世界大洋表层水中的210Pb

本工作获得了西太平洋,东印度洋和南大西洋15个站位表层水中的溶解态210Pb和颗粒态210Pb的浓度.溶解态210Pb的浓度范围为西太平洋0.71～3.80Bq/m3;东印度洋0.42～2.15Bq/m3;南大西洋0.97～1.78Bq/m3.210Pb最大值3.80Bq/m3是在27°18′N,125°40′E(北太平洋)测得的,而最小值0.42Bq/m3是在远离澳大利亚西岸的25°18′S,111°38′E(东印度洋)测得的.在26°56′S,166°07′E(南太平洋)观测到颗粒态210Pb浓度的最大值0.35Bq/m3,而在东南印度洋颗粒态210Pb的浓度都小于0.03Bq/m3.表层水中溶解态210Pb含量一般呈现出地理性变化,其随纬度的变化与文献报道的结果很相符.     

东海黑潮区海水中磷酸盐的分布特征及成因探讨

本文报道了1987年夏、冬两个航次在26°50′～32°30′N,124°30′～131°30′E海区中可溶性无机磷酸盐的调查结果,阐明了磷的分布特征和形成机制。结果表明陆架区表层测值较高,大洋区为低值区,底层则相反。大洋水常年分层,中层水有爬坡涌升现象,其浓度与Aou呈正相关,与pH和S呈负相关。夏、冬两季底层磷与Aou呈正相关,其浓度变化主要依赖于生物过程。     

昌黎黄金海岩国家级自然保护区

昌黎黄金海岩国家级自然保护区吕彩霞昌黎黄金海岩国家级自然保护区位于东经１１９°１１′～１１９°３７′，北纬３９°２７′～３９°４１′，坐落在河北昌黎县东部，面积约３００平方公里。该保护区是国务院批准由国家海洋局负责管理的第一批国家级海洋类型自然保护区...     

A study of ecology of Chaetognaths in the Western Taiwan Strait

This study is based on 172 planktonic samples collected by vertical hauls of planktonic net from the bottom to the surface in the Western Taiwan Strait (116°40′～120°30′E, 22°22′. 9～26°43′N) in four seasonal months from May 1984 to February 1985.     

The distribution of Euphausiacea in the western Taiwan Strait

The present paper reports the species composition and quantitative distribution of the Euphausiacea. The materials for study were taken from the western Taiwan Strait (22°22. 9′～25°43. 0′ N;116°40.0′～120°30.0′E) by the Third Institute of Oceanography, State Oceanic Administration during the investigations in May, August, November, 1984 and February, 1985.     

利用卫星测高资料确定全球海洋重力场

详细描述了卫星测高数据的平滑处理、高斯低通滤波、交叉点剩余垂线偏差计算、网格化方法以及根据逆的威宁·曼尼兹公式利用 1DFFT技术反演海域重力异常的解算过程 ,介绍一种确定正常轨道地面轨迹交叉点位置的简便方法 ,导出了海面地形对垂线偏差影响的改正公式以及剩余网格垂线偏差模型值的计算公式。所确定的全球 82°S～ 82°N ,0°～ 36 0°海域 30′× 30′网格平均重力异常与船测平均重力异常比较表明 ,精度达到± 4 .1～± 4 .7毫伽。     

中国海洋渔业资源(四)

Ⅱ.3. 带鱼种群特征和种群数量变动规律 著者根据已经公开发表过的生态习性和形态特征等资料分析,认为带鱼种群有:1.南海种群;2.东海种群;3.黄渤海种群等3个种群。 Ⅱ.3.1.种群特征 A.越冬场的分布 秋末冬初,南海种群带鱼移动到水深60～150m一带的深水区,如粤西深水区(19°30′～21°00′N,111 °30′～113°00′E)     

