热带大西洋表层环流及其月变化特征的分析

应用1993年4月至2001年3月的TOPEX/Poseidon卫星高度计遥感资料,分析了8 a平均热带大西洋(15°S～25°N,5°～50°W)表层环流结构的月变化特征.研究结果表明:热带大西洋表层环流中高纬度海区流速较小,赤道附近流速较大,表层环流系统大部分流系月变化不明显,部分流系月际波动较显著.具体来说,西南向的北赤道流下半年的纬向流速分量比上半年大.非洲沿岸流在5～11月流向为东北向,在其他月份主要为东南向.北赤道逆流可以分成两部分:25°W以东海区,北赤道逆流常年流向向东,到9月份前后流速达到最大值(约0.25 cm/s);25°W以西海区,7月至翌年1月流向向东,2～6月北赤道逆流减小,并有西向流产生.2°S～2°N,15°W以东海区的南赤道流在1～3月、9～10月流向向东,其他月份流向向西.南赤道流可认为是由南、北两支西向的海流构成,这两支海流的流轴分别位于6°S和1°N,在6～7月北支流速达到最大值0.6 m/s.南美洲纳塔耳东部西北向的北巴西海流流速月际变化不大,在5～6月份流速达到最大值0.3～0.4 m/s.相应的卫星风场遥感资料的分析表明热带大西洋表层环流结构的月变化特征与风场的分布及变化有较好的对应关系.用World Ocean Atlas 2001的月平均温盐数据反演出来的表层地转流场以及卫星跟踪ARGOS漂流浮标观测进行的对比验证表明,上述遥感分析的地转流场结果与水文数据以及海上观测结果一致.     

西北太平洋副热带逆流、北赤道流、北赤道逆流几个特征的比较

根据137°E断面1967～1995年冬、夏季的温、盐资料,计算和分析该断面的地转流;分析144°E断面上投放卫星跟踪漂流浮标的漂移轨迹;结合CSK图集中的海面重力势分布,对副热带逆流、北赤道流和北赤道逆流几个特征的相同点和不同点进行比较,得出若干有益的结论:(1)副热带逆流、北赤道流、北赤道逆流,并不是单纯的单支海流,而是存在着两支或多支现象;(2)流速结构的带状分布,东、西向流相互交错间隔出现,流层较浅,均为表层流或近表层流;(3)多年平均而言,3支海流的流速以北赤道逆流最强,北赤道流次之,副热带逆流最弱;流量则不同,北赤道流最大,副热带逆流最小,北赤道逆流居中.3支海流的流速夏季均大于冬季,但流量稍有差异:副热带逆流和北赤道流均具有夏强、冬弱的特点,而北赤道逆流为冬强、夏弱;(4)冬季,副热带逆流的"源地",位于巴士海峡和台湾以东"副热带脊"的一个"暖脊"中心附近海域;(5)冬季,卫星跟踪漂流浮标的漂移轨迹,基本上反映出北赤道流和北赤道逆流的路径.但因副热带逆流区为涡旋频繁区,致使浮标漂移轨迹难以反映出副热带逆流的路径.     

赤道暖池区漂流浮标运动轨迹分析

TOGA—COARE强化观测期间,对赤道暖池区海流作了多种方法、多层次的观测;根据美国释放的漂流浮标不同时刻位置的资料,分别对赤道及其南、北海域的表层漂流状况作了计算分析,指出:从1°N向北存在单一的北向流;从1°N～1°S这个近赤道区域内为东向流;1°N～2°S区域为过渡区,以东向流为主,个别浮标出现涡旋状运动。2°S以南为一反时针运动的大涡旋。     

