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以高精度三维地震资料为基础,系统研究了下刚果盆地深海麻坑的形态特征及其与盐构造活动的关系。研究发现,该区海底麻坑几何形态主要有平面上圆形、剖面上深V型和平面上条形、剖面浅U型两大类,并分别分布于由浅水到深水的东西两个不同区带。进一步分析认为,该区麻坑的发育、分布与下部盐岩构造活动有密切关系,东部盐岩底辟构造带上发育由压扭应力作用下的海底地层挤压破裂并诱发流体高压喷射而形成的深V型麻坑,西部盐岩挤压逆冲构造带上发育由拉张应力作用下的沿盐岩体边界上海底地层拉张破裂而形成的U型麻坑。该区产生麻坑的海底地层破裂和流体高压均由下部盐岩构造活动所控制。 相似文献
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北部湾广西沿岸全新世海侵过程的区域差异 总被引：2，自引：0，他引：2
通过分析北部湾广西沿岸3个地质钻孔的岩性、地球化学和有孔虫含量特征,确定了其沉积相序,在统一的高程坐标内,对各钻地层中沉积相的高程和年代进行了对比,分析了该区全新世以来海侵过程的区域差异;并以东亚全新世海平面波动曲线作为参照,估算了广西沿岸各主要海湾的构造沉降速度。研究表明:全新世以来,广西沿岸的海侵开始时间并不一致,这是由于各海湾构造沉降运动的区域差异造成的,东部的廉州湾构造基本稳定,而廉州湾以西则经历了较大幅度的构造沉降。构造沉降又导致了海平面波动过程的区域差异,进而影响到了地层形成,如海陆过度相沉积只发育于廉州湾以西遭受海侵时间较晚、相对海平面上升速度较低的区域。 相似文献
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大量研究表明南海北部珠江口盆地是天然气水合物发育区,但是该盆地东部揭阳凹陷水合物研究较少。本文利用揭阳凹陷新采集三维地震资料,对该三维地震资料进行成像道集优化和叠前时间偏移处理,得到针对水合物的新处理地震数据体,并通过高精度网格层析反演得到层速度数据体。利用该数据开展叠后约束稀疏脉冲反演,获得含天然气水合物地层波阻抗异常,综合分析反演与地震属性识别水合物。从新处理地震资料看,该区域似海底反射(bottom simulation reflection,BSR)反射呈连续、不连续与地层斜交等特征,BSR发育在一个继承性小型水道上,且下部断裂和气烟囱发育。通过分析BSR特征及BSR上下地层的速度、波阻抗、振幅、频率、相干等属性异常,结合水合物成藏条件,发现了南海北部新的天然气水合物有利富集区,为该区域水合物勘探提供基础。 相似文献
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利用近年来在山东半岛南部近海采集的浅地层剖面、单道地震等资料,进行精细处理与解释,结合前人的研究成果,系统地揭示了研究区内自新近系以来沉积层序。结果表明:研究区主要处在千里岩隆起背景上,第四系和新近系直接覆盖于印支期变质岩系上,由于新近系底界面为向东南缓倾的构造形态,故新近纪以来的海侵层不断向西北超覆,各期地层在厚度图上均表现为北西薄、南东厚的楔形体;全新统地层全区均有分布,最大厚度为15.5 m,整体呈现出楔形体的形态,是最近一次海侵形成的海相地层;上更新统地层的分布受下部构造形态影响较大,在乳山以东海域缺失,整体上在研究区东南部较厚,近岸处减薄,平均厚度约60 m;中更新世沉积仍受到区域构造背景的控制,越靠近南黄海盆地北部凹陷其沉积越厚,反之越薄,直至尖灭消失;下更新世的沉积格局类似于中更新统,也受控于区域构造背景,其分布范围较中更新统更小更局限;上新世时期,黄海海域继续稳定沉降,构造稳定,期间沉积了一层厚度均匀、平坦的地层,厚度大体呈向西北减薄的楔形,等值线变化相对比较平缓;中新统地层作为裂后坳陷沉积的首套地层,其厚度分布特征与新近系底界面埋深基本一致。 相似文献
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北康盆地沉降作用与构造运动 总被引：6，自引：1，他引：6
在地质构造特征研究的基础上,采用地层回剥法和局部均衡模式,研究北康盆地的构造沉降作用,并探讨该盆地构造演化与区域构造运动的关系。北康盆地是一个拉张性盆地,经历了3次快速沉降作用。中始新世沉降作用占总构造沉降量的28％～34％,沉降速率为234～325m／Ma,拉伸系数最大达1.72,它是43Ma时印度板块和欧亚板块碰撞的结果。上始新世—早渐新世构造沉降作用速率较慢,幅度也较小,为西卫运动影响下的越东—万安走滑断裂发生走滑拉张活动所致。上新世—第四纪的沉降速率极快,幅度很大,可达整个构造沉降的40％以上,可能是太平洋板块与欧亚板块相互作用所引起的整个南海区域沉降在盆地中的反映。 相似文献
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针对渤中探区Q构造新近系近十年探索没有取得突破性进展,借鉴周边成熟油田浅层岩性勘探的思路,以地质认识为指导,以精细构造解释和岩性圈闭刻画为核心,综合运用地层切片、地震属性分析、90度相移及低幅度构造变速成图等多项地球物理技术,对新近系明下段浅水三角洲岩性圈闭进行精细识别与刻画.结果表明：地层切片结合地震属性技术有效识别砂体平面展布特征,90度相移技术辅助完成砂体精细刻画,低幅度构造变速成图技术真实反映砂体构造特征.通过多项地球物理技术的应用,相继发现了Qa、Qb/c及Qd等一系列浅层岩性含油气构造,掀起了渤海海域浅层岩性勘探的热潮,同时也对相似地质背景探区具有借鉴意义. 相似文献
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根据川东石炭系实钻资料，结合前人资料对石炭系地层—构造复合圈闭进行了分类和总结；在此基础上，对川东石炭系地层—构造复合圈闭的控制因素进行了研究。研究表明沉积相是地层—构造复合圈闭的次要控制因素，而古岩溶、古构造是其主要控制因素；在此过程中，根据黄龙纽残余厚度分布状况提供的岩溶剥蚀强度信息、经压实恢复上覆梁山组碳质泥岩等厚度图反映的黄龙组顶面侵蚀地形变化印模及由岩溶相组合特征所显示的古水文条件，恢复了川东地区黄龙组古岩溶地貌。在分析古岩溶地貌单元古水文状况、溶蚀方式和强度、古构造及古岩溶厚度的基础上，对川东内古岩溶进行了区块划分。最后综合了各种资料，对川东石炭系地层—构造复合圈闭有利区带进行了预测。 相似文献
