西南印度洋洋盆演化和岩浆地球化学印迹

西南印度洋中脊(SWIR)平均扩张速率约为14 mm/yr,是全球洋中脊系统的重要组成端元,因其具有慢速-超慢速扩张特征,引起全球科学家的广泛关注.基于前人对SWIR的综合研究成果,从构造和岩浆作用两个角度出发,系统地回顾了 SWIR的形成和演化历史,探讨了岩浆的分布特征和地幔不均一性成因.SWIR的形成始于冈瓦纳大陆...     

慢速-超慢速扩张洋中脊热液活动及其机理

海底热液系统是地球热量平衡的重要组成,也是地球化学循环和成矿作用发生的主要场所,与洋中脊系统在空间上具有很强的联系。慢速-超慢速扩张洋中脊中确认的活跃热液喷口数量约占全球总数量的三分之一,查明热液发育位置及发育岩性与岩浆-构造活动的耦合关系,对于研究海底热液活动演化过程和海底找矿具有很好的指示意义。本文将全球慢速-超慢速扩张洋中脊中已确认的活跃热液活动进行统计分类,其中受岩浆活动控制的热液活动有29处,而受构造活动控制的热液活动有15处,相对于快速-中速扩张洋中脊显示出较强的构造相关性。研究发现,岩浆作用控制下的热液活动集中在洋中脊轴部中央裂谷内,而构造主控型热液活动常发育在非转换不连续间断和拆离断层系统内。随着大洋核杂岩成熟,热液活动位置向着离轴方向迁移,并且热液类型由高温"黑烟囱"型向低温弥散流型转变。     

贺根山缝合带晚石炭世TTG岩浆事件:奥长花岗岩锆石U-Pb年龄和地球化学制约

本文以贺根山缝合带呼都格奥长花岗岩体为研究对象,通过野外地质调查和岩石学、地球化学、锆石U-Pb年代学研究,讨论岩石成因、构造环境、TTG岩浆事件及古亚洲洋俯冲消亡过程。岩石地球化学研究表明,呼都格岩体富硅(SiO₂=66.27%～71.59%)、高铝(Al₂O₃=15.23%～15.94%)、富钠(Na₂O=4.13%～6.59%)、低钾(K₂O=1.72%～2.53%),相对高锶(Sr=196.60×10^-6～465.40×10^-6)、低钇(Y=5.70×10^-6～12.63×10^-6),富集Ba、Sr等大离子亲石元素和LREE,亏损Nb、Ta、Ti、P等高场强元素和HREE,无明显Eu异常。岩石学和岩石地球化学特征表明,呼都格岩体属于以奥长花岗岩为主的英云闪长岩-奥长花岗岩-花岗闪长岩TTG岩石组合。这套TTG组合除Sr、Mg、Ni和Cr含量相对较低之外,与高Si埃达克岩的地球化学特征...     

基于形态学的海洋锋形态特征提取

根据形态学梯度理论:不同尺寸的结构元素适合不同空间尺度的特征提取,结构元素尺寸的过大或者过小都会达不到最佳的特征边缘提取效果,从结构元素的尺寸δ与海洋锋横断面宽度γ和海流流幅的空间尺度λ的理论关系图推导中,提出δ,γ和λ的最佳定量关系:δ=γ/2,且δ<=λ/2,旨在对海洋锋形态特征进行提取。最后,以黑潮和墨西哥湾流为实验数据,进行海洋锋形态特征的自动提取,实验结果表明该定量关系的正确性和有效性。     

军民结合发展海洋技术

发达海洋国家在发展海洋科技的过程中非常重视军民结合,在实践中取得了非常好的效果。在英、美等国,发展军民两用技术已成为其国家战略。促进军民结合在我国海洋技术领域的应用具有非常重要的意义。     

现场波浪观测技术发展和应用

介绍与海洋工程有关的应用于水下、水面、水上和太空不同空间位置的现场波浪观测技术。根据不同仪器量测的基本原理,分析其对工程应用的适合性和局限性;并讨论了现场波浪观测的发展趋势以及我国应采取的对策。     

条片状绿藻食品制造工艺与设备——绿藻系列食品研究之二

叙述以礁膜、浒苔为原料试制条片状方便食品的工艺及要点。经过除腥、护色、调味、成型、喷油等工序后,制得的产品为墨绿色、条片状、口感香脆、无腥味、耐久藏。介绍了初步设计的洗藻机和压片切条机的结构、洗藻机的作用机理及干燥设备的选型。把压片、切条、烘干三个工序有机地连接在一起,实现了机械化生产。     

A VERTICAL COORDINATE TRANSFORMATION FOR 3-D NUMERICAL MODELLING OF OCEAN CIRCULATION

A so called sine-sigma vertical coordinate transformation is proposed. A vertical implicit scheme is de-rived by using cubic-spline representation of vertical current profiles. The derived 3-D nurmericalmodel has been applied to simulate the water leved field and the vertical structures of wind-induced cur-rents in an enclosed rectangular region, and the tides in the Bohai Sea. The model is believed to besatisfactory after comparing its results with an analytical soclution and observed data from tidal staions.     

SEASONAL HEAT BUDGET IN THE TROPICAL WESTERN PACIFIC OCEAN IN A GLOBAL GCM Ⅱ. IN FIVE SUBREGIONS

The general features of the seasonal suuface heat budget in the tropical western Pacific Ocean,20°S-20°N, western boundary-160°E, were documented by Qu (1995) using a high-resolution generalcirculation model (GCM, Semtner & Chervin,1992) ard existing observations.Close inspection of thesmaller areas, with the whole region further partitioned into six parts, showed different mechanisms balancethe seasonal surface heat budget in different parts of the region The results of study on five subregionsare detailed in this article. In the equatorial (3°S - 3°N) aed North Equatorial Countercurrent(3°N-9°N) region, the surface the flux the does not change significantly throughout the year, so the surface heat content is determined largely by vertical motion near the equator and roughly helf due to horizontal and halfdue to vertical circulation in the region of the North Equatorial Countercurrent(NECC). In the othersubregions (9°N-20°N, 20°S -11°S aed 11°S -3°S ), however, in addition to ocean dynamics     

Seasonal heat budget in the tropical Western Pacific Ocean in a global GCM II. In five subregions

The general features of the seasonal surface heat budget in the tropical western Pacific Ocean, 20° S–20°N, western boundary −160°E, were documented by Qu (1995) using a high-resolution general circulation model (GCM, Semtner & Chervin, 1992) and existing observations. Close inspection of the smaller areas, with the whole region further partitioned into six parts, showed different mechanisms balance the seasonal surface heat budget in different parts of the region. The results of study on five subregions are detailed in this article. In the equatorial (3°S–3°N) and North Equatorial Countercurrent (3°N–9°N) region, the surface heat flux does not change significantly throughout the year, so the surface heat content is determined largely by vertical motion near the equator and roughly half due to horizontal and half due to vertical circulation in the region of the North Equatorial Countercurrent (NECC). In the other subrigions (9°N–20°N, 20°S–11°S and 11°S–3°S), however, in addition to ocean dynamics, surface heat flux can also play a major role in the seasonal variation of sea surface temperature (SST). The remotely forced baroclinic waves and their effect on the surface heat storage in the model are also investigated. Comparison with observations indicates that the model wave activities are reasonably realistic. Contribution No. 2396 from the Institute of Oceanology, Chinese Academy of Sciences. This study was supported by the Australian CSIRO Division of Oceanography and the National Natural Science Foundation of China (No. 49176255)