基于两种数据集的全球SST变化趋势的对比研究     

郑崇伟  庄卉  李训强  贾本凯 《海洋科学进展》2012,30(2):171-176

分别利用了来自NOAA和Hadley中心的SST(Sea Surface Temperature)资料,分析了全球海域每个网格点上SST的变化趋势,并将两种资料分析的结果进行比较。研究发现:近150a期间,全球大部分海域的SST以0.003℃.a-1左右的速度显著性逐年线性递增,仅在格陵兰南部海域和两极部分海域呈显著的逐年线性递减趋势;NOAA的SST变化趋势的区域性差异比Hadley的SST明显,但后者变化趋势的强度稍大于前者;不同海域SST的逐年变化趋势由不同的季节主导;在1910年为近150a来SST的最低点,之后缓慢上升,在1942年附近达到1个相对高点,而后略有下降,但很快又恢复上升趋势,上升趋势一直延续至今。  相似文献   

南海北部陆缘磁静区及与全球大洋磁静区对比的研究评述   总被引：3，自引：1，他引：2  

高金耀  吴招才  王健  杨春国  张涛 《地球科学进展》2009,24(6):577-588

磁静区与磁异常条带不同,具有宽缓的低幅值磁异常特征,但可能同样包含了从陆壳张裂到海底扩张早期的构造活动和演化信息.为了加深认识南海北部陆缘磁静区,归纳了全球深海和边缘两大类型磁静区的物理、化学及构造三大成因,主要包括大西洋和西太平洋侏罗纪磁静区,以及北太平洋、印度洋和南大洋白垩纪磁静区,强调磁静区与不同程度地幔柱活动、斜交扩张初始产生的小型错断磁源体及隐含弱磁条带关系的重要性.总结了南海北部陆缘磁静区的研究现状,并从区域综合地球物理和地幔热活动作用两方面探讨了南海北部陆缘磁静区的可能成因机制,最后阐述了需要关注的研究重点及其研究意义.  相似文献   

夏季烟台—威海北部近海溶解氧浓度垂向分布的最小值     

孙利元  刘子洲  丁金强  翟方国  顾艳镇 《海洋科学》2021,45(11):20-29

基于2020年夏季的大面航次观测数据,分析了烟台—威海北部海洋牧场及邻近海域海水溶解氧浓度垂向分布最小值（氧最小值层）的空间分布特征,并探讨了影响因素。从6月至8月,海水溶解氧浓度不断减小,垂向结构亦存在显著变化。海水溶解氧浓度垂向分布的最小值主要集中于7月的近岸海域,最小值大致从外海向近岸方向减小,其距离海底高度及与底层溶解氧浓度之差的绝对值均于双岛湾邻近海域为最大。海水溶解氧浓度垂向分布的最小值位于最强密度层结以下。但是海水溶解氧浓度垂向分布最小值的强度向北减小,而密度层结向北增大,两者的空间分布基本相反,说明密度层结抑制垂向湍流扩散可极大减少深层海水溶解氧的来源,是海水溶解氧浓度垂向分布最小值形成的必要条件,但不是主导因素。在海水溶解氧浓度垂向分布的最小值层,表观耗氧量存在垂向分布的最大值,大部分站点的pH存在垂向分布的最小值,说明局地增强、持续的生物地球化学耗氧是控制海水溶解氧浓度垂向分布最小值形成和空间分布的一个重要过程。研究结果表明氧最小值层是夏季烟台—威海北部近岸海水溶解氧垂向结构的典型特征之一。  相似文献   

浪致混合对亚热带冬季海洋混合强度的影响   总被引：1，自引：1，他引：0  

陈思宇  乔方利  黄传江  宋振亚 《海洋学报》2020,42(5):22-30

上层海洋在全球气候系统中起着至关重要的作用。对上层海洋层结及混合的模拟偏差一直是海洋和气候数值模式发展中悬而未决的问题。本文首先评估了CMIP5中45个模式对上层海洋层结模拟的偏差,确认了冬季亚热带地区海洋模式垂向混合偏强。随后,基于自然资源部第一海洋研究所地球系统模式(FIO-ESM v1.0),分别开展了1986?2005年期间包含和关闭海浪垂向混合情况下的数值实验,分析浪致混合对亚热带冬季海洋混合强度模拟的影响及机制。发现浪致混合使得气候模式中亚热带海域冬季的海洋层结增强,增强的层结使上层海洋更加稳定。首次揭示了增加浪致混合反而降低了海洋总体的垂向混合率:浪致混合使北半球冬季亚热带海域混合率从无浪实验的227 cm2/s降低到有浪实验的178 cm2/s,降低了21.6%;南半球冬季亚热带海域混合率从无浪实验的189 cm2/s降低到有浪实验的165 cm2/s,降低了12.7%。进一步分析发现,浪致混合主要是通过增加冬季亚热带海域上层海洋的热含量从而强化了海洋的层结,最终改善了气候模式对上层海洋混合的模拟。  相似文献   

On the relationship between convection intensity of South China Sea summer monsoon and air-sea temperature difference in the tropical oceans     

LIN Ailan  LIANG Jianyin  GU Dejun  WANG Dongxiao 《海洋学报(英文版)》2004,23(3)