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黄河三角洲刺穿体分布在废弃三角洲叶瓣水下斜坡的下部,成因与密西西比三角洲有很大差别,其形成与软弱层变形(内因)和海洋侵蚀(外因)密切相关。高分辨率黄河三角洲典型的地震地层和解释地层剖面、浅地层剖面和钻孔资料联合解释表明,海底刺穿的发源层来自于河口沙坝下部的前三角洲相软弱层变形。三角洲特有的地层结构造成软弱层上覆的物质压力分布不均,普遍存在一个沿三角洲斜坡下部分布的低压异常带,三角洲堆积过程中,软弱层在低压异常带中的变形已经存在,形成前三角洲上部的凸出地形。黄河口摆动后,海底快速冲刷,在最大冲刷中心也是最大压力释放中心刺穿体形成,随着海洋侵蚀速率减缓,刺穿作用将逐渐减弱,最终将被冲刷消亡。软弱层变形及刺穿对海洋工程设施危害极大。类似这种三角洲特有的地层压力结构在平原海岸地区广泛存在,深入研究软弱层变形机理,对近海工程意义重大。 相似文献
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Grevemeyer Ingo Weigel Wilfried Dehghani G. Ali Whitmarsh Robert B. Avedik Felix 《Marine Geophysical Researches》1997,19(1):1-23
Two seismic refraction and gravity lines were obtained along and normal to the axis of the Aegir Rift, an extinct spreading centre in the Norway Basin. Velocity-depth solutions and crustal structure models are derived from ocean-bottom records using two-dimensional ray tracing and synthetic seismogram modelling techniques. Gravity data are used to generate models consistent with the lateral variations in thickness of the layers in the crustal models. The resulting models require considerable degree of lateral inhomogeneity along and perpendicular to the rift axis. Crust within the extinct spreading centre is found to be thinner and of low P-wave velocity when compared with the crust sampled off-axis. To explain reduced velocities of the lower crust we suggest that, due to the relationship between fracturing and seismic velocity, the decreasing spreading rate leading up to extinction let the mechanically strong layer thicken, so that faulting and fracturing extended to greater depths . Low velocities are also observed in the uppermost mantle underlying the extinct spreading ridge. This zone is attributed to hydrothermal alteration of upper mantle peridotites. Furthermore, after spreading ceased 32-26 my ago, ongoing passive hydrothermal circulation was accompanied by the precipitation of alteration products in open void spaces, thereby decreasing the porosity and increasing the velocity. Consequently the typical low velocities of layer 2 found at active mid-ocean ridges have been replaced by values typical of mature oceanic crust. 相似文献
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I. P. Chunchuzov S. N. Kulichkov O. E. Popov V. G. Perepelkin 《Izvestiya Atmospheric and Oceanic Physics》2010,46(5):597-607
A wave theory of propagation of an acoustic pulse in a moving stratified atmospheric layer above the ground with a finite
impedance of an underlying ground surface is developed. The shapes of acoustic signals in a near-ground atmospheric waveguide,
which are formed due to temperature inversion and a vertical shear of the wind velocity, are calculated based on this theory.
These signals are compared with those measured during the experiments where vertical profiles of the wind velocity and temperature
