共查询到19条相似文献，搜索用时 187 毫秒
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基于中国大洋36和41航次浅地层剖面数据,结合DSDP钻井及国内外相关研究,对西太平洋维嘉平顶山顶部沉积物的浅地层剖面特征、沉积环境、沉积时代、沉积物厚度分布特征等进行了研究,发现3种主要的地层反射特征,分别代表3个沉积单元;山顶沉积物的厚度分布呈现出3个沉积中心区和4个基岩裸露/沉积物稀薄区的特点;平顶山东部的沉积异常可能与始新世的第二次火山活动有关。根据富钴结壳的生长和发育特点,结合维嘉平顶山的沉积物分布特征,圈定了结壳资源潜力分布区。维嘉平顶山作为中国重要的富钴结壳合同区块,本次研究对其富钴结壳资源进一步的勘探工作具有指导意义。 相似文献
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新近系保德阶建阶研究新进展 总被引：12，自引：4，他引：8
根据与古地磁极性年表的对比 ,山西保德冀家沟剖面含保德动物群的保德组上界年龄为 5 .30 Ma,底界年龄不超过 10 Ma,其红黏土的底界为 8Ma,显示该剖面不存在定义的保德阶 11.2 Ma的下界 ,也没有保存保德阶下部的沉积。《国际地层指南》提倡用选择下界的界线层型来确定年代地层单位 ,其上界应该由后续单位的下界来确定。冀家沟剖面显然不具备保德阶的下界 ,但甘肃临夏盆地郭泥沟剖面含三趾马动物群的红黏土之下还有发育的中中新世沉积出露 ,因此 ,后一个地点应存在保德阶的下界 ,并有保德阶最底部的化石和适合于作古地磁分析的沉积物 ,所以临夏盆地是一个有可能建立保德阶下界界线层型的有利地点 相似文献
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阐述了对东海陆架南缘勘查区进行的高分辨率的浅地层探测情况。通过对测区的浅地层声学剖面的解释和研究,笔者认为:声学剖面较直观地反映了该区的海底地形、地貌、浅地层沉积物结构、构造及海底基岩埋深状况,对恢复该区沉积地质环境和发育历史有重要意义。 相似文献
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中太平洋海山富钴结壳生长习性及控制因素 总被引：15，自引：2，他引：15
通过对"大洋一号"调查船DY95-10、DY105-11、DY105-12等航次结壳样品和海底摄像照相资料等综合观测分析,从不同角度对中太平洋海山富钴结壳的生长习性及控制因素进行了初步探讨.结果表明,富钴结壳可以在海山区的各种岩石上生长发育,对岩性没有明显的选择性,载壳岩石类型统计结果与岩石类型区域上的分布不均衡有关,而与岩性本身并没有必然的联系.结壳生长的厚度除受载壳岩石形成年代、物化环境影响外,与其所经受构造活动的强度和频率也有密切联系.水深可能对结壳的生长发育具有一定的控制作用,但由于海山在结壳生长后存在移动和升降运动,因此现在海山上的结壳并不存在截然的水深界限.地形对富钴结壳覆盖率、产状、形态具有明显的控制作用,海山坡度太缓、太陡均不利于结壳的生长发育;在海山坡度较大处生长的结壳多呈平板状,而在坡度较小处生长的结壳多呈波纹状或枕状;海山的斜坡上生长的多为板状结壳,而在平坦低洼处则有利于砾状结壳、钴结核的生长发育. 相似文献
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中、西太平洋海山区是富钴结壳的重要富集区,钙质远洋沉积、碳酸盐岩沉积及重力作用引起的滑塌沉积是海山山顶和斜坡的主要沉积类型,它们的空间分布规律对于富钴结壳的分布至关重要.在国内首次利用EM122多波束回波强度资料对中太平洋潜鱼海山进行了底质类型研究,对回波强度资料进行处理和统计分类,并与浅地层剖面和地质取样结果对比,分析得出了4种底质类型,即富钴结壳、钙质远洋沉积、碳酸盐岩基底及碎屑流沉积.这几种底质类型具有不同的回波强度特征,其中富钴结壳区表现为均一的回波强度高值特征;钙质远洋沉积区表现为均一的回波强度低值特征,二者回波强度值相差约20 dB.结果显示潜鱼海山山顶仅局部发育钙质远洋沉积,大部分为碳酸盐岩基底出露区,山顶边缘及侧翼山脊处为主要的富钴结壳分布区.此外,该海山存在3处较大规模的重力滑塌沉积区,主要为碎屑流沉积. 相似文献
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浅地层剖面原始数据中海底反射信号的识别及海底地形的自动提取 总被引：1，自引：0，他引：1
2004年12月使用浅地层剖面仪GeoChirpⅡ在长江口南港进行了浅地层剖面观测,采集的原始数据反映了声波记录在海底表面存在着振幅的极大值及该记录的信噪比较低.根据声波记录在海底表面的反射特征,首先在剖面图像中确定海底表面所在的采样点范围,然后采用最大振幅法实现海底反射信号的识别及海底地形的自动提取,并对提取出的海底地形进行平滑处理.采用该方法从长江口南港的浅地层剖面原始数据文件中识别了海底反射信号,实现了海底地形的自动提取并把提取出的海底地形和原海底地形进行了比较.结果表明,提取出的海底地形能够较精确地反映原海底表面韵律性的起伏形态,证明了该方法的有效性. 相似文献
