2013年南沙群岛海域温跃层的季节变化及形成机理

利用调查数据及遥感数据揭示了2013年南沙群岛海域温跃层的季节变化特征,温跃层上界深度平均值春、夏、冬季基本一致,介于45~47 m之间,秋季最大,达60 m;温跃层厚度平均值夏、秋、冬季基本一致,介于85~87 m之间,春季相对较小,为78 m。温跃层强度平均值春、夏、秋、冬季几乎一致,介于0.13~0.15℃/m之间。调查海域温跃层上界深度季节变化的形成机理为:春季西深东浅的原因是西部受净热通量较小、大风速、负的风应力旋度以及中南半岛东部外海的中尺度暖涡和反气旋环流共同作用,东部近岸海域净热通量高值、风速相对较小及风应力旋度引起的Ekman抽吸效应共同控制;夏季深度分布较均匀的原因是10°N以北风致涡动混合强但受Ekman抽吸影响,10°N以南风致涡动混合弱但风应力旋度为负值;秋季深度较其他季节平均加深15 m的原因是南沙群岛海域被暖涡占据,暖涡引起的反气旋式环流使得温跃层上界深度被海水辐聚下压;冬季正的风应力旋度产生的Ekman抽吸和冷涡引起的气旋式环流共同作用,使得温跃层上界深度较秋季平均抬升15 m。     

孟加拉湾局地动力过程的季节变化研究

利用观测资料和理论模型,研究了孟加拉湾海表面高度的季节循环.结果表明,局地风应力旋度驱动的斜压Rossby波是孟加拉湾海表高度季节循环的主要控制因子,而孟加拉湾海底地形分布也影响了海表面高度的季节循环.受风应力旋度驱动的斜压Rossby波在短时间内就可以穿越孟加拉湾海盆,使得海洋温跃层在短时间内完成了对Rossby波的响应,保证了上层海洋满足准静止的Sverdrup平衡.在夏季(冬季)西南(东北)季风驱动下,上层海洋分别在孟加拉湾北部和南部形成气旋(反气旋)式和反气旋(气旋)式环流.     

粤西陆架温度锋三维结构与季节变化机制分析

基于2018–2019年现场高分辨率温度观测和1993–2021年的CMEMS再分析海表温度（SST）和风场数据,分析粤西陆架海温盐锋的三维结构、季节变化和影响机制。多年SST数据显示,海表温度锋冬季最强、出现概率和覆盖宽度最大,量值分别为0.049℃/km、75%和66 km。春季和夏季次之,而秋季则几乎完全消失。冬季锋面平均离岸50 km,夏季则向岸靠近为23.1 km。2018年春季、夏季和2019年夏季的现场观测进一步给出锋面在次表层的三维结构,结果显示春、夏季20 m等深线以浅处均有锋面存在,该锋面是沿岸高温海水与离岸低温海水辐聚而成,随着深度的增加锋面强度减小,覆盖范围向岸收缩。20 m以深水域锋面在次表层中强于表层,随深度增加而增强并向岸偏移。相关性和信息流分析发现,海表面风应力旋度和沿岸风是影响粤西陆架海表温度锋面的重要因素。该温度锋存在年际变化,PDO负位相时的La Niña年锋面强度出现极大值,而PDO正位相时的El Niño年则对应极小值。     

琼东和粤西海表温度锋的季节与年际变化特征分析

以2006—2013年卫星遥感海表温度资料(GHRSST SST)为基础,通过数字图像处理的边缘检测方法提取温度锋面的核心位置,分析了琼东、粤西海域海表温度锋位置及强度的季节变化和年际变化特征,并进一步结合海面高度异常资料和海面风场资料探讨了温度锋变化的可能机制。分析结果表明,琼东、粤西海域温度锋的空间分布及锋面强度存在显著的季节变化,沿岸风应力是影响该海域锋面变化的主要动力因素。夏季温度锋面主要分布于琼东沿岸的东部及南部海域近岸50m到100m等深线之间,而冬季则主要分布在琼东的东部海域和粤西沿岸20m到100m等深线之间,春秋两季为其过渡季节;锋面强度的季节变化表现为冬季最强,春季、夏季次之,秋季最弱,其冬季锋面强度平均值可达到3℃?100km–1,夏季为1.7℃?100km–1;同时,锋面核心位置及强度的分析结果表明,琼东和粤西海域温度锋也存在较强的年际变化。     