利用卫星高度计资料分析热带大西洋表层环流的季节性变化

利用1993年4月至2001年3月的TOPEX/POSEIDON卫星高度计遥感资料,研究了热带大西洋(15°S-25°N,50°W-5°W)海面高度距平和表层环流结构的季节性变化。研究结果表明:夏季和冬季海面高度距平分布呈相反的结构,低纬度海区(0°-15°N之间的海区)海表风应力旋度所产生的Ekman抽吸而导致的海面升降是该海区海面高度距平季节性振荡的重要影响因素。热带大西洋表层流结构大部分海域季节变化不明显,部分流系具有明显季节振荡,东向的北赤道逆流夏季强度较大,冬、春季流速较小;非洲沿岸流冬季流向为东南向,其他季节流向为东北向。值得一提的是,几内亚海湾表层流秋、冬季为东向,而春、夏季为西向。通过卫星跟踪ARGOS漂流浮标观测结果进行的对比验证表明,上述遥感资料分析的表层地转流场与海上观测结果一致。     

一个耦合模式下北赤道流分叉的初步研究

利用一个全球海洋-大气耦合模式,对北赤道流分叉的季节、年际变化特征进行了初步研究.模式结果表明北赤道流的分叉纬度,在表层大约是15.2°N,随深度而向北移动,在1000m深度大约为20°N.北赤道流分叉在春、夏季节偏南,而秋、冬季节偏北,可能主要与局地的Ekman抽吸有关.北赤道流分叉的年际变化周期表现有准2年、3～4...     

137°E 断面北赤道流的结构特征和年际变化

基于日本气象厅在1967～2009 年间获得的温盐深仪(CTD)资料以及美国提供的卫星高度计资料,分析了137°E 断面北赤道流(NEC)的结构特征和年际变化, 并探讨了其年际变化的控制机制。结果表明,在137°E 断面, NEC 的平均位置位于8°～18°N, 其流核出现在10°～12°N 附近; 无论冬季还是夏季, NEC的流速距平场都具有南、北向的反位相年际振荡特征, 而这种南、北向的反位相振荡可能是由热带西北太平洋的气旋性和反气旋性异常环流所控制; NEC 内部的流速对EI Ni?o-Southern Oscillation (ENSO)的响应也存在着明显的季节特征, 其中, 在El Ni?o(La Ni?a)期间的夏季, NEC 中上部的流速增大(减小); 在El Ni?o(La Ni?a)期间的冬季, NEC 中下部的流速减小(增大), 而NEC 南、北两侧的流速则增大(减小)。     

基于OFES模式数据的北赤道流分叉研究

利用1957—2006 共50 年高分辨率的长时间序列海洋模式OFES(OGCM for the Earth Simulator)数据, 对北赤道流(NEC)的分叉规律及其与ENSO循环的关系进行了分析。结果表明: (1) NEC分叉纬度具有明显的季节和年际变化, 周期主要呈现为3—6个月的季节内振荡和2年、2—7年左右ENSO尺度周期振荡以及10年以上的年代际变化。在季节尺度上, 分叉位置春季偏南, 秋季偏北, 并且分叉纬度随深度的增加向北移动, 其北移幅度冬季最大, 夏季最小。而在年际变化尺度上, NEC分叉纬度具有较强的年际变化信号, 与ENSO循环密切相关, El Ni?o 年分叉位置偏北, La Ni?a年分叉位置偏南。(2)NEC分叉纬度的变化与北太平洋0—30°N之间的纬向风应力旋度积分零线位置密切相关, 零线的南北偏移导致了分叉位置的改变, 在不同深度上, 零线位置对分叉纬度改变的影响时间不同, 表层需1个月, 而500 m深度则需4个月左右。(3)NEC分叉影响着黑潮(KC)与(棉兰老流)MC的流量分配率, 其年际异常变化与冷、暖ENSO事件发生密切相关, 当El Ni?o发生时, KC流量分配率减少, MC 流量分配率增加; La Ni?a年情况则相反。     

一个高分辨率太平洋-印度洋海盆环流模式的初步结果

利用LASG/IAP发展的一个0.25°×0.25°高分辨率太平洋-印度洋海盆环流模式,初步分析了模式在太平洋区域的模拟结果,并与海洋同化资料以及前人的研究结果作比较,检验此模式对该区域平均气候态、年际变化的模拟能力。分析表明,模式较好地再现了海表温度（SST）分布、赤道温跃层和纬向流结构、赤道流系分布形态、海表高度以及正压流函数空间分布特征;同时,对显著的El Ni?o和La Ni?a事件的模拟等方面与Simple Ocean Data Assimilation（SODA）2.0.2版本结果相近。此外,模式模拟北赤道流（NEC）分叉点位置的季节和年际变化以及吕宋海峡流量的年际变化与已有研究结果基本一致。进一步分析还发现,在年际尺度上,NEC分叉点位置和吕宋海峡流量与ENSO密切相关。     

