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1.
本文使用SODA(simple ocean data assimilation)海洋同化资料,系统分析了厄尔尼诺-南方涛动(El Ni?o-Southern Oscillation,ENSO)循环中冷暖位相期间热带太平洋上层海洋环流的演变规律,探讨了形成海洋环流异常的新机制。结果表明,在厄尔尼诺成熟期,热带中东太平洋赤道潜流最弱,赤道两侧出现反气旋性环流异常;西太平洋赤道外热带海域出现气旋性环流异常,该区南、北赤道流、棉兰老流、黑潮、新几内亚沿岸潜流及南赤道逆流增强;北赤道逆流区出现异常气旋性环流串,北赤道逆流接近正常。在厄尔尼诺衰退期和拉尼娜发展期,热带中西太平洋赤道潜流达到极强,赤道两侧出现气旋性环流异常;西太平洋赤道外热带海域异常环流减弱,该处主要流场的强度减弱或处于正常状态;北赤道逆流区反转为异常西向流。结果表明, ENSO循环期间的上层海洋环流异常受到热带太平洋温跃层深度异常产生的压强梯度力异常调控,在赤道外热带海洋温跃层深度异常和科里奥利力共同作用产生大尺度海洋环流异常,而在赤道海域,海洋温跃层深度异常和Gill效应造成赤道潜流异常以及关于赤道对称的气旋或反气旋性环流异常。  相似文献   

2.
Hydrographic data collected aboard R. V. Anton Bruun along 65°E between 18°N and 42°S from 17 May to 4 July 1964 are used to investigate water characteristics and current structure in the upper 500 m in the Indian Ocean. The water characteristics indicate the occurrence of three main water masses,viz., warm, saltier, low-oxyty and nutrient-rich Arabian Sea Surface Water, relatively fresh and high-oxyty Equatorial Indian Ocean Water, and more saline, high-oxyty and nutrient-poor Tropical Water of the South Indian Ocean. The recently discovered South Equatorial Countercurrent and Subtropical Countercurrent (renamed Tropical Countercurrent, at the suggestion of Dr. R. B.Montgomery) are observed in the current structure at 13°S and 22°–26°S respectively, and these could also be identified on the vertical sections of temperature, thermosteric anomaly and salinity. Contrary to the existing concept, the North Equatorial Current continues to be present even after the onset of the southwest monsoon. The Equatorial Undercurrent could not be traced in the Indian Ocean during this period.  相似文献   

3.
热带非稳定波(TIWs)关于赤道的径向不对称是其突出特征之一。本文利用二层半线性海洋模式研究各种不对称背景条件对非稳定波不对称性的影响。结果表明,在大西洋和太平洋上热带非稳定波(TIWs)的不对称性似是由于南赤道流的两个分支和海面温度锋面对于赤道的不对称性,而不是由于北赤道逆流的出现。  相似文献   

4.
Using the Comprehensive Ocean-Atmosphere Data Set (COADS), wind, surface pressure and SST fields in the Equatorial Eastern Pacific and the Equatorial South Indian Ocean were analysed comprehensively.lt is pointed out that the seesaw between surface pressure in the Equatorial South Indian Ocean and the Equatorial Southeast Pacific causes the seesaw between the wind fields in the two areas, and the seesaw of wind fields results in the seesaw of SST between Indonesia and the Equatorial Eastern Pacific. El Nino is the response of ocean to the forcing of monsoon system in the Indian Ocean and the trade system in the Pacific.  相似文献   

5.
用一个水平分辨率比较高的非线性正压模式,对热带西太平洋海域里的海流进行了数值模拟。计算海流与观测结果颇相一致。结果表明:赤道以北、棉兰老岛以东附近海域中,棉兰老冷涡在一年的大部分时间里都得到发展,但是其范围、强度和中心位置在各个月份并不相同,显示出很强的季节变化;在哈马黑拉岛东北海域,6月份突然出现了一个反气旋式的涡旋;这个涡旋8月份发展得最强,一直持续到10月份,在11月份就消亡了。  相似文献   