台湾西南部海域风应力旋度偶极子的季节和年际变化分析

利用1995~2013年间NCEP风场资料,分析研究了台湾西南部海域风应力旋度偶极子的季节和年际变化特征,及其受ENSO事件的影响,结果表明:台湾西南部海域风应力旋度偶极子的分布存在明显季节变化,其分布期主要集中于每年10月至次年4月,夏季台湾海峡不存在风应力旋度偶极子的分布;风应力旋度偶极子的强度异常要滞后ENSO 1个月,当厄尔尼诺事件发生时,风应力旋度偶极子的分布强度较正常年份要弱,而当拉尼娜事件发生时,风应力旋度偶极子的分布强度较正常年份要强;风应力旋度偶极子的分布还存在准16.0个月和准45.3个月的显著年际变化周期,其变化同ENSO循环密切相关.     

北太平洋Hadley 环流纬向结构的季节和年际变化

为了描述北太平洋上空Hadley 环流的纬向结构特征, 利用NCEP 再分析资料(1979～2010 年), 研究了北太平洋上空Hadley 环流纬向结构的季节和年际变化。发现在西太平洋, Hadley 环流季节性上升支呈西北-东南倾斜, 其垂向核心位于对流层中层, 纬向核心在北半球冬季(夏季)位于日界线附近(150°E); 而永久性上升支主要在东太平洋, 其垂向核心位于对流层低层, 且沿经度东移逐渐增强。根据纬向环流结构特征, 北半球冬季环流形态分为3 个区域: 160°E 以西, 主要表现为低层辐合高层辐散;160°E～130°W, 主要表现为高层辐合; 130°W 以东, 表现为低层辐合高层辐散特征。相似地, 北半球夏季环流形态也可沿纬向分为如下3 个区域: 165°E 以西、165°E～165°W 和165°W 以东, 分别对应东亚夏季风主导经圈环流区、过渡区、Hadley 环流主导经圈环流区。在年际变化上, 北太平洋Hadley 环流与ENSO 有很强的相关, 这与前人的研究是一致的。因此北太平洋上空Hadley 环流具有显著的空间性态, 并且对应时间尺度不同, 影响其变化的主要因素也不尽相同。     

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。     

黑潮延伸体区域50-100公里涡旋分布特征

本文使用基于热成风速度的涡旋识别拓展方法,通过海表面温度数据对黑潮延伸体区域50-100公里涡旋进行研究,发现50-100公里涡旋主要分布在黑潮延伸体流轴两侧,气旋涡和反气旋涡的寿命、半径分布具有一致性。气旋涡多出现在35°N以北,反气旋涡在35°N以南比较集中,与尺度较小的中尺度涡旋分布特征较为相似。冬夏两季涡旋地理分布存在一定差异,主要与不同季节该区域海表温度梯度及风应力旋度的变化有关。35°N以南50-100公里涡旋数量的季节性变化与风速大小的季节性变化存在明显的正相关性。35°N以南50-100公里涡旋三倍半径内风速异常和风应力旋度归一化表明,气旋涡对应风速负异常而反气旋涡对应风速正异常,反气旋涡的产生依赖于风应力负旋度,气旋涡的生成与风应力正旋度有关。     

大西洋海表温度异常与中国东北地区夏季降水的关系

利用1950～1992年全球海温月平均(2°×2°)和NCAR/NCEP提供的1950～1997年全球500hPa月平均高度场(2.5°×2.5°)资料，分析了大西洋海表温度异常的特征及其与中国东北地区夏季降水的关系。结果指出北大西洋冬季海表温度经验正交展开的第二特征向量表明，海表温度的距平分布有南北差异的异常特征；其中心位置和中国东北地区夏季降水与冬季大西洋海表温度相关显著区中心基本重合北大西洋冬季海表温度出现南暖北冷异常时，同期北大西洋中高纬度地区的阻塞形势偏强，与之相对称的北太平洋北部的阻塞高压也偏强，对应来年夏季东亚西风环流指数偏低，造成东北区夏季降水偏多；反之亦然。     