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太平洋海山钴结壳资源量估算 总被引：2，自引：0，他引：2
为合理地估算出太平洋海山钴结壳资源量, 基于我国西太平洋海山钴结壳拖网采样调查资料以及对太平洋海山钴结壳资源分布规律和钴结壳矿区圈定参数指标的深入研究, 创造性地按海山不同高度、不同洋壳年龄赋予不同结壳厚度, 进而首次计算出太平洋海山干结壳资源量为(507.06~1 014.11)×108 t, 锰为(111.15~222.29)×108 t, 钴为(3.04~6.08)×108 t, 镍为(2.23~4.46)×108 t, 铜为(0.66~1.32)×108 t, 结壳分布面积为2 062 862 km2.通过Co通量与结壳Co沉积量、结壳厚度的相关分析表明, 赋予不同洋壳年龄段的结壳厚度是理论厚度的6.10%~12.20%, 这与Ku et al.得出"结壳生长时间只占其整个生命史4%"的认识非常相近, 说明所赋结壳厚度基本合理, 得出的结壳资源量基本正确.为整个大洋海盆内海山钴结壳资源量的估算提供了新方法. 相似文献
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HeGaowen LiangDonghong SongChengbin SunXiaoming WuShuigen ZhouJianping ZhangXuehua 《中国地质大学学报(英文版)》2005,16(2):178-182
Cobalt richferromanganesecrust,hereaftercalled Fe Mncrust,isoneoftheimportantmarinemineralre sourcesintheinternationalseabed.Fe Mncrustoccurs onthesurfaceofseamounts,whichareenrichedinco balt,nickel,copper,platinumgroupelements,rare earthelementsandothe… 相似文献
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青藏高原东北缘岩石圈密度与磁化强度及动力学含义 总被引：4，自引：0，他引：4
利用横贯柴达木盆地南北的格尔木—花海子剖面岩石圈二维P波速度结构以及地震波速度与介质密度之间的关系,建立了该剖面岩石圈二维密度结构与二维磁化强度的初始模型。依据重磁同源原理,在柴达木盆地重、磁异常的二重约束下完成了重磁联合反演,获得了该剖面岩石圈二维密度结构与二维磁化强度分布。结果表明:柴达木盆地地壳厚度沿测线变化较大,平均厚度约60km。在柴达木盆地南缘地壳厚约50km,达布逊湖附近地壳最厚为63km左右,大柴旦附近地壳较薄,为50km左右。柴达木盆地的地壳纵向上可分为三层,即上地壳、中地壳与下地壳。位于盆地中部的中、下地壳分别发育大范围的壳内低密度体,并处于上地幔隆起的背景之上;横向上可将盆地分成南北两个部分,分界在达布逊湖附近。整个剖面结晶基底埋深变化也很大,在达布逊湖附近为12km,在昆仑山北缘基底几乎出露地表。结晶基底的展布形态与地壳底界,即莫霍面呈近似镜像对称。综合研究认为,柴达木盆地的岩石圈结构存在着明显的南北差异,其分界在达布逊湖的北面。在盆地南部,岩石圈介质横向变化较小,各层介质分布正常;在盆地的北侧,岩石圈结构特别在中、下地壳和上地幔顶部横向上发生了变化。壳内低密度体的存在意味着柴达木盆地具有较热的岩石圈和上地幔,加之基底界面与莫霍面的镜像对称分布,形成与准噶尔盆地和塔里木盆地的构造差异。多种地球物理参数所揭示的地壳上地幔结构及其横向变化特点为柴达木盆地构造演化及青藏高原北部边界的地球动力学研究提供了岩石圈尺度的地球物理证据。 相似文献
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The recent acquisition of high-quality seismic refraction data in the Jordan—Dead Sea rift and adjacent areas has made possible the investigation of the dynamic properties of seismic P-waves refracted and reflected at the crust—upper mantle boundary.