137°E赤道潜流1月年际变化及其原因的探讨

利用日本海洋调查船沿137°E断面8°N—1°S之间、1968—1985年每年1月份的海流实测资料,分析了该断面上赤道潜流的变化。资料表明,该处赤道潜流位于1°—2°N之间的温跃层中、下部,其单、双核结构均可出现,且下层流核之流速多大于上层流核。该处潜流1月年际变化明显,一般E1 Nino(简称EN)后期流速小于非EN时期。这主要是由于EN初期夏、秋季中太平洋信风风场发生变化,从而导致赤道及热带太平洋纬向压力梯度变化。此外,137°E赤道潜流与其两侧流的经向辐合关系密切,这表明了北赤道逆流和南赤道流对潜流的可能影响。     

南海北部次表层盐度的变化及其与北赤道流分叉点的关系

吕宋海峡是南海与外界水交换的重要通道,黑潮作为北太平洋最强的1支西边界流,在经过吕宋海峡时会对南海北部的环流和环境产生重要影响。本文用1991—2011年期间CTD断面实测资料和高度计资料,提取23.0~25.5 kg/m³等密度面之间的盐度极大值,研究了南海北部不同年月盐度极大值变化、黑潮入侵方式与强弱,以及盐度极大值变化与北赤道流分叉点南北移动的关系,结果表明:(1)黑潮入侵南海方式多样,既有分支形式,也有弯曲、流套形式。(2)不同年月间,黑潮入侵南海的强弱存在较大差别,120°E断面的次表层盐度极大值的变动可超过0.3。(3)北赤道流分叉点位置的南北变动对黑潮入侵南海的强弱具有重要影响:北赤道流分叉点位置偏北,黑潮入侵南海较强;北赤道流分叉点位置偏南,则黑潮入侵相对较弱。     

关于海洋中的正压流和斜压流问题的讨论

关于海洋中的正压流和斜坛流的概念，目前存在着３种不同的提法．本文首先分别简述它们在定义上的差别，然后对３种定义在理解海流性质问题上的长、短处加以评述。一些理论物理海洋学家依据地转关系式，把与海面倾斜相连系的流视为正压流部分，而与密度不均匀性有关的视为斜压流部分。笔者认为这种定义在物理概念上是清楚，在实际应用中是方便，因此在讨论海流性质时最好采用这种观点。     

The Current Structure of the Tsushima Warm Current along the Japanese Coast

The branching of the Tsushima Warm Current (TWC) along the Japanese coast is studied based upon intensive ADCP and CTD measurements conducted off the Wakasa Bay in every early summer of 1995–1998, the analysis of the temperature distribution at 100 m depth and the tracks of the surface drifters (Ishii and Michida, 1996; Lee et al., 1997). The first branch of TWC (FBTWC) exists throughout the year. It starts from the eastern channel of the Tsushima Straits, flows along the isobath shallower than 200 m along the Japanese coast and flows out through the Tsugaru Strait. The current flowing through the western channel of the Tsushima Straits feeds the second branch of TWC (SBTWC) which develops from spring to fall. The development of SBTWC propagates from the Tsushima Straits to Noto Peninsula at a speed of about 7 cm sec⁻¹ following the continental shelf break with a strong baroclinicity. However, SBTWC cannot be always found around the shelf break because its path is influenced by the development of eddies. It is concluded that SBTWC is a topographically steered current; a current steered by the continental shelf break. Salient features at intermediate depth are the southwestward subsurface counter current (SWSCC) between 150 m and 300 m depths over the shelf region in 1995–1998 with the velocity exceeding about 5 cm sec⁻¹, although discrepancies of the velocity and its location are observed between the ADCP data and the geostrophic currents. This revised version was published online in August 2006 with corrections to the Cover Date.     

