热带大西洋大眼金枪鱼和黄鳍金枪鱼渔场温跃层的时空变化特征     

杨胜龙  张胜茂  蒋兴伟  邹斌  化成君  周为峰 《台湾海峡》2013,32(3)

采用2007 ～2011年Argo浮标剖面温度资料研究了大西洋黄鳍金枪鱼(Thunnus albacares)和大眼金枪鱼(Thunnus obesus)延绳钓主要作业渔场温跃层的时空变化特征.研究结果表明热带大西洋黄鳍金枪鱼、大眼金枪鱼延绳钓主要作业渔场温跃层的上界深度和温度存在着明显的季节性变化.温跃层上界深度呈现出冬深夏浅的季节性变化特征,大致呈纬向带状分布,12月至翌年4月份,15°N以北海域温跃层上界深度超过80 rn,同期10°S以南海域的多低于50 m;6～10月份的则相反.在赤道纬向区域温跃层上界温度在27℃以上,往南北两侧30°区域温度值依次递减至20℃及以下.温跃层下界深度和温度没有明显的季节性变化.温跃层下界深度高值区域的空间分布呈现“W”形状,深度值在220 m以上.在25°S以南,从南美洲到非洲西沿岸海域并延伸到安哥拉外海,以及10°N非洲西海岸外海,在1a中的大部分月份里,温跃层下界深度浅于150 m.在15°N以北和15°S以南区域下界温度大于15℃,在这之间的纬向区域下界温度低于14℃.全年在大西洋西部的5 °～ 15°N和5 °～15°S区域的温跃层厚度最大,在80～150 m之间,冬季和夏季呈现相反的分布特征;温跃层强度高值在5°S～ 15°N纬向区域,尤其是大西洋东部,介于0.15 ～ 0.25℃/m之间.根据文中揭示的大西洋金枪鱼延绳钓主要作业渔场区温跃层的时空变化特征,作者建议晚上大眼金枪鱼和黄鳍金枪鱼投钩深度应该在温跃层上界深度分布的附近水域;白天捕捞黄鳍金枪鱼投钩深度应该在温跃层下界深度分布的水域附近,大眼金枪鱼投钩深度要比黄鳍金枪鱼的更深.  相似文献   

渤海表层悬沙分布季节变化特征与控制因子的数值研究     

张德强  庞重光  王延平  陈祥舰 《海洋与湖沼》2023,54(4):1015-1027

针对整个渤海海域悬浮泥沙季节变化及其影响机制的数值研究相对缺乏且机制尚不清晰,基于ROMS三维海洋模型对渤海海域水动力环境与悬沙分布开展数值模拟。模拟结果显示,渤海海峡环流终年“北进南出”,夏季环流明显强于冬季,并呈现外围逆时针环、内部顺时针环的“双环”结构。渤海中部海域在夏季存在明显的温跃层现象,其强度分布与等深线较为一致,温跃层在4月开始形成,7月最强。渤海表层悬沙分布具有显著的季节变化,冬季悬沙浓度最大,秋季次之,春季再次之,夏季最小。控制悬沙浓度的波流底切应力在秋冬季节较大,春夏相对较小,且流致切应力始终在波流切应力中占主导地位。秦皇岛海域悬沙浓度常年偏低的主要原因是位于M2无潮点附近,属于弱潮流区,底层流速相对较小,底部沉积物发生再悬浮概率较小。夏季温跃层的存在在一定程度上减小了底边界层流速,增大了流速的垂向梯度,对底部悬浮泥沙的向上扩散有明显的抑制作用。因此,温跃层的存在是造成夏季表层悬沙浓度最低的重要原因。  相似文献   

侧扫声纳声线反射和折射干扰的实验分析     

邓志军  魏建江  葛健  丰启明 《海洋测绘》2006,26(6):45-47

介绍了侧扫声纳由自身声源反射和折射衍生的两种干扰波的形成机理,提出以绘制声线图进行分析的研究方法,着重通过海上实作验证了温度跃层产生的声线弯曲对声纳的影响特点,为外业工作的设计和施测提供了几点建议。  相似文献   

