首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 359 毫秒
1.
—?Two chemical calibration explosions, conducted at the former Semipalatinsk nuclear test site in 1998 with charges of 25 tons and 100 tons TNT, have been used for developing travel-time curves and generalized one-dimensional velocity models of the crust and upper mantle of the platform region of Kazakhstan. The explosions were recorded by a number of digital seismic stations, located in Kazakhstan at distances ranging from 0 to 720?km. The travel-time tables developed in this paper cover the phases P, Pn, Pg, S, Sn, Lg in a range of 0–740?km and the velocity models apply to the crust down to 44?km depth and to the mantle down to 120?km. A comparison of the compiled travel-time tables with existing travel-time tables of CSE and IASPEI91 is presented.  相似文献   

2.
Summary The paper deals with the results of DSS measurements along international profile VII, carried out by Czechoslovak and Polish geophysicists in 1970 – 71. The profile situation is shown in Fig. 1. By 1971 part of the profile in the region of the Bohemian Massif between points 1 and 3 and in Poland between points 5 and 7 had been surveyed (Fig. 2). The seismograms were used to construct the travel-time curves of the fundamental types of waves PK, PM, Pn (Fig. 4). The mean velocities were computed from the travel-time curves of the reflected waves (PM and PK) and the refracted waves (Pg). Isolines of the mean velocities could be constructed for the region of the Bohemian Massif (Fig. 6). The velocity data found were used for the depth interpretation of the travel-time curves of the principal types of waves and to construct a seismic section (Fig. 8). In the region of the Pre-Sudeten block the thickness of the crust was found to be 34–37 km, and in the Sudeten it increased to 40 km. Towards the south the thickness of the crust gradually reduces to 30 km in the system of the Luice faults. In the Bohemian Cretaceous the thickness of the crust is about 30 km. Further to the south, in the region of the Moldanubicum, the thickness of the Earth's crust increases rapidly, and at the southern border of the Central Bohemian pluton it reaches values of about 42 km.  相似文献   

3.
Introduction Bohai Bay, along with its adjacent areas, is one of the seismically active areas in North China. Understanding its crust/upper-mantle structural characteristics and lateral heterogeneity of the medium in this area is of great significance to the study of seismogenic environment, thus improvimg the level of earthquake prediction. For years, scientists have studied the area by gravity and magnetic methods (FENG, et al, 1989), geothermal field (WU, et al, 1988; TIAN, ZHANG, 19…  相似文献   

4.
A two dimensional velocity model of the upper mantle has been compiled from a long-range seismic profile crossing the West Siberian young plate and the old Siberian platform. It revealed considerable horizontal and vertical heterogeneity of the mantle. A sharp seismic boundary at a depth of 400 km outlines the high-velocity gradient transition zone, its base lying at a depth of 650 km. Several layers with different velocities, velocity gradients and wave attenuation are distinguished in the upper mantle. They likewise differ in their inner structure. For instance, the uppermost 50–70 km of the mantle are divided into blocks with velocities from 7.9–8.1 to 8.4–8.6 km s?1.Comparison of the travel-time curves for the Siberian long-range profile with those compiled from seismological data for Europe distinguished large-scale upper mantle inhomogeneities of the Eurasian continent and allowed for the correlation of tectonic features and geophysical fields. The velocity heterogeneity of the uppermost 50–100 km of the mantle correlates with the platform age and heat flow, i.e., the young plates of Western Europe and Western Siberia have slightly lower velocities and higher heat flows than the ancient East European and Siberian platforms. At greater depths (150–250 km) the upper mantle velocities increase from the ocean to the inner parts of the continent. The structure of the transition zone differs significantly beneath Western Europe and the other parts of Eurasia. The sharp boundary at a depth of 400 km, traced throughout the whole continent as the boundary reflecting intensive waves, transforms beneath Western Europe into a gradient zone. This transition zone feature correlates with positions of the North Atlantic-west Europe geoid and heat-flow anomalies.  相似文献   

5.
—Comparison of deep seismic sounding (DSS) results of different profiles across the Narmada-Son Lineament (NSL), India indicates the anomalous nature of the crust along the Ujjain-Ma han profile. Forward travel time and synthetic seismogram modeling, using normalized record sections of refraction and wide angle reflection data acquired along the Ujjain-Mahan deep seismic sounding profile across NSL, brings into focus the presence of high velocity (7.0–7.3?km/s) subhorizontal layers from a depth of 8–12?km down to Moho. The tectonic implication of such reflections (layering in the crust) is discussed. The two fault zones, reported by earlier workers, flanking the rift might have acted as feeders for the mantle material to intrude into the middle and lower crustal columns.  相似文献   

6.
Extensive seismic investigations of the crust and upper mantle have been carried out in the region of the Barents and Kara seas during the past decade. One of the profiles (2-AR) measured by FGU NPP “Sevmorgeo” with the CDP and deep seismic sounding methods was successfully used for comparatively analyzing different technologies of constructing seismic sections and for demonstrating a high information content of the method of mathematical modeling and the constructions of wave sections from supercritical reflected waves. It is shown that the crusts of the North Barents and South Kara basins are different. In the first case, the velocity section changes insignificantly, whereas, in the second case, velocities in the crust increase under the basin and the M boundary rises. The crust of the Novaya Zemlya orogen has a thickness of 48 km, and its average thickness on the profile is 35 km.  相似文献   