大西洋海表温度异常与中国东北地区夏季降水的关系

本文利用1950～1992年全球海温月平均(2°×2°)和NCAR／NCEP提供的1950～1997年全球500hPa月平均高度(2．5°×2．5°)资料,分析了大西洋海表温度异常的特征及其与中国东北地区夏季降水的关系。结果指出北大西洋冬季海表温度经验正交展开的第二特征向量表明海表温度的距平分布有南北差异的异常特征其中心位置和中国东北地区夏季降水与冬季大西洋海表温度相关显著区中心基本重合;北大西洋冬季海表温度出现南暖北冷异常时,北大西洋中高纬度地区的阻塞形势偏强,与之相对称的北太平洋北部的阻塞高压也偏强,对应夏季东亚西风环流指数偏低,造成东北地区夏季降水偏多。     

Fronts and strong currents of the upper southeast Indian Ocean

1 IntroductionBaroclinic component is the dominant part ofAntarcticCircum polarCurrent (ACC) (FandryandPillsbury,1979),and a baroclinictransportation asso-ciatedwithfrontsmakesupthem ajoritypartoftheto-talbaroclinictransportation oftheACC (Nowlin andCliff…     

Numerical study of the Subtropical Front and the Subtropical Countercurrent

Using a multi-level numerical model, it is shown that the Subtropical Front and the Subtropical Countercurrent can be reproduced realistically in a highly idealized model, as a consequence of the coupling effect of wind driven gyre circulation and differential heating. In the model, the North Pacific Ocean is idealized as a rectangular flat-bottomed model ocean, and is driven by wind stress, which features the Westerlies and the Trades, and by heat flux through the sea surface formulated after Haney (1971).In the model ocean, a shallow front and an eastward current associated with the front are formed around the central latitude of the Subtropical Gyre, which show close similarities to the Subtropical Front and the Subtropical Countercurrent in the real ocean.Although the detailed mechanism of formation of the Subtropical Front and the Subtropical Countercurrent is not clarified in the present study, two factors are found inessential for the formation of the Subtropical Front and the Subtropical Countercurrent. First, the results of the model indicate that a small trough of wind stress curl in the lower latitudes of the Subtropical Gyre, which Yoshida and Kidokoro (1967a, b) attributed to the Subtropical Countercurrent, is not necessary for the formation of the Subtropical Front and the Subtropical Countercurrent, since they are reproduced well in the model without the trough. Second, using a model driven by meridional wind stress, it is shown that the meridional Ekman convergence, which many authors related to the Subtropical Front, is not essential for the formation of the Subtropical Front and the Subtropical Countercurrent.     

Interannual variability of the North Pacific Subtropical Countercurrent: role of local ocean–atmosphere interaction

Seasonal and interannual variability of the Subtropical Countercurrent (STCC) in the western North Pacific are investigated using observations by satellites and Argo profiling floats and an atmospheric reanalysis. The STCC displays a clear seasonal cycle. It is strong in late winter to early summer with a peak in June, and weak in fall. Interannual variations of the spring STCC are associated with an enhanced subtropical front (STF) below the surface mixed layer. In climatology, the SST front induces a band of cyclonic wind stress in May north of the STCC on the background of anticyclonic curls that drive the subtropical gyre. The band of cyclonic wind and the SST front show large interannual variability and are positively correlated with each other, suggesting a positive feedback between them. The cyclonic wind anomaly is negatively correlated with the SSH and SST below. The strong (weak) cyclonic wind anomaly elevates (depresses) the thermocline and causes the fall (rise) in the SSH and SST, accelerating (decelerating) STCC to the south. It is suggested that the anomalies in the SST front and STCC in the preceding winter affect the subsequent development of the cyclonic wind anomaly in May. Results from our analysis of interannual variability support the idea that the local wind forcing in May causes the subsequent variations in STCC.     