A THREE-DIMENSIONAL THERMOCLINE MODEL FOR THE YELLOW SEA AND NORTHERN EAST CHINA SEA     

彭马川  张法高  焦志新 《中国海洋湖沼学报》1996,14(3):243-249

A time-dependent, three-dimensional finite difference model is presented for simulating the stratifiedYellow Sea and northem East China Sea. The mode is forced by time-dependent observed wind, surfaceflux of heat, and tidal turbulence. With this model, momentum and temperature distribution can be computed,and an approximation for the sub-grid scale effects is introduced by the use of mass and momentumexchange coefficients. The vertical exchanges are quite dependent on these assumed coefficents, whichare complicated functions of the turbulence energy of tide and wind, of the stratified strength and otherfactors. This model was applied to describe the mechanics of the variations in strength and thickness ofthe thermocline covering almost the whole Yellow Sea and northern East Chna Sea in summer. Comparisonsof the computed output with obtained survey data led to some important conclusions.  相似文献   

Variations in late Quaternary upper ocean structure of Okinawa Trough: A nannofossil approach     

Cheng Xinrong  Wang Pinxian 《中国科学D辑(英文版)》1998,41(3):290-296

The relative abundance ofFlorisphueru profunda, a calcareous nannofossil species in lower euphotic zone, affords an opportunity to study variations in upper ocean structure such as thickness of mixed layer. As revealed by the nannofossil analysis in sediments since 20 ka B. P. from three Okinawa Trough cores, the percentage ofF. profunda increased significantly from glacial to Holocene, with a declining event ca 4 ka B. P. in its southern part. Its downcore trend is similar to that ofPulleniatina obliquiloculuta, a tropical planktonic foraminifera1 species which lives in subsurface water below thermocline in the modern ocean. Their similar variations imply an eastward shift of the Kuroshio Current, a reduction in thickness of the mixed layer, a shallowing of thermocline and a possible increase of turbidity in the upper ocean during the glaciation. The eastward shift of the Kuroshio might be repeated again about 4 ka B.P. Project supported by the National Natural Science Foundation of China (Grant Nos. 49776289 and 49406067)  相似文献   

On the Second-Year Warming in Late 2019 over the Tropical Pacific and Its Attribution to an Indian Ocean Dipole Event※     

Licheng FENG  Fei LIU  Rong-Hua ZHANG  Xue HAN  Bo YU  Chuan GAO 《大气科学进展》2021,38(12):2153-2166

After its maturity, El Ni?o usually decays rapidly in the following summer and evolves into a La Ni?a pattern. However, this was not the case for the 2018/19 El Ni?o event. Based on multiple reanalysis data sets, the space-time evolution and triggering mechanism for the unusual second-year warming in late 2019, after the 2018/19 El Ni?o event, are investigated in the tropical Pacific. After a short decaying period associated with the 2018/19 El Ni?o condition, positive sea surface temperature anomalies (SSTAs) re-intensified in the eastern equatorial Pacific in late 2019. Compared with the composite pattern of El Ni?o in the following year, two key differences are evident in the evolution of SSTAs in 2019. First, is the persistence of the surface warming over the central equatorial Pacific in May, and second, is the re-intensification of the positive SSTAs over the eastern equatorial Pacific in September. Observational results suggest that the re-intensification of anomalous westerly winds over the western and central Pacific, induced remotely by an extreme Indian Ocean Dipole (IOD) event, acted as a triggering mechanism for the second-year warming in late 2019. That is, the IOD-related cold SSTAs in the eastern Indian Ocean established and sustained anomalous surface westerly winds over the western equatorial Pacific, which induced downwelling Kelvin waves propagating eastward along the equator. At the same time, the subsurface ocean provided plenty of warm water in the western and central equatorial Pacific. Mixed-layer heat budget analyses further confirm that positive zonal advection, induced by the anomalous westerly winds, and thermocline feedback played important roles in leading to the second-year warming in late 2019. This study provides new insights into the processes responsible for the diversity of El Ni?o evolution, which is important for improving the physical understanding and seasonal prediction of El Ni?o events.  相似文献   