Current structure and volume transport of the Soya Warm Current in summer

ADCP, CTD and XBT observations were conducted to investigate the current structure and temperature, salinity and density distributions in the Soya Warm Current (SWC) in August, 1998 and July, 2000. The ADCP observations clearly revealed the SWC along the Hokkaido coast, with a width of 30–35 km and an axis of maximum speed of 1.0 to 1.3 ms⁻¹, located at 20–25 km from the coast. The current speed gradually increased from the coast to a maximum and steeply decreased in the offshore direction. The SWC consisted of both barotropic and baroclinic components, and the existence of the baroclinic component was confirmed by both the density front near the current axis and vertical shear of the alongshore current. The baroclinic component strengthened the barotropic component in the upper layer near the axis of the SWC. The volume transport of the SWC was 1.2–1.3 SV in August, 1998 and about 1.5 SV and July, 2000, respectively. Of the total transport, 13 to 15% was taken up by the baroclinic component. A weak southeastward current was found off the SWC. It had barotropic characteristics, and is surmised to be a part of the East Sakhalin Current.     

Predicting the East Australian Current

Results are presented from an ensemble prediction study (EPS) of the East Australian Current (EAC) with a specific focus on the examination of the role of dynamical instabilities and flow dependent growing errors. The region where the EAC separates from the coast, is characterized by significant mesoscale eddy variability, meandering and is dominated by nonlinear dynamics thereby representing a severe challenge for operational forecasting. Using analyses from OceanMAPS, the Australian operational ocean forecast system, we explore the structures of flow dependent forecast errors over 7 days and examine the role of dynamical instabilities. Forecast ensemble perturbations are generated using the method of bred vectors allowing the identification of those perturbations to a given initial state that grow most rapidly. We consider a 6 month period spanning the Austral summer that corresponds to the season of maximum eddy variability. We find that the bred vector (BV) structures occur in areas of instability where forecast errors are large and in particular in regions associated with the Tasman Front and EAC extension. We also find that very few BVs are required to identify these regions of large forecast error and on that basis we expect that even a small BV ensemble would prove useful for adaptive sampling and targeted observations. The results presented also suggest that it may be beneficial to supplement the static background error covariances typically used in operational ocean data assimilation systems with flow dependent background errors calculated using a relatively cheap EPS.     

On the Taiwan Warm Current Water

Using our data from special observation in the source area of the Taiwan Warm Current from 19S2 to 1985) and historical data, the authors conducted studies to clarify the temperature and salinity characteristics, variability, and origin of the Taiwan Warm Current Water, and its influence on the expanding direction of the Changjiang Diluted Water.The main results of these studies are briefly given below. (1) The Taiwan Warm Current Water can be divided into two parts:the Surface Water of the Taiwan Warm Current and the Deep Water of the Taiwan Warm Current; the former is formed due to the mixing of the Kuroshio Surface Water flowing northward along the east coast of Taiwan with the Taiwan Strait Water; the latter completed originates from Kuroshio Subsurface Water to the east of Taiwan. It is characterized by lower temperature and higher salinity in summer and the characteristics of temperature and salinity are more stable. The maximum seasonal variational range and maximum secular variational range of t     

南海东部区域的海流状况——Ⅰ.潮流性质

对南海东部海域 1 997- 1 998年实测海流资料进行了分析。统计得出潮流各方向的出现频率、平均流速及最大流速、各月平均流速和最大涨落潮流速及流速和流向的联合分布 ;经调和分析 ,给出了各主要分潮流的调和常数和潮流椭圆要素 ;确定该区域属于正规全日潮流性质。     