得天独厚的舟山群岛

舟山群岛位于长江口东南、杭州湾以东的浙江北部沿海,介于北纬29°32′～31°04′,东经121°30′～123°25′之间,由1339个岛屿、3550个岩礁组成,陆地面积1241平方公里,是我国最大的群岛,其中舟山岛面积502平方公里,是我国第四大岛。较大的岛屿集中在西南部,其余岛屿按分布、排列状况,自北至南又分     

简讯

海峡两岸合作勘探南海油气 中国海洋石油总公司与我国台湾“中油公司”签订的“台南盆地与潮汕凹陷部分海域协议区物探协议”于1998年4月16日正式批准生效,5月1日开始执行。 该协议是海峡两岸两大石油公司根据经济上平等互利原则签订的第一个合作协议。“物探协议区”位于116°30′E～118°30′E、20°55′N～22°50′N范围内的南海珠江口海域,毗邻台湾海峡位于台湾省高雄市以西250公里和广东省     

胶州湾

胶州湾在黄海中部西北岸。固古时属胶州,故得名。胶州湾地处北纬35°58′～36°18′,东经120°04′～120°23′。古时曹称动海、少海、南海,《明史》中称麻湾。胶州湾湾口向东,南起海西半岛北端脚子石嘴,北至青岛港南岸的团岛嘴,岸线曲抑,长163公里,口宽3公里;湾内东西宽约28公里,南北长约     

东海地区地热场综述

综述了东海地区地热场的特征及研究进展,根据收集的各航次热流值资料,绘制了东海地区的热流值分布图,并根据热流值的分布特点将东海地区分为陆架区、冲绳海槽区、琉球岛弧和海沟区、菲律宾海盆区等4个区块,详细分析了它们的热流分布成因,在已有的东海南北热结构模型基础上对东海南北热结构差异进行了分析。南冲绳海槽区的地壳热流值和地壳减薄程度都明显高于北冲绳海槽及其它各区,说明高热流值起源于地幔抬升和地壳的减薄,东海的扩张已经从冲绳海槽北部转移到南部。     

南海中央海盆热流特征及成因

对南海中央海盆70个热流观测值的统计结果表明,南海中央海盆属于高热流区,热流平均值可达89.9mW/m2。其中西南次海盆热流平均值为96.6mW/m2,东部次海盆热流平均值为86mW/m2,西南次海盆比东部次海盆更＂热＂。高热流值的主要原因是岩石圈的构造拉张减薄以及壳内高导层埋深较浅。而局部存在的热流高值异常其根本原因是断裂和岩浆活动的结果。通过对研究区热流分布以及高值特征的分析,不仅可以对洋壳年龄和扩张年代进行估算,还可以对构造特征以及沉积环境进行有效推测。     

The Crustal Structure Character of East China Sea

This paper presents actuality of investigation and study of the crustal structure characters of East China Sea at home and abroad. Based on lots of investigation and study achievements and the difference of the crustal velocity structure from west to east, the East China Sea is divided into three parts - East China Sea shelf zone, Okinawa Trough zone and Ryukyu arc-trench zone. The East China Sea shelf zone mostly has three velocity layers, i.e., the sediment blanket layer （the velocity is 5.8-5.9 km/s）, the basement layer （the velocity is 6.0-6.3 km/s）, and the lower crustal layer （the velocity is 6.8-7.6 km/s）. So the East China Sea shelf zone belongs to the typical continental crust. The Okinawa Trough zone is located at the transitional belt between the continental crust and the oceanic crust. It still has the structural characters of the continental crust, and no formation of the oceanic crust, but the crust of the central trough has become to thinning down. The Ryukyu arc-trench zone belongs to the transitional type crust as a whole, but the ocean side of the trench already belongs to the oceanic crust. And the northwest Philippine Basin to the east of the Ryukyu Trench absolutely belongs to the typical oceanic crust.     

