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1.
本文根据黄、东海现代底地形和地质构造研究新成果，中国新构造分区和地震区带划分结果，认为１９９６年１１月９日发生的引起沪，苏，浙沿海较强有感的６．１级地震，仍应称为９９６年南黄海６．１级地震为宜，该地震在地震区划上归属于下扬子－南黄海地震带。 相似文献
2.
针对南黄海盆地深层地震地质条件差,地震波受屏蔽,能量严重衰减,在海洋反射地震资料中很难识别反映中-古生界的反射地震波组,不能满足南黄海盆地前第三系油气资源前景评价的需要等问题,于2006年5月,开展了南黄海海域海底大地电磁测深试验,在盆地内五莲斜坡和胶州凹陷区布设了3个海底大地电磁测深点,取得了可靠的海底观测数据.本文详细阐述了海底大地电磁测深与常规大地电磁测深在数据处理方法上的差别,论述了海洋电磁噪声对海底大地电磁场观测的影响,提出了海底大地电磁场实测资料“水平姿态”校正、“方位”校正和“海洋电磁噪声”校正的方法.通过对试验观测资料的处理和反演,并结合地质、物性资料进行综合分析,结果表明在南黄海盆地海底以下深部还存留有古生代地层,这对于南黄海前第三系含油气前景的评价具有重要意义.试验结果也证明了海底大地电磁测深技术在研究古生代残留盆地方面的问题可以发挥相当好的作用. 相似文献
3.
根据信息预测理论分析,江苏一南黄海地区M≥6级强震具有显著的可公度性。在回顾总结1996年11月9日南黄海6.1级地震预测的基础上,对南黄海海域1846年以来6级强震可公度性的基本结构及其预测功能进行了深入研究,同时建立了可公度预测模型,对该区未来强震趋势进行预测探讨。结果表明,1999～2000年,该区有可能发生M≥5地震,2002年前后南黄海海域有可能再次发生M≥6级强震。 相似文献
4.
本文分析了宁波ZK－03井1979－1987年的水氡观测资料，发现该井水氡正常动态平稳，但在南黄海6．2级地震，舟山3．9级地震和台湾花莲7．6级地震前均有不同程度的负异常显示，文中还对异常形成和机理作了探讨。 相似文献
5.
门可佩 《地震地磁观测与研究》2001,22(6):38-42
1 江苏—南黄海地区中强震与台湾 7级强震的相关关系江苏—南黄海地区 ( 3 1°～ 3 5.5°N,1 1 8°～ 1 2 4 .5°E)地处扬州—铜陵地震带中东段 ,位于华北地震区与华南地震区的交接部位 ,这里是我国东部地震活动水平较高的地区 ,众所周知 ,太平洋板块、菲律宾板块对欧亚板块的俯冲挤压 ,是我国大陆东部地区地震活动的主要动力源。 1 999年 9月 2 1日台湾 7.6级大震的发生 ,使得本区在 1 994～ 1 997年 4年中强震连发的形势之下又面临一场严峻的考验。表 1 台湾地区 7级强震与江苏—南黄海地区中强震之间相关关系序号台湾地区江苏—南黄海… 相似文献
6.
1991年11月5日在江苏射阳发生了4．7级地震，1992年1月23日在南黄海北部发生了5．3级地震，10月22日射阳东海域发生了4．8级地震，11月4日南黄海北部发生了4．6级地震，对上述4次地震笔者等曾作出了一定程度的年度中期预报。本文对该地震震前的预报概况，预报基本思路和主要科学依据作了概述，并讨论了给予的启示。认为在一定条件下对某些地震作出某种程度的科学预报还是可能的。 相似文献
7.
依据震前资料,对2002年7月23日南黄海北部Ms4．9地震的年度预测过程进行简要回顾,对关键预测依据进行初步讨论。研究结果表明,在南黄海地区,地震活动图像在同一区域的集中演化及3级地震的丛集活动对未来地震发生地点的判别具有指示意义;该区5级以上地震活动时间结构的分析(活跃时段划分及其对比、准周期活动特征等)对年度预测的时间判断起到了关键作用。 相似文献
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9.