These waves cause high-amplitude arrivals near the outer cusp of the travel-time curve which are followed by an abrupt decrease in amplitudes at increasing distances beyond the cusp.
It has been shown that such amplitude distributions can only be the result of a smooth rapid increase of velocity with depth. In the case of the Jordan—Dead Sea rift the amplitude distribution indicates the presence of a transition zone between the lower crust and upper mantle in which the velocity increases smoothly. The interpretation of seismic refraction data in the Rhinegraben indicates the existence of a similar transition zone. In both rifts the crust—mantle boundary outside the rift is represented by sharp velocity discontinuity.
The comparison of the velocity structure of the crust—upper mantle boundary suggests that a smooth transition zone at the base of the lower crust is a characteristic property of continental rifts which could be interpreted in terms of crust—mantle interaction. 相似文献
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Takashi Iidaka Tetsuya Takeda Eiji Kurashimo Tomonori Kawamura Yoshiyuki Kaneda Takaya Iwasaki 《Tectonophysics》2004,388(1-4):7
A seismic experiment with six explosive sources and 391 seismic stations was conducted in August 2001 in the central Japan region. The crustal velocity structure for the central part of Japan and configuration of the subducting Philippine Sea plate were revealed. A large lateral variation of the thickness of the sedimentary layer was observed, and the P-wave velocity values below the sedimentary layer obtained were 5.3–5.8 km/s. P-wave velocity values for the lower part of upper crust and lower crust were estimated to be 6.0–6.4 and 6.6–6.8 km/s, respectively. The reflected wave from the upper boundary of the subducting Philippine Sea plate was observed on the record sections of several shots. The configuration of the subducting Philippine Sea slab was revealed for depths of 20–35 km. The dip angle of the Philippine Sea plate was estimated to be 26° for a depth range of about 20–26 km. Below this depth, the upper boundary of the subducting Philippine Sea plate is distorted over a depth range of 26–33 km. A large variation of the reflected-wave amplitude with depth along the subducting plate was observed. At a depth of about 20–26 km, the amplitude of the reflected wave is not large, and is explained by the reflected wave at the upper boundary of the subducting oceanic crust. However, the reflected wave from reflection points deeper than 26 km showed a large amplitude that cannot be explained by several reliable velocity models. Some unique seismic structures have to be considered to explain the observed data. Such unique structures will provide important information to know the mechanism of inter-plate earthquakes. 相似文献
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The Ordovician Sierras Pampeanas, located in a continental back-arc position at the Proto-Andean margin of southwest Gondwana, experienced substantial mantle heat transfer during the Ordovician Famatina orogeny, converting Neoproterozoic and Early Cambrian metasediments to migmatites and granites. The high-grade metamorphic basement underwent intense extensional shearing during the Early and Middle Ordovician. Contemporaneously, up to 7000 m marine sediments were deposited in extensional back-arc basins covering the pre-Ordovician basement. Extensional Ordovician tectonics were more effective in mid- and lower crustal migmatites than in higher levels of the crust. At a depth of about 13 km the separating boundary between low-strain solid upper and high-strain lower migmatitic crust evolved to an intra-crustal detachment. The detachment zone varies in thickness but does not exceed about 500 m. The formation of anatectic melt at the metamorphic peak, and the resulting drop in shear strength, initiated extensional tectonics which continued along localized ductile shear zones until the migmatitic crust cooled to amphibolite facies P–T conditions. P–T–d–t data in combination with field evidence suggest significant (ca. 52%) crustal thinning below the detachment corresponding to a thinning factor of 2.1. Ductile thinning of the upper crust is estimated to be less than that of the lower crust and might range between 25% and 44%, constituting total crustal thinning factors of 1.7–2.0. While the migmatites experienced retrograde decompression during the Ordovician, rocks along and above the detachment show isobaric cooling. This suggests that the magnitude of upper crustal extension controls the amount of space created for sediments deposited at the surface. Upper crustal extension and thinning is compensated by newly deposited sediments, maintaining constant pressure at detachment level. Thinning of the migmatitic lower crust is compensated by elevation of the crust–mantle boundary. The degree of mechanical coupling between migmatitic lower and solid upper crust across the detachment zone is the main factor controlling upper crustal extension, basin formation, and sediment thickness in the back-arc basin. The initiation of crustal extension in the back-arc, however, crucially depends on the presence of anatectic melt in the middle and lower crust. Consumption of melt and cooling of the lower crust correlate with decreasing deposition rates in the sedimentary basins and decreasing rates of crustal extension. 相似文献