南海北部陆缘地热状态及其成因探讨

对收集、整理的462组大地热流和地温梯度数据进行统计分析,结果表明南海北部陆缘具有普遍偏高的大地热流和地温梯度,大地热流总体表现为由陆架向洋盆方向递增的趋势。海底热流资料经稳态温度场计算南海北部随深度变化的热流和温度分布,获取热居里面深度,与地磁资料反演的居里面深度进行对比,发现南海北部中、下陆坡磁居里面深度浅于热居里面深度,处于地热不平衡状态。通过对地壳结构、拉张因子、莫霍面埋深、断裂带及火山活动的综合分析,表明南海北部陆缘地热状态受控于地壳拉张减薄和莫霍面抬升的构造格局,裂后晚期局部岩浆活动对地热状态亦有影响。     

南海北部地球物理特征及地壳结构

为了研究南海地壳结构，中国和日本合作在南海北部首次进行了以炸药为震源的综合地球物理调查。经初步分析其地壳结构主要特征为：南海北部地壳分为沉积层、上地壳层、中地壳层及下地壳层。大陆架及上陆坡地壳厚度大、稳定。下陆坡地壳厚度除中地壳外，其他壳层厚度减薄且不稳定。深海盆地壳分３层，厚度虽薄但相对稳定，其底部缺失７．３ｋｍ·ｓ－１的高速层。测区内地壳总厚度：陆壳２６—３０ｋｍ，过渡壳１３—２２ｋｍ，洋壳为８ｋｍ。     

“Uniform geothermal gradient” and heat flow in the Qiongdongnan and Pearl River Mouth Basins of the South China Sea

The Pearl River Mouth Basin (PRMB) and Qiongdongnan Basin (QDNB) are oil and gas bearing basins in the northern margin of the South China Sea (SCS). Geothermal survey is an important tool in petroleum exploration. A large data set comprised of 199 thermal conductivities, 40 radioactive heat productions, 543 measured geothermal gradient values, and 224 heat flow values has been obtained from the two basins. However, the measured geothermal gradient data originated from diverse depth range make spatial comparison a challenging task. Taking into account the variation of conductivity and heat production of rocks, we use a “uniform geothermal gradient” to characterize the geothermal gradient distribution of the PRMB and QDNB. Results show that, in the depth interval of 0–5 km, the “uniform geothermal gradient” in the PRMB varies from 17.8 °C/km to 50.2 °C/km, with an average of 32.1 ± 6.0 °C/km. In comparison, the QDNB has an average “uniform geothermal gradient” of 31.9 ± 5.6 °C/km and a range between 19.7 °C/km and 39.5 °C/km. Heat flows in the PRMB and QDNB are 71.3 ± 13.5 mW/m² and 72.9 ± 14.2 mW/m², respectively. The heat flow and geothermal gradient of the PRMB and QDNB tend to increase from the continental shelf to continental slope owing to the lithosphereic/crustal thinning in the Cenozoic.     

南海热流特征及其构造意义

根据南海 592个热流数据 ,为克服热流站位分布不均及局部异常热流的影响 ,结合各单元的地质史及其地壳厚度等资料对研究区热流特征进行了详细分析。结果表明 ,具拉张背景的区域如北部陆缘、湄公盆地以及北巴拉望盆地具有中等偏高热流 ;海沟区热流相对较低 ,东部海沟区除台西南盆地外均为低热流区 ,而南部边缘东段古海沟区处于热恢复中 ;南部边缘西区因边界断裂的扭张及深部热源的异常补给而具高热流 ;属于剪切断裂带的西部陆缘也具高热流特征 ;中沙—西沙地区热流中等偏高 ,并由NW往SE方向增加 ,而南沙地区热流较低 ,约为 60mW·m- 2 ;海盆的热流基本满足随洋壳年龄增加而降低的规律 ,东部次海盆实测热流与理论预测基本一致 ,而西南次海盆实测热流普遍低于预测值 ;在南海北部下陆坡区识别出一条高热流带 ,该带与前人给出的海盆北缘断裂带位置基本一致。研究区不同区域地热特征直接或间接地受控于其所处的构造环境。据此 ,给出了研究区的热流趋势图。     