6.
The average vertical distribution of equivalent potential temperature, horizontal divergerce, relative vorticity and vertical velocity overthe observation area were computed using 6-days NAVAID wind data from the R/V Shijian and R/V Xiangyanghong 09 during FGGE (the First GARP Global Experiment) and upper air sounding data of two island stations within the same period. Yanai's method was used to compute the vertical distributions of the apparent heat source, apparent moisture sink and total eddy heat flux. Satellite cloud photographs and surface meteorological measurements were used to subdivide the six days of observation into three disturbed days and three undisturbed or trade days. This paper describes the large-scale structure and heat budgets in the disturbed and trade wind periods and compared them with those of the trade wind regions of the Atlantic. Some interesting results of the structure and heat budgets of large-scale disturbances over the equatorial trough region in the western Pacific are  相似文献   

7.
利用Topex/Poseidon卫星高度计1992年10月到1998年12月连续75个月,230个重复周期的有效波高资料对南北太平洋的波高成份进行了分析,结果显示所有的月份,频数密度峰值对应的波高成份因子为1.4,以赤道太平洋海域最高为1.6,南北太平洋海域为1.2左右。7、8、9、10月份太平洋涌浪成份占频数密度累积率的比例大于95%,其余各月占90%左右,表明太平洋海域波高成份以涌浪为主。  相似文献   

8.
通过对我国沿海多次野外实地考察以及文献报道,对铜藻进行了分类地位及生物地理分布特征介绍。结合分子数据,目前由过去单一的狭义铜藻Sargassum horneri和线形马尾藻Sargassum filicinum结合而成广义铜藻。其生物地理分布区系由西北太平洋扩大到东北太平洋的有限区域。根据我国沿海铜藻底栖和漂浮种群的发生季节变化,初步判断我国可能存在2个以上的底栖铜藻种群:春季成熟型、夏季成熟型和/或秋季成熟型。结合铜藻的自然生境、底栖分布区系以及海流等水文资料,本文对2016年底黄海漂浮铜藻种群的源头进行了初步分析,其最可能地域源头为渤海海峡区及其邻近水域,最可能的种群来源为夏季成熟型。  相似文献   

9.
On the basis of the salinity distribution of isopycnal(σ_0=27.2 kg/m~3) surface and in salinity minimum, the Antarctic Intermediate Water(AAIW) around South Australia can be classified into five types corresponding to five regions by using in situ CTD observations. Type 1 is the Tasman AAIW, which has consistent hydrographic properties in the South Coral Sea and the North Tasman Sea. Type 2 is the Southern Ocean(SO) AAIW, parallel to and extending from the Subantarctic Front with the freshest and coldest AAIW in the study area. Type 3 is a transition between Type 1 and Type 2. The AAIW transforms from fresh to saline with the latitude declining(equatorward). Type 4, the South Australia AAIW, has relatively uniform AAIW properties due to the semienclosed South Australia Basin. Type 5, the Southeast Indian AAIW, progressively becomes more saline through mixing with the subtropical Indian intermediate water from south to north. In addition to the above hydrographic analysis of AAIW, the newest trajectories of Argo(Array for real-time Geostrophic Oceanography) floats were used to constructed the intermediate(1 000 m water depth) current field, which show the major interocean circulation of AAIW in the study area. Finally, a refined schematic of intermediate circulation shows that several currents get together to complete the connection between the Pacific Ocean and the Indian Ocean. They include the South Equatorial Current and the East Australia Current in the Southwest Pacific Ocean, the Tasman Leakage and the Flinders Current in the South Australia Basin, and the extension of Flinders Current in the southeast Indian Ocean.  相似文献   

10.
Hydrographic measurements by CTD were made in the western-central Equatorial Pacific (160°W–147°E) during the Japanese Pacific Climate Study cruise in January–February 1991. InT-S diagram, three water masses are seen in the layer of kg/m3: salinity water corresponding to the Tropical Water of eastern South Pacific origin, less saline water in the North Pacific, and water with salinity between the above two, found on the equator. In three meridional sections (160°W–160°E), the Tropical Water of eastern South Pacific origin extends further equatorward than the climatological data of Levitus (1982).  相似文献   