in an atmospheric boundary layer have been continuously controlled using a sodar, a temperature profile meter, and acoustic
anemometers or thermometers mounted on a 56-meter-high mast. The joint action of a near-ground acoustic waveguide, the impedance
of the underlying surface, and a vertical layered structure of the boundary atmospheric layer on a signal shape far from the
acoustic source are studied. 相似文献
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为准确建立海底地声模型,本文探讨地声模型的基本组成和基本结构。通过样品实验室测量,分析南海海底表层沉积物的密度、孔隙度与声速随着埋深变化的关系,得出海底实际存在的低声速表面–声速缓慢变化类型、低声速表面–声速增大类型、高声速表面–声速缓慢变化类型和高声速表面–声速增大类型4种典型地声结构;对比钻探测量,分析黄海海底沉积物的密度、孔隙度与声速随埋深变化关系,得出海底地声模型分层特征与地声结构组合特征。研究表明,地声模型可以归结为4种基本地声结构的组合,通过与底层海水声速、同层内声速剖面以及与上层海底沉积物下表面声速的比较,可以建立各种海底地声模型;基于实验室测量法建立的地声模型可以作为参考地声模型,但需要考虑实际海底温度和压力梯度以及海底沉积物的频散特性等,借助于声速比校正法和频散性理论模型进行计算及修正。 相似文献
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Acoustic environment and physico‐mechanical properties of the shelf seabed off the pearl river mouth
Abstract The vast shallow sea off the Pearl River mouth in the northern South China Sea is an important prospecting area for offshore oil development. In recent years, the authors have investigated acoustic and geotechnical characteristics of marine sediments in this area. An intercalated layer of low sound velocity and low compressive strength has been found within the seabed, in which the median diameter of sediment grains is fine and the sound velocity is 100–200 m/s lower than that of the overlying and underlying layers. The minimum unconfined compressive strength of this layer is 0.075 kg/cm2, which is lower than that of the over‐ and underlying layers by an order of magnitude. Such an intercalation often constitutes a threat to the stability of shallow foundation soil. In case of overloading, the layer may be weakened, and seafloor sliding between different sediment layers may occur. The regional distribution of these kinds of weak intercalations of low sound velocity may be traced by a subbottom profiler and by means of sediment acoustical investigations. Correlation between the gray level of a layer on subbottom profile records and physical properties of the layer (including sound velocity and reflectivity) suggests that the layer of sufficient bearing capacity must be searched by means of sediment acoustics at least to the depth of a high‐velocity substratum of stronger reflection. 相似文献
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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. 相似文献
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Naresh Kumar Thakur Pasupuleti Prasada Rao N. Vishwanath Sanjeev Rajput Bhaskarabhatla Ashalatha 《Marine Geophysical Researches》2007,28(4):373-378
Seismic tomography is an effective means of estimating velocity and structure from multichannel seismic (MCS) reflection data.