据中国地震台网测定，北京时间2006年12月26日20时26分和34分，在南海海域（北纬21．9度，东经120．6度）发生7．2、6．7级地震。震中距大陆最近海岸线约350km，距台湾陆地约15km。厦门市部分地区震感强烈，福建、广东、江西大部分地区有震感。我国广东省和福建省启动了地震应急预案。地震使14条海底通信光缆发生事故，亚洲互联网、通讯受到很大影响。 相似文献
10.
南黄海Ms6.1地震电磁辐射特征 总被引：5，自引：0，他引：5
介绍了长江三角洲观测台网记录到的南黄海６．１级地震电磁辐射异常，并结合１９７９年淋阳Ｍｓ６．０、１９８４年南黄海Ｍｓ６．２地震前的电磁辐射观测资料有为内其它资料，分析了异常的主要特征。初步讨论了ＤＰＪ型电磁辐射观测仪的甚低频低及ＵＬＦ型地震电磁信息观测仪的超低频段天线方向特性对震中预测的意义问题。 相似文献
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12.
分析了天然气水合物分解引起海底斜坡不稳定性的原因,探讨了水合物分解引起沉积物层孔隙压力变化规律.以南海北部神狐海域水合物样品钻获区为研究对象,应用极限平衡法探讨了海底无限斜坡的稳定性问题,计算了设定的不同滑动面的安全系数,建立了目标不稳定区相关参数条件下的水合物分解与海底斜坡不稳定的模式图,模拟计算了不同程度的水合物分解对海底斜坡失稳的影响作用.结果表明：在假设条件下,南海神狐海域当水深为1200 m,沉积物层厚度为200 m,对于20°的较大坡角,沉积物层中5%水合物分解将引起海底斜坡失稳;斜坡坡角为5°时,沉积物层中15%水合物分解后,将会引起海底斜坡失稳;当斜坡坡角为3°或更小时,沉积物层中25%水合物分解后,将会引起海底斜坡失稳. 相似文献
13.
Richard S. Fiske Katharine V. Cashman Atsushi Shibata Kazuki Watanabe 《Bulletin of Volcanology》1998,59(4):262-275
A new and detailed bathymetric map of the Myojinsho shallow submarine volcano provides a framework to interpret the physical
volcanology of its 1952–1953 eruption, especially how the silicic pyroclasts, both primary and reworked, enlarged the volcano
and were dispersed into the surrounding marine environment. Myojinsho, 420 km south of Tokyo along the Izu–Ogasawara arc,
was the site of approximately 1000 phreatomagmatic explosions during the 12.5-month eruption. These explosions shattered growing
dacite domes, producing dense clasts that immediately sank into the sea; minor amounts of pumice floated on the sea surface
after some of these events. The Myojinsho cone has slopes of almost precisely 21° in the depth range 300–700 m.We interpret
this to be the result of angle-of-repose deposition of submarine pyroclastic gravity flows that traveled downslope in all
directions. Many of these gravity flows resulted from explosions and associated dome collapse, but others were likely triggered
by the remobilization of debris temporarily deposited on the summit and steep upper slopes of the cone. Tephra was repeatedly
carried into air in subaerial eruption columns and fell into the sea within 1–2 km of the volcano's summit, entering water
as deep as 400 m. Because the fall velocity of single particles decreased by a factor of ∼30 in passing from air into the
sea, we expect that the upper part of the water column was repeatedly choked with hyperconcentrations of fallout tephra. Gravitational
instabilities within these tephra-choked regions could have formed vertical density currents that descended at velocities
greater than those of the individual particles they contained. Upon reaching the sea floor, many of these currents probably
continued to move downslope along Myojinsho's submarine slopes. Fine tephra was elutriated from the rubbly summit of the volcano
by upwelling plumes of heated seawater that persisted for the entire duration of the eruption. Ocean currents carried this
tephra to distal areas, where it presumably forms a pyroclastic component of deep-sea sediment.