11.
印度洋-西太平洋海洋动物谱系地理演化格局   总被引:2,自引:1,他引:1  
印度洋和西太平洋海域,拥有大量浅海大陆架、边缘海和岛屿,孕育了全球最丰富的初级生产力和渔业资源,尤其是作为该区域陆源物质输入、两大洋能量汇聚中心和生物多样性中心的东印度三角,在全球海洋生物分布和进化中扮演了重要角色。本文结合物理海洋和化学海洋环境,通过线粒体基因和核基因等分子标记研究结果,归纳分析了印度洋和西太平洋区域海洋动物谱系生物地理演化格局及其可能的成因。具体结果如下:(1)雷州半岛-海南岛、冰期暴露的台湾海峡和长江冲淡水等沿岸海区,阻碍了海洋动物在海区间的扩散,南海、东海和黄、渤海广布类群,多由一个星状辐射谱系组成,种群经历最近的数量扩张和区域扩散,而仅分布于南海的物种,一般具有多个深度分歧的遗传谱系,种群呈现出数量平衡状态,同一广布物种的南海和东海种群,因区域海洋环境差异,种群数量动态演化历史不同;(2)黑潮影响区的沿岸广布类群,黑潮海流促进了顺流扩散、限制了跨海流基因交流;(3)东印度三角区,存在"华莱士线"、"赫胥黎线"和"印度洋-太平洋线"等生物地理边界,该区域海洋或咸淡水溯河洄游动物多呈现为分布在生物地理边界两侧的2个遗传谱系;(4)西太平洋,存在与目前东西向大洋环流垂直的南北向跨赤道扩散和基因流现象,可能受到目前南北向随季节反转的沿岸流和深层海流影响;(5)印度洋东西海岸共享物种,受印度洋西向赤道流影响,海洋动物多由东印度洋向西印度洋跨洋扩散;(6)西印度洋广布物种/类群,呈现了两种不同种群分化格局——遗传同质均一种群和深度分化的遗传谱系;(7)东、北印度洋和南海区域共享大量物种,可能是海盆间双向扩散的结果;(8)海洋生物谱系生物地理进化史信息,可以用于地质事件、海洋环流和古气候重建。  相似文献   

12.
根据美国TOGA水位中心所提供的1975—1988年水位月平均资料,分析、讨论了热带西太平洋水位的年际变化特征,特别是与ENSO事件有关的低水位现象。此外,还重点叙述了1986—1987年ENSO事件中水位沿经向和赤道剖面的变化,以及与此有关的赤道流系的变化。文中还定性地讨论了赤道开尔文波沿赤道剖面的传播特性。  相似文献   

13.
14.
为了解西太平洋菲律宾海浮游动物丰度和生物量的水平分布特征,于2012年11月26日至2012年12月12日对菲律宾海上层海洋(0—200m)的浮游动物进行了调查。调查站位分别位于受赤道逆流(NECC)、棉兰老流(MC)、北赤道流(NEC)和黑潮(KC)影响的海域。通过比较浮游动物的丰度和生物量(分别用干重,灰分,无灰干重和含能量等指标表示),探讨不同海流中浮游动物的分布特征。结果表明:桡足类、毛颚类和水母类是菲律宾海浮游动物的三大主要类群。调查海域浮游动物丰度为11—116ind./m3,NECC区平均丰度最高((96±28)ind./m3),然后依次是MC区和KC区,NEC区最小((26±9)ind./m3)。在浮游动物生物量(干重)方面,同样NECC区最高((3.25±1.11)mg/m3),其次为MC区,但是平均丰度最小的NEC区生物量超过KC区。造成这一差异的主要原因,可能是由于KC区的浮游动物具有更高的含水量以及较小个体所占比例较高。不同水团之间浮游动物灰分、无灰干重和含能量的分布特征与干重相一致。结合环境因子分析显示,上升流、叶绿素a、初级生产力、海流和温度等因素对浮游动物的分布具有一定影响。  相似文献   

15.
This paper analyses the sea surface temperature (SST) of the eastern Pacific Ocean, the Kuroshio in the East China Sea, the subtropical high pressure of the Pacific Ocean and the precipitation for rainy season of Qingdao. We obtain a result that if this year the eastern Pacific Equatorial Zone is a warm-water year, the Kuroshio path in the East China Sea for next year will be subject to oscillation westward. The SST of the eastern Pacific Ocean may predict precipitation for rainy season of Qingdao one year earlier than that of the Kuroshio in the East China Sea.  相似文献   