The annual, interannual and inter-decadal variability of convection intensity of South China Sea (SCS) summer monsoon and air-sea temperature difference in the tropical ocean is analyzed, and their relationship is discussed using two data sets of 48-a SODA (simple ocean data assimilation) and NCEP/NCAR. Analyses show that in wintertime Indian Ocean (WIO), springtime central tropical Pacific (SCTP) and summertime South China Sea-West Pacific (SSCSWP), air-sea temperature difference is significantly associated with the convection intensity of South China Sea summer monsoon. Correlation of the inter-decadal time scale (above 10 a) is higher and more stable. There is interdecadal variability of correlation in scales less than 10 a and it is related with the air-sea temperature difference itself for corresponding waters. The inter-decadal variability of the convection intensity during the South China Sea summer monsoon is closely related to the inter-decadal variability of the general circulation of the atmosphere. Since the late period of the 1970s, in the lower troposphere, the cross-equatorial flow from the Southern Hemisphere has intensified. At the upper troposphere layer, the South Asian high and cross-equatorial flow from the Northern Hemisphere has intensified at the same time. Then the monsoon cell has also strengthened and resulted in the reinforcing of the convection of South China Sea summer monsoon.  相似文献   

全球海洋中Argo剖面浮标运行状况分析   总被引：4，自引：0，他引：4  

孙朝辉  刘增宏  朱伯康  许建平 《海洋技术学报》2006,25(3):127-134

A rgo剖面浮标是A rgo全球海洋实时观测网建设中的主要观测设备。自2001年国际A rgo计划组织实施以来,世界上已经有22个国家和团体在全球海洋中陆续布放了3 000多个A rgo剖面浮标,它们的寿命和运行状况一直是人们重视和关心的问题,因为这关系到何时能够实现国际A rgo计划的最终目标,更重要的是,涉及到浮标的性能、资料的可靠性。文中就这些问题进行了探讨,希望能有助于关注者对A rgo全球海洋实时观测网的建设及运行情况有一比较全面的了解。  相似文献   

Mapping of an approximate neutral density surface with Ungridded data     

YOU Yuzhu 《中国海洋大学学报(英文版)》2008,7(1):1-9

A neutral density surface is a logical study frame for water-mass mixing since water parcels spread along such a surface without doing work against buoyancy restoring force. Mesoscale eddies are believed to stir and subsequently mix predominantly along such surfaces. Because of the nonlinear nature of the equation of state of seawater, the process of accurately mapping a neutral density surface necessarily involves lateral computation from one conductivity, temperature and depth （CTD） cast to the next in a logical sequence. By contrast, the depth of a potential density surface on any CTD cast is found solely from the data on this cast. The lateral calculation procedure causes a significant inconvenience. In a previous paper by present author published in this journal （You, 2006）, the mapping of neutral density surfaces with regularly gridded data such as Levitus data has been introduced. In this note, I present a new method to find the depth of a neutral density surface from a cast without having to specify an integration path in space. An appropriate reference point is required that is on the neutral density surface and thereafter the neutral density surface can be determined by using the CTD casts in any order. This method is only approximate and the likely errors can be estimated by plotting a scatter diagram of all the pressures and potential temperatures on the neutral density surfaces. The method assumes that the variations of potential temperature and pressure （with respect to the values at the reference point） on the neutral density surface are proportional It is important to select the most appropriate reference point in order to approximately satisfy this assumption, and in practice this is found by inspecting the θ-p plot of data on the surface. This may require that the algorithm be used twice. When the straight lines on the θ-p plot, drawn from the reference point to other points on the neutral density surface, enclose an area that is external to the cluster of θ-p points of the neutral density surface, errors will occur, and these errors can be quantified from this diagram. Examples showing the use of the method are presented for each of the world＇s main oceans.  相似文献   

对西北太平洋海域表层密度流的初步探索   总被引：3，自引：0，他引：3  

梁振英  李明  牟秀珍 《测绘学报》1998,27(1):24-30

在文［９］［１０］关于西北太平洋海面动力地形研究的基础上,本文对该海域表层密度流进行了初步探索。特别是用０．５°×０．５°方区多年船测资料,对西部边界流——黑潮进行了专门研究。结果表明,该海域表面密度流模式与主要由风驱动的大洋总的环流模式基本一致。据研究结果,对文［９］给出的海面动力地形和全球海面动力地形的某些特征作出了解释。另外,还就卫星测高在确定大洋环流的局限性和若干概念性问题提出了明确的看法。  相似文献   

Seas under ice: Stability of liquid-water oceans within icy worlds     

Javier Ruiz  Alberto G. Fairén 《Earth, Moon, and Planets》2005,97(1-2):79-90

The present-day existence of internal oceans under the outer ice shell of several icy satellites of the Solar System has been recently proposed. The presence of antifreeze substances decreasing ice’s melting point (and tidal heating in Europa’s case) has been generally believed to allow the stability of such oceans; limited cooling of the water (ice plus liquid) layer, due to stability against convection or to stagnant lid convection in the icy shell, have been also considered. Here we propose that even pure liquid-water oceans could survive today within several icy worlds, and we consider some factors affecting thermal modeling in these bodies. So, the existence of such oceans would be a natural consequence of the physical properties of water ice, independently from the addition of antifreeze substances or any other special conditions. The inclusion of these substances would contribute to expand the conditions for water to stay liquid and to increase ocean’s volume.  相似文献   

Consistent atmospheric and oceanic excitation of the Earth's free polar motion     

Florian Seitz  Jochen Stuck  Maik Thomas 《Geophysical Journal International》2004,157(1):25-35

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