In this study we have followed a 2D approach to arrive at the probable velocity field configuration from multichannel seismic
data and infer the presence of gas hydrates/free-gas in the offshore Kerala-Konkan region, along the eastern part of a seismic
line on which a bottom simulating reflector (BSR) has previously been identified. Tomographic modeling consists of the identification
of reflection phases and picking of respective travel times for various source-receiver positions. These picks were then utilized
to arrive at a 2D velocity field following a forward and inversion approach using a ray tracing technique. The modeling for
the first time brought out the finer scale velocity structure under the region of investigation. Modeling through the 2D approach
shows lateral variation in velocity field along the studied segment of the seismic line. The results indicate a thin (∼50–60 m)
sedimentary cover with velocity ranging from 1,770 to 1,850 m/s. A sedimentary layer with high P-wave velocity 1,980–2,100 m/s
below the sea floor was interpreted as the hydrate layer. The thickness of this layer varies between 110 and 140 m. The hydrate
layer is underlain by a low-velocity layer having velocities in the range 1,660–1,720 m/s. This low velocity may represent
a free gas layer, whose thickness varies between 50 and 100 m located below the hydrated layer. The investigation suggests
the occurrence of gas hydrate underlain by free gas in some parts of the Kerala-Konkan offshore region. 相似文献
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This report describes extensive investigations of the near bottom layer of the Western Baltic (Mecklenburg Bight, Darss Sill and Arkona Basin) which were conducted over a 5 year period to determine the typical structure, vertical thickness, vertical turbulence structure, and spatial and temporal variability of this water mass with regard to the area's particular hydrographic conditions. Series of vertical profiles were obtained using the microstructure profiler MSS86, which is capable of measuring high resolution profiles of temperature, conductivity, current shear, light attenuation and pressure down to the seafloor. The near bottom current structure was simultaneously measured with conventional current metres at fixed depths. A typical vertical density structure of the near bottom layer was found. At all investigation sites the Bottom Boundary Layer was separated from the overlying water mass by a well pronounced thermohaline pycnocline. A homogeneous water layer was situated above the bottom with a mean thickness of 2.2 m and typical variation between 0.5 and 3.5 m. The thickness of both the homogeneous layer and of the near bottom layer vary considerably. It is suggested that horizontal advection is responsible for these fluctuations in thickness. The variation in thickness of the Homogeneous Layer is independent of the local mean current velocity, wind speed and energy dissipation rate. Over periods of about 2 days the thickness of the Homogeneous Layer is determined by the average wind speed. The Bottom Boundary Layer shows its own characteristic dynamic, which is largely decoupled from that of the remaining water body. A logarithmic layer was generally not resolved by the current measurements. From dissipation rate measurements, the wall layer was determined to be 0.9 m thick. There was no significant correlation between the dissipation rate and the local wind speed, or between the dissipation rate and local mean current u100. This means that any simple parameterisation relating u100 or friction velocity to the locally produced turbulence and consequently to the resuspension of sediment is probably not applicable to shallow sea areas with properties like the Western Baltic. The investigation of sediment concentration in the BBL illustrates the importance of local effects combined with advection. The sediment stratified layer covers only the bottom most 50 cm. 相似文献
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The quality of depth imaging is directly related to the accuracy of the underlying velocity model. In most sub-salt settings, lack of angular illumination severely degrades the resolution and accuracy of velocity information derived from the seismic data itself. A standard approach for building a starting velocity model uses more reliable velocity information outboard of salt which is subsequently extrapolated to populate the sub-salt regions. The shortcoming of this method lies in the assumption that the effective stress observed outboard of salt can be extrapolated beneath salt solely as a function of depth below mudline. 相似文献