西非被动大陆边缘重力滑脱构造体系下的塑性构造

论述了西非被动大陆边缘深水环境下的重力滑脱构造体系中的塑性构造。研究发现塑性地层在整个西非被动大陆边缘都有分布,且盐岩塑性层主要分布在西非被动大陆边缘的西南部和西北部,发育层位为过渡期(J-K)构造层之内;中部尼日尔三角洲等塑性层主要为泥岩塑性层,发育层位为古近系和新近系。根据重力滑脱构造体系发育特征可划分为:以正断裂和塑性焊接构造为主的上部重力滑脱伸展构造、以底辟构造为主的中部重力滑脱底辟构造、以冲断裂、塑性褶皱和塑性冲断构造为主的下部重力滑脱冲断构造。根据塑性构造上覆地层的变形过程,塑性构造演化主要经历了后生变形期和同生变形期。塑性构造变形机制主要受基底掀斜作用和上覆地层的沉积速率控制。塑性构造中的底辟、褶皱、冲断及塑性焊接构造对油气成藏的控制作用依次减弱。     

基于FVCOM的泉州湾海域三维潮汐与潮流数值模拟

基于FVCOM海洋数值模式,采用非结构的三角形网格和有限体积法,建立了泉州湾海域高分辨率(26 m)的三维潮汐、潮流数值模型。模拟结果同2个验潮站和3个连续测流站的观测资料符合良好,较好地反映了泉州湾内潮汐、潮流运动的变化状况和分布特征,给出了M₂、S₂、K₁、O₁ 4个主要分潮的同潮图、表层潮流椭圆分布,以及模拟区域内最大可能潮差、表层最大可能潮流流速和潮余流分布。分析表明,4个分潮的最大潮汐振幅和迟角差分别为219 cm和19°,85 cm和25°,26 cm和12°,26 cm和9°;石湖港以东海域的潮波为逆时针旋转的驻波,以西海域为前进波;最大可能潮差由湾口的8.0m向湾内增加至8.8 m。湾内潮流类型为规则半日潮流,落潮最大流速大于涨潮最大流速,北乌礁水道为强流区,表层最大可能潮流流速为2.4 m/s;湾口潮流运动以逆时针方向的旋转流形式为主,湾内的潮流运动以往复流形式为主,长轴走向主要沿着水道方向,与等深线和海岸线平行;四个分潮流表层最大流速分别为1.4 m/s,0.58 m/s,0.12 m/s,0.10 m/s。余流流速大小与潮流强弱有密切的联系,表、中、底层最大余流流速分别为26 cm/s,20 cm/s,16 cm/s,三者在水平方向基本呈北进南出的分布形态。     

1013号台风“鲇鱼”风暴潮特点分析

1013号超强台风“鲇鱼”在福建漳浦县登陆.登陆时逢农历九月十六的天文高潮,给闽南沿海地区造成了较大的灾害.本文从台风路径特点及灾害、天气形势、与历史相似台风(9914号)对比、数值模拟等方面对此次台风引起的风暴潮过程进行分析得出:进行历史台风相似分析时,除了台风本身路径、强度、移速等参数之外,还要注意分析台风的季节时间,天气形势,登陆地点,这些都会造成台风增水的明显不同;台风登陆后,受地形和降水影响,有时增水也会持续增大几小时.     

First six months quality assessment of HY-2A SCAT wind products using in situ measurements

The first Chinese microwave ocean environment satellite HY-2A, carrying a Ku-band scatteromenter （SCAT）, was successfully launched in August 2011. The first quality assessment of HY-2A SCAT wind products is presented through the comparison of the first 6 months operationally released SCAT products with in situ data. The in situ winds from the National Data Buoy Center （NDBC） buoys, R/V Polarstern, Aurora Australis, Roger Revelle and PY30-1 oil platform, were converted to the 10 m equivalent neutral winds. The temporal and spatial differences between the HY-2A SCAT and the in situ observations were limited to less than 5 min and 12.5 km. For HY-2A SCAT wind speed products, the comparison and analysis using the NDBC buoys yield a bias of-0.49 m/s, a root mean square error （RMSE） of 1.3 m/s and an increase negative bias with increasing wind speed observation above 3 m/s. Although less accurate of HY-2A SCAT wind direction at low winds, the RMSE of 19.19° with a bias of 0.92° is found for wind speeds higher than 3 m/s. These results are found consistent with those from R/Vs and oil platform comparisons. Moreover, the NDBC buoy comparison results also suggest that the accuracy of HY-2A SCAT winds is consistent over the first half year of 2012. The encouraging assessment results over the first 6 months show that wind products from HY-2A SCAT will be useful for scientific community.     