Relationships between long-term ocean warming,marine heat waves and primary production in the New Zealand region

ABSTRACT

We test the paradigm that in a future warmer ocean, shallower winter mixing will lead to less net primary production (NPP), by investigating whether warming between 2002 and 2018 led to changes in NPP in the Tasman Sea/New Zealand region. The 2002–18 trend in sea surface temperature (SST) was positive over most of the region, and was driven by increasingly warmer summers and marine heat waves (MHWs) rather than year-round warming. In contrast, the trends in sea surface chlorophyll (SSC) and NPP were generally positive over the Subtropical Front (STF) and in a subtropical band north-east of New Zealand, but negative elsewhere. Regressions between SSC and SST, and between spring SSC and the coldest SST during the preceding winter, show similar spatial patterns to the SSC trend. We suggest these findings reflect different ecosystem functioning in the subtropical and subantarctic biomes that are separated by the STF. We conclude that any future warming is likely to lead to less production in the Tasman Sea, but more production over the STF. Three recent MHWs had different impacts on production, but generally led to less surface biomass north of the STF and more biomass south of the front.     

Radionuclides as tracers of water fronts in the South Indian Ocean—ANTARES IV Results

Anthropogenic ⁹⁰Sr, ^239,240Pu and ²⁴¹Am were used as tracers of water mass circulation in the Crozet Basin of the South Indian Ocean, represented by three main water fronts—Agulhas (AF), Subtropical (STF) and Subantarctic (SAF). Higher ⁹⁰Sr concentrations observed north of 43°S were due to the influence of AF and STF, which are associated with the south branch of the Subtropical gyre, which acts as a reservoir of radionuclides transported from the North to the South Indian Ocean. On the other hand, the region south of 43°S has been influenced by SAF, bringing to the Crozet Basin Antarctic waters with lower radionuclide concentrations. The ²³⁸Pu/^239,240Pu activity ratios observed in water and zooplankton samples indicated that, even 35 years after the injection of ²³⁸Pu to the Indian Ocean from the burn-up of the SNAP-9A satellite, the increased levels of ²³⁸Pu in surface water and zooplankton are still well visible. The radionuclide concentrations in seawater and their availability to zooplankton are responsible for the observed ²¹⁰Po, ^239,240Pu and ²⁴¹Am levels in zooplankton.     

我国近海陆架锋面与生态效应研究回顾

海洋锋面存在于特征明显不同的2种或多种水系或水团交界处,锋面区域形成的次生环流和辐聚作用可显著影响到海洋中的物质输运与生物生产,故受到海洋学家的广泛关注。研究发现,我国近海陆架存在14个永久性的准静止锋面（渤海海峡锋面、山东半岛沿岸锋面、苏北沿岸锋面、西韩湾锋面、京畿湾锋面、济州岛西锋面、长江环形浅滩锋面、闽浙沿岸锋面、黑潮锋面、台湾沿岸锋面、闽粤沿岸锋面、珠江口沿岸锋面、琼东锋面和北部湾锋面）,且部分海域观测到双锋面、穿刺锋面和锋面波等现象。它们与陆架环流及其他动力过程（如：涡旋、内波等）共同控制着我国边缘海的物质能量输运与交换以及生物生产力格局。近岸物质沿锋面、跨锋面输运与锋区的垂向输送过程对我国边缘海生物地球化学循环和生态过程存在显著季节性影响。冬季到春季,沿岸锋面松弛能够加强物质从近岸向陆架的输运,进而在空间上调制春季藻华暴发的时间与量级;夏季到秋季,我国边缘海存在显著的潮汐锋面系统,锋面的辐聚效应以及次级环流可显著提高锋面区域的营养盐浓度和改善光照水平,对浮游植物的生长聚集起到促进作用,故在富营养化的河口与沿岸海域,锋面区域容易成为赤潮或缺氧高发区。此外,锋面的物理屏障作用使得两侧水团保持相对独立的物理与化学特征,因而在我国边缘海生境区划和生物多样性梯度变化等方面扮演重要角色,这些研究对认识我国边缘海物质循环与生物生产的控制机制具有重要作用。未来仍需充分结合观测与卫星资料,运用多过程耦合的高分辨率模型,深入认识锋面的精细结构与动态变化,加强亚中尺度和小尺度过程及其生态效应的研究。     