潮汐作用下渤海温跃层波动与起伏的数值研究   总被引：1，自引：0，他引：1  

周小兵  张延廷  曾庆存 《海洋学报》2002,24(2):20-29

研究了潮汐(四大分潮 M₂,S₂,K₁,O₁同时输入)作用下渤海温跃层起伏与波动的三维数值模型(将海洋分为3层,即上混和层、跃层和下混和层),揭示了整个海区温跃层上界面处跃层起伏(在文中指每个时刻跃层波高的周期平均值)的地理分布及叠加在起伏之上的潮周期波动的时空变化,模拟出跃层波动与实测基本一致.结果发现大振幅的跃层波动均发生在海峡及近海地形突变之处.一般界面波动的波高大于甚至远远大于同一位置的表层潮波.从位相以及周期来看,潮波和跃层上下界面波动相互之间,有些海域一致,有些地方则相差甚远.跃层上界深度及厚度的梯度,对跃层起伏分布有一定的影响.跃层起伏还可能与海岸海底摩擦有关.  相似文献   

春末黄东海域溶解氧垂直结构及氧最大值初步分析     

李福荣 《中国海洋大学学报(自然科学版)》1993,(2)

根据1987年5～6月中日合作对黄东海域进行综合调查的溶解氧资料,讨论了该海区溶解氧垂直结构及氧最大值分布。指出在南黄海北部、中部及东海北部和中部的中层存在明显的溶解氧垂直分布最大值,它总是和冷水同存。并对氧最大值及垂直结构同温跃层及冷暖水之间关系进行了初步分析。  相似文献   

后向散射强度与温跃层关系研究   总被引：1，自引：0，他引：1  

吕连港  乔方利  葛人峰  卢燕  刘建军 《海洋科学进展》2003,21(4):465-470

2003年8月12-13日，用300kHz的坐底式声学多普勒海流剖面仪(ADCP)在台湾海峡北部海区进行了观测。根据回声强度计算得到的后向散射强度具有明显的日变化，这是浮游动物的垂直迁移造成的。此外，后向散射强度还与叶绿素、浊度和温度梯度有关，其中叶绿素、浊度和温度梯度对后向散射强度的贡献分别是1．41，7．73和3．54dB。温度梯度最大值的深度与后向散射强度第一个峰值的深度一致，故根据后向散射强度能推断出温跃层的位置。  相似文献   

Evaluation of the U.S. Navy’s Modular Ocean Data Assimilation System (MODAS) Using South China Sea Monsoon Experiment (SCSMEX) Data     

Peter?C.?ChuEmail author  Wang?Guihua  Chenwu?Fan 《Journal of Oceanography》2004,60(6):1007-1021

The Navy’s Modular Ocean Data Assimilation System (MODAS) is an oceanographic tool to create high-resolution temperature and salinity on three-dimensional grids, by assimilating a wide range of ocean observations into a starting field. The MODAS products are used to generate the sound speed for ocean acoustic modeling applications. Hydrographic data acquired from the South China Sea Monsoon Experiment (SCSMEX) from April through June 1998 are used to verify the MODAS model. MODAS has the capability to provide reasonably good temperature and salinity nowcast fields. The errors have a Gaussian-type distribution with mean temperature nearly zero and mean salinity of −0.2 ppt. The standard deviations of temperature and salinity errors are 0.98°C and 0.22 ppt, respectively. The skill score of the temperature nowcast is positive, except at depth between 1750 and 2250 m. The skill score of the salinity nowcast is less than that of the temperature nowcast, especially at depth between 300 and 400, where the skill score is negative. Thermocline and halocline identified from the MODAS temperature and salinity fields are weaker than those based on SCSMEX data. The maximum discrepancy between the two is in the thermocline and halocline. The thermocline depth estimated from the MODAS temperature field is 10–40 m shallower than that from the SCSMEX data. The vertical temperature gradient across the thermocline computed from the MODAS field is around 0.14°C/m, weaker than that calculated from the SCSMEX data (0.19°–0.27 °C/m). The thermocline thickness computed from the MODAS field has less temporal variation than that calculated from the SCSMEX data (40–100 m). The halocline depth estimated from the MODAS salinity field is always deeper than that from the SCSMEX data. Its thickness computed from the MODAS field varies slowly around 30 m, which is generally thinner than that calculated from the SCSMEX data (28–46 m).  相似文献