New heat flow measurements in the Ulleung Basin, East Sea (Sea of Japan): relationship to local BSR depth, and implications for regional heat flow distribution

In July 2007, new marine heat flow data were collected at ten sites (HF01–10) in the central and southwestern sectors of the Ulleung Basin (East Sea or Sea of Japan) as part of regional gas hydrate research. In addition, cores were collected at five of these sites for laboratory analysis. The results show that the geothermal gradient ranged from 103–137 mK/m, and the in-situ thermal conductivity from 0.82–0.95 W/m·K. Laboratory measurements of thermal conductivity were found to deviate by as much as 40% from the in-situ measurements, despite the precautions taken to preserve the cores. Based on the in-situ conductivity, the heat flow was found to increase with water depth toward the center of the basin, ranging from 84–130 mW/m². Using a simple model, we estimated the heat flow from the depths of the BSR, and compared this with the observed heat flow. In our study area, the two sets of values were quite consistent, the observed heat flows being slightly higher than the BSR-derived ones. The evaluation of regional pre-1994 data revealed that the heat flow varied widely from 51–157 mW/m² in and around the basin. Due to a large scatter in these older data, a clear relationship between heat flow and water depth was not evident, in contrast to what would be expected for a rifted sedimentary basin. This raises the question as to whether the pre-1994 data represent the true background heat flow from the underlying basin crust since the basin opening, and/or whether they contain large measurement errors. In fact, evidence in support of the latter explanation exists. BSRs are generally found in the deep parts of the basin, and vary by only ±15 m in depth below the seafloor. From the average BSR depth, we inferred the background heat flow using a simple model, which in the case of the Ulleung Basin is approximately 120 and 80 mW/m² for 2.5 and 1 km below sea level, respectively.     

东海及其邻域地球动力学研究进展

分别对东海陆架盆地和冲绳槽盆地的地质概况,地壳结构、地热场分布及热水活动状况,地震层析成像及其它地球动力学研究做了综合分析,研究结果偏重于大陆地壳下的物质向边缘海方向扩张,形成边缘海和边缘洋盆的模式,从而取代多年来关于西北太平洋边缘海盆是由于海沟向欧亚大陆的俯冲产生的观点。     

Seismic study of the Ulleung Basin crust and its implications for the opening of the East Sea (Japan Sea)

The Ulleung Basin (Tsushima Basin) in the southwestern East Sea (Japan Sea) is floored by a crust whose affinity is not known whether oceanic or thinned continental. This ambiguity resulted in unconstrained mechanisms of basin evolution. The present work attempts to define the nature of the crust of the Ulleung Basin and its tectonic evolution using seismic wide-angle reflection and refraction data recorded on ocean bottom seismometers (OBSs). Although the thickness of (10 km) of the crust is greater than typical oceanic crust, tau-p analysis of OBS data and forward modeling by 2-D ray tracing suggest that it is oceanic in character: (1) the crust consists of laterally consistent upper and lower layers that are typical of oceanic layers 2 and 3 in seismic velocity and gradient distribution and (2) layer 2C, the transition between layer 2 and layer 3 in oceanic crust, is manifested by a continuous velocity increase from 5.7 to 6.3 km/s over the thickness interval of about 1 km between the upper and lower layers. Therefore it is not likely that the Ulleung Basin was formed by the crustal extension of the southwestern Japan Arc where crustal structure is typically continental. Instead, the thickness of the crust and its velocity structure suggest that the Ulleung Basin was formed by seafloor spreading in a region of hotter than normal mantle surrounding a distant mantle plume, not directly above the core of the plume. It seems that the mantle plume was located in northeast China. This suggestion is consistent with geochemical data that indicate the influence of a mantle plume on the production of volcanic rocks in and around the Ulleung Basin. Thus we propose that the opening models of the southwestern East Sea should incorporate seafloor spreading and the influence of a mantle plume rather than the extension of the crust of the Japan Arc.