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A study based on computation of D-function anomalies (method of joint gravity and magnetic data analysis) along profiles in the Bering Sea has been performed in both the Aleutian Basin with oceanic crust and the Bering continental shelf. This study revealed extended faults that affect not only the Earth’s crust but also the upper mantle. This is supported by seismic profiling. The calculated palinspastic reconstructions of the position of North America relative to “immobile” Eurasia 80, 52–50, 50–47, and 15–20 Ma ago allowed us to show that the revealed strike-slip faults are probable relics of an echeloned transform boundary between the Eurasian and North American lithospheric plates. The formation of this boundary beginning from the Late Cretaceous was apparently related to opening of the North Atalantic, which determined the large rate of displacement of North America relative to Eurasia. 相似文献
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大陆浅源地震震源空间分布可以看作是一种地球物理特征,大量震源的空间位置数据可用来刻划大陆地壳结构。通过研究南北地震带南段震源的空间分布特征,发现研究区震源深度分布在横向上的疏密变化与地质构造特征相对应。剖面震源分布等密度图显示,中、下地壳不同深度广泛分布着多震层。多震层的分布与地壳低速、低阻层具有相关性,多震层一般位于低速、低阻层的上方。中地壳层次的低速、低阻层很可能是壳内滑脱层,是韧性下地壳与脆性上地壳发生拆离解耦的构造层次;下地壳低速、低阻层是部分熔融、含流体的韧性流变层;壳内多震层的构造属性应是上地壳硬的脆性层,容易发生突然破裂,产生地震。低速、低阻层是大陆板块内部上地壳脆性层构造过程的主控因素,包括对大陆内部浅源地震的控制;因此,在低速、低阻层之上往往形成多震层,越是活动性强的低速、低阻层,其上多震层震源密度越高。南北地震带南段不同层圈和块体之间的差异运动控制了其地壳层次的构造活动,包括大量地震的发生,其中,下地壳流层与上地壳脆性层的差异运动在中地壳层次发生剪切拆离是最重要的因素。 相似文献
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Based upon the deep seismic sounding profiles carried out in the Tengchong Volcano-Geothermal Area (TVGA), western Yunnan Province of China, a 2-D crustal P velocity structure is obtained by use of finite-difference inversion and forward travel-time fitting method. The crustal model shows that a low-velocity anomaly zone exists in the upper crust, which is related to geothermal activity. Two faults, the Longling–Ruili Fault and Tengchong Fault, on the profile extend from surface to the lower crust and the Tengchong Fault likely penetrates the Moho. Moreover, based on teleseismic receiver functions on a temporary seismic network, S-wave velocity structures beneath the geothermal field show low S-wave velocity in the upper crust. From results of geophysical survey, the crust of TVGA is characterized by low P-wave and S-wave velocities, low resistivity, high heat-flow value and low Q. The upper mantle P-wave velocity is also low. This suggests presence of magma in the crust derived from the upper mantle. The low-velocity anomaly in upper crust may be related to the magma differentiation. The Tengchong volcanic area is located on the northeast edge of the Indian–Eurasian plate collision zone, away from the eastern boundary of the Indian plate by about 450 km. Based on the results of this paper and related studies, the Tengchong volcanoes can be classified as plate boundary volcanoes. 相似文献
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Crustal studies within the Japanese islands have provided important constraints on the physical properties and deformation styles of the island arc crust. The upper crust in the Japanese islands has a significant heterogeneity characterized by large velocity variation (5.5–6.1 km/s) and high seismic attenuation (Qp=100–400 for 5–15 Hz). The lateral velocity change sometimes occurs at major tectonic lines. In many cases of recent refraction/wide-angle reflection profiles, a “middle crust” with a velocity of 6.2–6.5 km/s is found in a depth range of 5–15 km. Most shallow microearthquakes are concentrated in the upper/middle crust. The velocity in the lower crust is estimated to be 6.6–7.0 km/s. The lower crust often involves a highly reflective zone with less seismicity, indicating its ductile rheology. The uppermost mantle is characterized by a low Pn velocity of 7.5–7.9 km/s. Several observations on PmP phase indicate that the Moho is not a sharp boundary with a distinct velocity contrast, but forms a transition zone from the upper mantle to the lower crust. Recent seismic reflection experiments revealed ongoing crustal deformations within the Japanese islands. A clear image of crustal delamination obtained for an arc–arc collision zone in central Hokkaido provides an important key for the evolution process from island arc to more felsic continental crust. In northern Honshu, a major fault system with listric geometry, which was formed by Miocene back arc spreading, was successfully mapped down to 12–15 km. 相似文献