Received: 5 December 1996 / Accepted: 17 September 1997 相似文献
14.
A.L. DeGeest B.L. Mullenbach P. Puig C.A. Nittrouer T.M. Drexler X. Durrieu de Madron D.L. Orange 《Continental Shelf Research》2008
Previous work in the Gulf of Lions (western Mediterranean Sea) has suggested that significant amounts of sediment escape through the western part of this tectonically passive margin, despite it being far removed from the primary sediment source (the Rhone River, ∼160 km to the NE). The primary mechanism behind this export is hypothesized to be the interaction of a regional, southwestward sediment-transport path with a canyon deeply incising the southwestern part of the shelf, Cap de Creus Canyon. 相似文献
15.
Samples collected from the shelf-edge wedge using surface grab samples and the Jago submersible constrain the KwaZulu-Natal shelf-edge wedge to a late Pliocene age on the basis of the absence of Gephyrocapsa oceanica s.l. and Discoaster brouweri, and the presence of Calcidiscus macintyrei. This correlates with proposed Tertiary sea-level curves for southern Africa and indicates relative sea-level fall during the late Pliocene coupled with hinterland uplift. Exposed failure scarps in the upper portions of submarine canyons yield sediment samples of early Pleistocene ages, indicating the uppermost age of deposition of clinoform topsets exposed in the scarp walls. Partially consolidated, interbedded silty and sandy deposits of similar age outcrop in the thalweg of Leven canyon at a depth of 150 m. These sediments provide an upper age limit of the shelf-edge wedge of early Pleistocene, giving a sedimentation rate of this wedge of 162–309 m/Ma. The distribution of widespread basal-most Pleistocene sediments on the upper slope indicates that these sediments escaped major reworking during sea-level falls associated with Pleistocene glaciations and remain as relict upper slope veneers. The absence of more recent sediments suggests that this area has been a zone of sediment bypass or starvation since the early Pleistocene. Areas where younger sediments mantle deposits of early Pleistocene ages represent areas of offshore bedload parting, re-distributing younger Holocene sediment offshore and downslope. 相似文献
16.
该理论模式将湖,海岸坡上的波场冲积场置于波场和重力场的耦合作用中,该区带地貌剖面的坡度和坡形上的响应性变化,使冲积物在其向,离岸振荡运动中形成振距耦合均衡势,与此同时,导致相对稳定的动力地貌均衡剖面的形成。本文提出耦合均衡的含义,条件及其均衡坡度θｅ和坡度梯度的表达式,该理论模式对认识湖,海岸环境中有关岸坡发育问题有一定意义。 相似文献
17.
A hydrodynamic model is employed to derive the magnitude of on-shelf fluxes through a shelf-break canyon for a wide range of canyon sizes and ambient oceanic conditions. Predicted canyon-upwelling fluxes are of the order of 0.05–0.1 Sv (1 Sv=1 million m3/s), being several orders of magnitude greater than upslope fluxes in the bottom Ekman layer on the ambient continental slope. On the basis of ∼150 simulations conducted, a bulk formula of upwelling flux in a submarine canyon is derived. For typical conditions, the upwelling flux varies quadratically with forcing strength (speed of incident flow), linearly with canyon depth, and is inversely proportional to the buoyancy frequency of the density stratification inside the canyon. Other parameters such as density stratification above shelf-break depth and bottom friction are found to have minor influences on the resultant canyon-upwelling flux. 相似文献
18.