Upwelling in the Southern Benguela Current

This survey of the southernmost significant upwelling site in the Benguela Current showed that the oceanography is dominated by the seasonal wind cycle of predominant S-E winds in summer and N-W winds in winter. In the upwelling season, extending from September to March, a semi-permanent plume is isolated by a pronounced oceanic front whose position varies in the short-term and is related to wind direction. Surface waters change immediately and deeper waters more slowly to fluctuations in wind. The rate of upwelling was statistically related to wind data. A maximum rate of 32 m day^?1 was found.In spring low temperature and salinity water flows northward on the shelf while between late summer and later winter oxygen-depleted water, rich in nutrients, flowed south at an estimated rate of 7–21 × 10⁴ m³ s^?1 in a counter current to the Good Hope Jet.Local depletion of oxygen occurs due to phytoplankton decomposition caused, in autumn, by falling light levels and, in summer in calm periods, by nitrate depletion (<1 μg-at N 1^?1). Primary productions is estimated at 3.7 kg C m^?2 yr^?1 with a maximum growth rate (PI_max) = 17.4–19.0 mg C mg chlorophyll a^?1 hr^?1 and half-saturation constant (K_S) = 0.4–1.1 μg-at N 1^?1. Nutrients were utilized and oxygen produced: ΔP:ΔN:ΔSi:ΔO=1:19.1 to 23.3:17.5 to 23.3:?227 to ?293. High N:Si ratios (maximum 4.28) were found in oxygen-depleted water produced locally while that coming from the north had low ratis, due to resolution of silica from the sediments and nitrate reduction. The mean zooplankton standing stock, 2.3 g dry weight m^?2, was 12% of the phytoplankton crop. In summer stocks were maximal 40–100 km and minimal 20–50 km from the coast while in winter they were maximal inshore. Little vertical migration occurred and the waters above the thermocline contained the majority of the population.     

南海东部区域的海流状况——Ⅱ.海洋激流现象

用南海东部 1 997年 1 1月实测的高密度海流资料 ,分析了海流的形态。发现了海洋激流现象 ,它具有流速特别大、持续时间短暂和突然发生以及随机现象等复杂性质     

On the stability of the Soya Warm Current

The stability of the Soya Warm Current is examined, in an attempt to explain the mechanism of the formation of the wave-like pattern seen in satellite infrared imagery in summer. A linear stability theory is applied to barotropic shear flows over a realistic bottom topography. Effects of bottom friction are also taken into consideration. For this current in summer, when volume transport is greatest, the possibility of barotropic instability is suggested. The most unstable waves obtained in this study have wavelengths of 60–80 km, periods of about 1. 5 days, and phase velocities of 45–55 cm sec^–1, which is in good agreement with observations.     

Freshwater export from the Labrador Current to the North Atlantic Current at the Tail of the Grand Banks of Newfoundland

Historical hydrographic data, spanning the period 1896–2006, are used to examine the annual mean and seasonal variations in the distribution of freshwater along and across the shelf/slope boundary along the Labrador and Newfoundland Shelves and the Grand Banks of Newfoundland. Particular attention is paid to the export of freshwater along the eastern Grand Banks, between Flemish Cap and the Tail of the Grand Banks, as this has long been identified as a preferential region for the loss of mass and freshwater from the boundary. The data are combined into isopycnally averaged long-term annual and monthly mean gridded property fields and the evolving distribution of fresh arctic-origin water is analyzed in fields of salinity anomaly, expressed as departures from the “central water” temperature–salinity relation of the Gulf Stream. The climatology confirms that cold/fresh northern-source waters are advected offshore within the retroflecting Labrador Current along the full length of the boundary between Flemish Cap and the Tail of the Grand Banks. In fact, it is estimated that most of the equatorward baroclinic transport at the boundary must retroflect back toward the north in order to explain the annual mean distribution of salinity in the climatology. While the retroflection of the Labrador Current appears seasonally robust, the freshwater distribution within the retroflection region varies in response to (1) the freshness of the water available for export which is set by the arrival and rapid flushing of the seasonal freshwater pulse at the boundary, (2) seasonal buoyancy forcing at the surface which alters the vertical stratification across the retroflection region, restricting certain isopycnal export pathways, and (3) the density structure along the eastern Grand Banks, which defines the progressive retroflection of the Labrador Current.