16.
海山可以通过与洋流的相互作用改变水体结构,促进悬浮体以及海洋生物的再分配,进而影响海洋生物地球化学过程,促进大洋物质和能量交换。西太平洋有着复杂的环流结构,也是海山分布最多的海区之一。为研究西太平洋海山区的悬浮体分布及其控制机制,2017年夏季在西太平洋卡罗琳M4海山区进行现场调查,利用扫描电镜分析了该海山区悬浮体样品的物质组成及分布,并结合温度、盐度和荧光叶绿素a浓度数据,讨论了海山对悬浮体分布的影响。结果表明,M4海山区的悬浮体由生物碎屑、矿物颗粒和絮凝体等组成。海水的强烈层化阻碍了该海山区下层营养物质的上涌,使上层水体呈现出寡营养的特征,导致大部分站位悬浮体丰度较低;但在海山顶部,潮流和海山地形相互作用在山顶上方形成反气旋环流,不仅促进了深水的营养物质向上扩散,使得荧光叶绿素a浓度升高,同时对平流输送来的以及从深水中上涌的悬浮体起到了滞留作用,使山顶上方的悬浮体丰度远高于离山顶较远的位置。随着水深的增大,温、盐跃层的强度减弱,水体中的营养盐浓度升高,为浮游生物的生长提供了适宜的环境,进而使生物碎屑及絮凝体的丰度升高。北赤道潜流挟带来自西太平洋近岸海区的陆源矿物颗粒到达M4海山区,...  相似文献   

17.
用赤道太平洋长达21a的温度资料以及经验正交函数(EOF)分析方法,讨论了在5°S-5°N平均纬向垂直剖面上赤道太平洋垂向温度梯度距平的时空变化,得到了一些有意义的结果。赤道太平洋垂向温度梯度距平EOF分析第1模态的正/负位相反映了El Nino/La Nina发生前赤道太平洋温跃层的分布,第2模态的正/负位相反映了El Nino/La Nina鼎盛以及开始衰减时赤道太平洋温跃层的分布。根据我们对赤道太平洋温跃层核心位置的定义,在El Nino向LaNina转换的过程中,赤道东太平洋温跃层上升了30-40m,而赤道中太平洋温跃层先是上升了40-50m,然后又下降了40-50m,赤道西太平洋温跃层下降了90m;随着赤道西太平洋暖水的堆积以及东移,温跃层首先在赤道西太平洋加深,El Nino发生前赤道中东太平洋温跃层开始加深,El Nino达到鼎盛时赤道西太平洋温跃层抬升,而赤道中东太平洋温跃层加深;赤道太平洋垂向温度梯度距平EOF分析第1特征向量的时间系数与Nino3区的SST距平有非常好的相关,并且超前于Nino3区的SST距平,超前3个月的相关系数高达0.7017,超前6个月的相关系数高达0.6467,因此可以用该量来预测Nino3区的SST距平。  相似文献   

18.
为了模拟以南、北赤道流、赤道逆流和赤道潜流为特征的赤道流系,从长时间平均的线性化的海水运动方程出发,考虑海水层化、保留经向摩擦作用,利用赤道太平洋中部海区经向流通量不随纬度变化的量阶估计,得到海水密度跃层对赤道风场的响应,即跃层深度的分布规律,然后应用我们已构建的改进Fourier方法求解(由于地转口效应所引入的)变系数的海水运动方程,得到适用于中部赤道太平洋的级数形式的三维流场解。  相似文献   

