of measurements of the atmospheric turbulence in the layer between 1.5 and 21 m above sea level and the drag coefficient of the sea surface as the wind blows from a 4-km-long mountainous slope with a mean inclination of 11° are presented. The measurements of wind-speed profiles and its fluctuations at several levels, waves, and the main meteorological parameters were carried out in autumn 2005 and 2008 from a stationary platform located in the Black Sea at a distance of approximately 1 km from the southern coast of Crimea. It is shown that during weak synoptic wind a low-level wind jet develops at night over the sea with a maximum velocity up to 5–6 m/s at a level of approximately 6 m over the sea induced by the katabatic wind over the coastal slope. According to the approximate estimates, the horizontal scale of the low-level jet can reach a few tens of kilometers. This flow is characterized by the dissipation rate of the turbulence energy independent of height and low-frequency velocity fluctuations related to the gravity waves and advection of turbulence from the coast. It is shown that the lower part of the boundary layer (up to a height of 3 m) is adjusted to the sea-surface roughness. The dependencies of the drag coefficient on the wind speed or wave age are steadier than in the data for the open sea. However, the age of the waves is not a universal parameter at long and short fetches.  相似文献   

16.
王寿景  李立 《台湾海峡》1993,12(4):303-311
本文根据历史水文气象资料,用条件谱分析方法,分析了厦门港水动力因素低频波动特征并探讨其发生机制。结果表明,低频波动清楚地表现为水位和表层盐度的波动。厦门港水位的低频波动主要源自平潭站的水位波动,风的贡献是次要的;条件谱分析了难以描述表层盐度低频波动和九江径流波动的复杂关系。  相似文献   

17.
The carbon cycle of lower trophic level in the Bohai Sea is studied with a three-dimensional biological and physical coupled model. The influences of the processes (including horizontal advection, river nutrient load, active transport etc. ) on the phytoplankton biomass and its evolution are estimated. The Bohai Sea is a weak sink of the CO2 in the atmosphere. During the cycle, 13.7% of the gross production of the phytoplankton enter the higher trophic level and 76.8 % of it are consumed by the respiration itself. The nutrient reproduction comes mainly from the internal biogeochemical loop and the rem-ineralization is an important mechanism of the nutrient transfer from organic form to inorganic. Horizontal advection decreases the total biomass and the eutrophication in some sea areas. Change in the nutrient load of a river can only adjust the local system near its estuary. Controlling the input of the nutrient, which limits the alga growth, can be very useful in lessening the phytoplankton biomass.  相似文献   

18.
本文基于2016年11月8日—2019年6月29日大沽河入海口水深观测数据分析了大沽河河口水位变化特征,并结合风场、降水量、卫星高度计融合产品资料对其影响因素展开了讨论。结果表明:1)大沽河口水位变化由潮汐过程主导,潮汐类型为正规半日潮,M2分潮占主导;2)余水位在2017年7月—2019年1月存在周期约为110—150天的显著季节内变化,主要受到纬向风的影响,监测系统处在大沽河入海口西岸,东向(西向)风将驱动水体向东(西)输运,导致西岸监测系统处水量减少(增加),从而观测到余水位下降(上升);3)观测期间,余水位存在显著下降趋势,约为–0.53×10–2 m/月,主要受到大沽河流域降水量减少的影响。  相似文献   

19.
Interannual variability(IAV) in the barrier layer thickness(BLT) and forcing mechanisms in the eastern equatorial Indian Ocean(EEIO) and Bay of Bengal(BoB) are examined using monthly Argo data sets during 2002–2017. The BLT during November–January(NDJ) in the EEIO shows strong IAV, which is associated with the Indian Ocean dipole mode(IOD), with the IOD leading the BLT by two months. During the negative IOD phase, the westerly wind anomalies driving the downwelling Kelvin waves increase the isothermal layer depth(ILD). Moreover, the variability in the mixed layer depth(MLD) is complex. Affected by the Wyrtki jet, the MLD presents negative anomalies west of 85°E and strong positive anomalies between 85°E and 93°E. Therefore, the BLT shows positive anomalies except between 86°E and 92°E in the EEIO. Additionally, the IAV in the BLT during December–February(DJF) in the BoB is also investigated. In the eastern and northeastern BoB, the IAV in the BLT is remotely forced by equatorial zonal wind stress anomalies associated with the El Ni?o-Southern Oscillation(ENSO). In the western BoB, the regional surface wind forcing-related ENSO modulates the BLT variations.  相似文献   

20.
Field measurements during the Bay of Bengal Monsoon Experiment (BOBMEX-99), data from a deep sea moored buoy, and satellite altimeter were used to describe variability in the hydrographic and meso-scale features in the Bay of Bengal (BoB) during the summer monsoon of 1999. The thermohaline fields showed two regions of upsloping of isopleths centered at 82°E and 84.75°E, ~110 km and 450 km away from the coast, respectively, followed by downsloping. The upsloping/downsloping of isopleths and the alternating currents was part of cyclonic and anti-cyclonic circulation patterns in the western BoB. In this region, both wind and current were important in the dynamics of coastal upwelling. The observations showed a relationship between the propagating waves and eddy on variability of thermohaline fields. On an annual cycle, four Kelvin waves were observed in the BoB, but only the downwelling Kelvin wave formed during October entered the Arabian Sea. During the monsoon season, four eddies were formed in the western BoB, of which the anticyclonic eddy centered at 15°N, 84°E and the cyclonic eddy centered at 17.5°N, 84.5°E were prominent. The baroclinic instability caused by the opposing currents along the east coast and the wind stress curl favored the formation of eddies. Okhubo-Weiss and Isern-Fontanet parameter confirmed the presence of eddies in the BoB.  相似文献   

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