Seasonal variation of atmospheric coupling with oceanic mesoscale eddies in the North Pacific Subtropical Countercurrent

This study investigated the seasonal variation in the atmospheric response to oceanic mesoscale eddies in the North Pacific Subtropical Countercurrent (STCC) and its mechanism, based on satellite altimetric and reanalysis datasets. Although mesoscale eddy in the study area is more active in summer, the sea surface temperature (SST) anomaly associated with mesoscale eddies is more intense and dipolar in winter, which is largely due to the larger background SST gradient. Similarly, the impact of the oceanic eddy on sea surface wind speed and heat flux is strongest in winter, whereas its effect on precipitation rate is more significant in summer. The study revealed that the SST gradient in STCC could impact the atmosphere layer by up to 800 hPa (900 hPa) in boreal winter (summer) through the dominant vertical mixing mechanism. Moreover, the intensity of the SST gradient causes such seasonal variation in mesoscale air-sea coupling in the study region. In brief, a stronger (weaker) background SST gradient field in wintertime (summertime) leads to a larger (smaller) eddy-induced SST anomaly, thus differently impacting atmosphere instability and transitional kinetic energy flux over oceanic eddies, leading to seasonal variation in mesoscale air-sea coupling intensity.     

Seasonal variation in the three-dimensional structures of coastal thermal front off western Guangdong

The seasonal structure and dynamic mechanism of oceanic surface thermal fronts(STFs) along the western Guangdong coast over the northern South China Sea shelf were analyzed using in situ observational data, remote sensing data, and numerical simulations. Both in situ and satellite observations show that the coastal thermal front exhibits substantial seasonal variability, being strongest in winter when it has the greatest extent and strongest sea surface temperature gradient. The winter coastal thermal front begins to appear in November and disappears after the following April. Although runoff water is more plentiful in summer, the front is weak in the western part of Guangdong. The frontal intensity has a significant positive correlation with the coastal wind speed,while the change of temperature gradient after September lags somewhat relative to the alongshore wind. The numerical simulation results accurately reflect the seasonal variation and annual cycle characteristics of the frontal structure in the simulated area. Based on vertical cross-section data, the different frontal lifecycles of the two sides of the Zhujiang(Pearl) River Estuary are analyzed.     

Indices of strength and location for the North Pacific Subtropical and Subpolar Gyres

The adjustment of the North Pacific Subtropical and Subpolar Gyres towards changes in wind stress leads to different time-scale variabilities, which plays a significant role in climate changes. Based on the Simple Ocean Data Assimilation (SODA) and Global Ocean Data Assimilation System (GODAS) datasets, the variations of the Subtropical and Subpolar Gyres are diagnosed using "three-dimension Ocean Circulation Diagnostic Method", and established three types of index series describe the strength, meridional and depth center of the Subtropical and Subpolar Gyres. The above indices present the seasonal, interannual and interdecadal variabilities of the Subtropical and Subpolar Gyres, which proves well. Both the Gyres are the strongest in winter, but the Subtropical Gyre is the weakest in summer and the Subpolar Gyre is the weakest in autumn. The Subtropical Gyre moves northward from February to March, southward in October, and to the southernmost in around January, while the Subpolar Gyre moves northward in spring, southward in summer, northward again in autumn and reaching the extreme point in winter to the south. The common feature of the interannual and interdecadal variabilities is that the two gyres were weaker and to the north before 1976-1977, while they were stronger and to the south after 1976-1977. The Subpolar Gyre has made a paramount contribution to the variability on interdecadal scales. As is indicated with the Subpolar Gyre strength indices, there was an important shift from weak to strong around 1976-1977, and the correlation coefficient with the North Pacific Decadal Oscillation (PDO) indices was 0.45, which was far better than that between the Subtropical Gyre strength indices and the PDO. Tests show that influenced by small and mesoscale eddies, the magnitude of large-scale gyres strength is strongly dependent on data resolution. But seasonal interannual and interdecadal large-scale variabilities of the two gyres presented with indices is less affected by model resolution.