19.
热带太平洋与热带大西洋海表温度主模态的相互作用   总被引:2,自引:0,他引:2  
郑建  刘秦玉 《海洋与湖沼》2010,41(6):799-806
根据英国Hadley气候中心的海表温度资料和美国NCEP/NCAR中心的大气资料,研究了热带太平洋与热带大西洋海表温度主模态的相互作用。热带太平洋的ENSO可以导致大西洋Nino模态或经向偶极子模态,这主要是通过热带海洋-大气相互作用,或大气的太平洋-北美遥相关过程实现的。大西洋Nino模态的暖(冷)位相会导致赤道中东太平洋的海表温度降低(升高)。这可能是通过两种途径完成的:一种可能是大西洋Nino使印度洋增暖(变冷),进而引起赤道中太平洋的东(西)风异常,通过海洋-大气相互作用正反馈机制能发展成为La Nina(El Nino),使赤道东太平洋海温降低(升高);另一种可能是大西洋Nino直接可以导致太平洋Walker环流增强(减弱),从而使赤道东太平洋海温降低(升高)。  相似文献   

20.
Circulations associated with the Indonesian Throughflow (IT), particularly concerning subsurface currents in the Pacific Ocean, are studied using three types of models: a linear, continuously stratified (LCS) model and a nonlinear, -layer model (LOM), both confined to the Indo-Pacific basin; and a global, ocean general circulation model (COCO). Solutions are wind forced, and obtained with both open and closed Indonesian passages. Layers 1-4 of LOM correspond to near-surface, thermocline, subthermocline (thermostad), and upper-intermediate (AAIW) water, respectively, and analogous layers are defined for COCO.The three models share a common dynamics. When the Indonesian passages are abruptly opened, barotropic and baroclinic waves radiate into the interiors of both oceans. The steady-state, barotropic flow field from the difference (open − closed) solution is an anticlockwise circulation around the perimeter of the southern Indian Ocean, with its meridional branches confined to the western boundaries of both oceans. In contrast, steady-state, baroclinic flows extend into the interiors of both basins, a consequence of damping of baroclinic waves by diapycnal processes (internal diffusion, upwelling and subduction, and convective overturning). Deep IT-associated currents are the subsurface parts of these baroclinic flows. In the Pacific, they tend to be directed eastward and poleward, extend throughout the basin, and are closed by upwelling in the eastern ocean and Subpolar Gyre. Smaller-scale aspects of their structure vary significantly among the models, depending on the nature of their diapycnal mixing.At the exit to the Indonesian Seas, the IT is highly surface trapped in all the models, with a prominent, deep core in the LCS model and in LOM. The separation into two cores is due to near-equatorial, eastward-flowing, subsurface currents in the Pacific Ocean, which drain layer 2 and layer 3 waters from the western ocean to supply water for the upwelling regions in the eastern ocean; indeed, depending on the strength and parameterization of vertical diffusion in the Pacific interior, the draining can be strong enough that layer 3 water flows from the Indian to Pacific Ocean. The IT in COCO lacks a significant deep core, likely because the model’s coarse bottom topography has no throughflow passage below 1000 m. Consistent with observations, water in the near-surface (deep) core comes mostly from the northern (southern) hemisphere, a consequence of the wind-driven circulation in the tropical North Pacific being mostly confined to the upper ocean; as a result, it causes the near-surface current along the New Guinea coast to retroflect eastward, but has little impact on the deeper New Guinea undercurrent.In the South Pacific, the IT-associated flow into the basin is spread roughly uniformly throughout all four layers, a consequence of downwelling processes in the Indian Ocean. The inflow first circulates around the Subtropical Gyre, and then bends northward at the Australian coast to flow to the equator within the western boundary currents. To allow for this additional, northward transport, the bifurcation latitude of the South Equatorial Current shifts southward when the Indonesian passages are open. The shift is greater at depth (layers 3 and 4), changing from about 14°S when the passages are closed to 19°S when they are open and, hence, accounting for the northward-flowing Great Barrier Reef Undercurrent in that latitude range.After flowing along the New Guinea coast, most waters in layers 1-3 bend offshore to join the North Equatorial Countercurrent, Equatorial Undercurrent, and southern Tsuchiya Jet, respectively, thereby ensuring that northern hemisphere waters contribute significantly to the IT. In contrast, much of the layer 4 water directly exits the basin via the IT, but some also flows into the subpolar North Pacific. Except for the direct layer 4 outflow, all other IT-associated waters circulate about the North Pacific before they finally enter the Indonesian Seas via the Mindanao Current.  相似文献   

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