The evaluation of the wave-induced excess pore pressure around a buried pipeline is particularly important for pipeline engineers involved in the design of offshore pipelines. Existing models for the wave-induced seabed response around submarine pipeline have been limited to poro-elastic soil behavior and de-coupled oscillatory and residual mechanisms for the rise in excess pore water pressure. To overcome the shortcoming of the existing models, in this study a three-dimensional poro-elasto-plastic soil model with submarine pipeline is established, in which both oscillatory and residual mechanisms can be simulated simultaneously. With the proposed model, a parametric study is conducted to investigate the relative differences of the predictions of the wave-induced pore pressure with poro-elasto-plastic model. Based on numerical examples, it can be concluded that the poro-elasto-plastic behaviors of soil have more significant influence on wave-induced pore pressure of seabed around submarine pipeline. As the seabed depth increases, the normalized pore pressures decrease rapidly at the upper part of seabed, and then change slightly at the lower part of the seabed. Soil permeability and wave period have obvious influence on the wave-induced normalized pore pressure. 相似文献
19.
S. M. Straub 《Bulletin of Volcanology》1995,57(6):403-421
Discrete Quaternary (<400 ka) tephra fallout layers (mostly <1 cm thick) within the siliceous oozes of the central Mariana Trough at 18°N are characterized by medium-K to high-K subalkalic volcanic glasses (K2O=0.8–3.2 wt.%) with high large-ion lithophile elements (LILE)/high-field-strength elements (HFSE) ratios and Nb depletion (Ba/La35; Ba/Zr3.5; La/Nb4) typical for convergent margin volcanic rocks. Compositional zoning within layers ranges from basaltic to dacitic (SiO2=48–71 wt.%; MgO=0.7–6.5 wt.%); all layers contain basaltic andesites. The tephra layers are interpreted as single explosive eruptive events tapping chemically zoned reservoirs, the sources being the Mariana arc volcanoes (MAV) due to their proximity (100–400 km) and similar element ratios (MAV: Ba/La=36±7; Ba/Zr=3.5±0.9). The glasses investigated, however, contrast with the contemporaneous basaltic to dacitic lavas of the MAV by being more enriched in TiO2 (1.2 wt.%; MAV0.8 wt.%), FeO* (10 wt.%, MAV8–9 wt.%), K2O (1.1 wt.%; MAV0.8 wt.%) and P2O5 (0.4 wt.%; MAV0.2 wt.%). (Semi-)Incompatible trace elements (including Rare Earth Elements (REE)) of the basaltic-andesitic and dacitic glasses match those of the dacitic MAV lavas, which became enriched by fractional crystallization. Moreover, the glasses follow a tholeiitic trend of fractionation in contrast to MAV transitional trends and have a characteristic P2O5 trend that reaches a maximum of 0.6 wt.% P2O5 at 57 wt.% SiO2, whereas MAV lavas increase linearly in P2O5 from 0.1 to 0.3 wt.% with increasing silica. Both explosive and effusive series are interpreted to have evolved in common magma reservoirs by convective fractionation. Similar parental magmas are suggested to have separated into coexisting Si-andesitic to dacitic and basaltic melts by in situ crystallization. The differentiated melt is interstitial in an apatite-saturated crystalline mush of plag+px±ox±ol at the cooler chamber margins in contrast to the less differentiated basaltic to basaltic-andesitic magmas, which are not yet saturated in apatite and occupy the chamber interior. Reinjection of interstitial melt into the chamber interior and mixing with larger melt fractions of the interior liquid (mixing ratios about 1: 8–9) can explain the paradoxical behavior of apatite-controlled P and MREE variation in the basaltic andesite glasses and their MAV dacite-like fractionation patterns. The process may also account for the exclusively tholeiitic trend of fractionation of the glass shard series, but in situ crystallization alone cannot cause their absolute enrichment in (semi-)incompatible elements. The newly mixed melt is suggested to form the basaltic end member of the glass shard series. However, it must have become physically separated from the main MAV magma body (possibly by density-driven convective fractionation) in order to allow for further evolution of the contrasting geochemical paths as well as differentiation. 相似文献