Distribution of large-scale detachment faults on mid-ocean ridges in relation to spreading rates

Large-scale detachment faults on mid-ocean ridges （MORs） provide a window into the deeper earth. They have megamullion on their corrugated surfaces, with exposed lower crustal and upper mantle rocks, rela- tively high residual Bouguer gravity anomaly and P-wave velocity, and are commonly associated with ocean- ic core complex. According to 30 detachment faults identified on MORs, we found that their distances to the axis mostly range from 5 to 50 km, half-spreading rates range from 6.8 to 17 mm/a, and activity time ranges from recent to 3 Ma. Most of the detachment faults are developed on the slow spreading Mid-Atlantic Ridge （MAR） and ultra-slow spreading Southwest Indian Ridge （SWIRl, with the dominant half-spreading rates of 7-13 mm/a, especially 10-13 mm/a. Furthermore, they mostly occur at the inside corner of one segment end and result in an asymmetric seafloor spreading. The detachment faults on MORs are mainly controlled by the tectonism and influenced by the magmatism. Long-lived detachment faults tend to be formed where the ridge magma supply is at a moderate level, although the tectonism is a first-order controlling factor. At the slow spreading ridges, detachment faults tend to occur where local magma supply is relatively low, whilst at the ultra-slow spreading ridges, they normally occur where local magma supply is relatively high. These faults are accompanied by hydrothermal activities, with their relationships being useful in the study of hydrothermal polymetallic sulfides and their origin.     

南太平洋所罗门群岛海域黄鳍金枪鱼繁殖生物学研究

根据2012年9~12月所罗门群岛海域采集的353尾黄鳍金枪鱼Thunnus albacares样本,分析渔获物个体组成、性别比例、性成熟率和性腺指数等繁殖生物学参数。结果表明,捕获个体中包含大小两个群体;雌性群体个体规格明显小于雄性(p0.001)。春夏季9~12月雌、雄总体性别比为0.67︰1,显著偏离1︰1(p0.01);但性别比例与调查月份和个体大小密切相关,从9月到12月逐渐接近,至12月达到1︰1(p0.05)。性别比例随叉长增长逐步降低,叉长大于110cm个体中以雄性为主(p0.05),雌性比例与叉长呈现线性负相关关系,相关系数为-0.90,(p0.01)。雌、雄个体性成熟率和性腺指数在春末夏初间逐步增长,至11~12月达到最高;Ⅴ~Ⅵ期产卵个体比例增加,这表明所罗门群岛海域黄鳍金枪鱼春夏季存在产卵群体,从10月开始出现产卵个体,调查期间12月产卵个体比例达到相对最高,并且性腺指数与叉长呈现正相关关系;更一步的分析表明,雌、雄个体初次性成熟叉长分别为97.4cm和103.7cm。对该海域黄鳍金枪鱼繁殖生物学的研究有助于了解该种群资源状况,对渔业资源评估具有重要意义。     

三疣梭子蟹HMGR基因的克隆及其在蜕皮中的表达分析

为了研究3-羟基-3-甲基戊二酰辅酶A还原酶(3-hydroxy-3-methyl glutaryl coenzyme A reductase,HMGR)在甲壳动物蜕皮调控中的作用,采用RT-PCR和c DNA末端快速扩增技术(RACE),克隆得到三疣梭子蟹(Portunus trituberculatus)HMGR基因的c DNA序列(Gen Bank登录号:KF280756)。该序列全长2575bp,包括一个53bp的5′端非编码区,一个686bp的3′端非编码区和一个长度为1836bp的开放阅读框,编码611个氨基酸。该氨基酸序列与已公布的美洲海鳌虾HMGR氨基酸序列相比一致性达65%,具有Ⅰ型HMGR保守催化区域、两个HMG-Co A结合基序和两个NADP(H)结合基序。采用实时荧光定量PCR(q RT-PCR)技术,分析三疣梭子蟹HMGR基因的组织差异表达及在蜕皮周期中的表达水平变化,结果表明HMGR基因在三疣梭子蟹大颚器(MO)中的表达量最高,在其它组织中表达量均极低;在三疣梭子蟹蜕皮周期中,大颚器中HMGR基因的表达量自A期至D0亚期升至最高,然后下降,至D4亚期最低。验证了大颚器是三疣梭子蟹合成甲基法尼酯的唯一器官,表明HMGR在三疣梭子蟹蜕皮调控中起着重要作用。     

基于破碎临界区的新型拍岸浪统计计算模型研究

When waves propagate from deep water to shallow water, wave heights and steepness increase and then waves roll back and break. This phenomenon is called surf. Currently, the present statistical calcula...     

2008年中国沿岸冬季寒潮激发陆架波的小波分析

This study applies the wavelet analysis to the tidal gauge records, alongshore winds, atmospheric temperature and pressure along the China coast in winter 2008. The analysis results show three events of sea level oscillations(SLOs) on the shelf induced by winter storms. The first event occurred from January 9 to 21. The SLO periods were double-peaked at 1.6–5.3 and 7.0–16.0 d with the power densities of 0.04–0.05 and 0.10–0.15 m2·d, respectively.The second event occurred from February 5 to 18. The SLO period was single-peaked at 2.3–3.5 d with power density of 0.03–0.04 m2·d. The third event occurred from February 20 to March 8. The SLO periods were doublepeaked at 1.5–4.3 and 6.1–8.2 d with the power densities of 0.08–0.11 and 0.02–0.08 m2·d, respectively. The SLOs propagated along the coast from Zhejiang in north to Guangdong in south. The phase speeds ranged about 9–29m/s from Kanmen to Pingtan, 5–11 m/s from Xiamen to Huizhou and 11–22 m/s from Huizhou to Shuidong. The dispersion relation of the SLOs shows their nature of coastal-trapped wave.