7.
The transitional area between the northeastern margin of the Qinghai-Tibetan Plateau, Ordos Block and Alxa Block,also being the northern segment of the North-South Seismic Belt, is characterized by considerably high seismicity level and high risk of strong earthquakes. In view of the special tectonic environment and deep tectonic setting in this area, this study used two seismic wide-angle reflection/refraction cross profiles for double constraining, so as to more reliably obtain the fine-scale velocity structure characteristics in both the shallow and deep crust of individual blocks and their boundaries in the study area,and further discuss the seismogenic environment in seismic zones with strong historical earthquakes. In this paper, the P-wave data from the two profiles are processed and interpreted, and two-dimensional crustal velocity structure models along the two profiles are constructed by travel time forward modeling. The results show that there are great differences in velocity structure,shape of intra-crustal interfaces and crustal thickness among different blocks sampled by the two seismic profiles. The crustal thickness along the Lanzhou-Huianbu-Yulin seismic sounding profile(L1) increases from ~43 km in the western margin of Ordos Block to ~56 km in the Qilian Block to the west. In the Ordos Block, the velocity contours vary gently, and the average velocity of the crust is about 6.30 km s-1; On the other hand, the velocity structures in the crust of the Qilian Block and the arclike tectonic zone vary dramatically, and the average crustal velocities in these areas are about 0.10 km s-1 lower than that of the Ordos Block. In addition, discontinuous low-velocity bodies(LVZ1 and LVZ2) are identified in the crust of the Qilian Block and the arc-like tectonic zone, the velocity of which is 0.10–0.20 km s-1 lower than that of the surroundings. The average crustal thickness of the Ordos Block is consistently estimated to be around 43 km along both Profile L2(Tongchuan-Huianbu-Alashan left banner seismic sounding profile) and Profile L1. In contrast to the gently varying intra-crustal interfaces and velocity contours in the Ordos Block along Profile L1, which is a typical structure characteristic of stable cratons, the crustal structure in the Ordos Block along Profile L2 exhibits rather complex variations. This indicates the presence of significant structural differences in the crust within the Ordos Block. The crustal structure of the Helan Mountain Qilian Block and the Yinchuan Basin is featured by "uplift and depression" undulations, showing the characteristics of localized compressional deformation.Moreover, there are low-velocity zones with alternative high and low velocities in the middle and lower crust beneath the Helan Mountain, where the velocity is about 0.15–0.25 km s-1 lower than that of the surrounding areas. The crustal thickness of the Alxa Block is about 49 km, and the velocity contours in the upper and middle-lower crust of the block vary significantly. The complex crustal velocity structure images along the two seismic sounding profiles L1 and L2 reveal considerable structural differences among different tectonic blocks, their coupling relationships and velocity structural features in the seismic zones where strong historical earthquakes occurred. The imaging result of this study provides fine-scale crustal structure information for further understanding the seismogenic environment and mechanism in the study area.  相似文献   

8.
We present new seismic velocity models of the crust and uppermost mantle along two refraction and wide-angle reflection profiles in the southern Fennoscandia: the Pribalt and 1-EB profiles. Some new results obtained along the Coast and the Baltic Sea profiles are also presented. The intercept time method and ray tracing are used for the modeling. The study shows that the lateral variations are small in the velocity structure of?? the crust up to the depth of 20?C25 km. The most significant lateral variations are observed in the Moho discontinuity topography and in the seismic velocities in the lower crust. In Paleoproterosoic Svekofennian domain, besides the well-known Moho depression in southern Finland, another Moho depression is revealed in the region from the Gotland Island to the Gulf of Riga. We suggest that this depression can correspond to the unknown crustal unit (we call it the Gotland-Riga belt). The Moho depth increases from the average of 40?C45 km to 55 km in this belt. The Moho depression is filled by the matter with velocities of 6.8?C7.1 km/s. Deep faults inclined to the north and strong variations of the mantle velocities are typical for the uppermost mantle of the Gotland-Riga belt.  相似文献   

9.
Crustal structure in Xiaojiang fault zone and its vicinity   总被引:5,自引:0,他引:5  
Based on the integrative interpretation of travel-time data and amplitude information obtained from the deep seismic sounding experiment on the Chuxiong-Luoping profile,eastern Yunnan province,carried out in January of 2005,we present a 2-D P wave velocity structure along the profile. The crustal structure shows remarkable contrasts between the two sides of the Xiaojiang fault zone,although the whole profile is situated within the Yangtze platform. The average P wave velocities of the crust on the west and ...  相似文献   

10.
云南西部地壳深部结构特征   总被引:10,自引:3,他引:7       下载免费PDF全文
在云南西部,穿过红河、小江断裂带完成了一条长360 km、呈北东向的深地震宽角反射/折射剖面.通过对该测线的观测资料进行一维、二维模拟解释,得到了沿剖面的二维地壳速度模型.研究结果显示,沿测线Moho界面埋深横线变化大,其西南侧Moho埋深约35 km,东北侧Moho最大埋深可达43 km.沿剖面从西南到北东方向,地壳平均P波速度从5.9 km/s逐渐增加到6.13 km/s,但显著低于全球大陆平均值.结合以往的接收函数和面波联合反演结果,我们推算沿测线从西南到东北,其下方地壳泊松比介于0.23~0.25之间.剖面西南侧上地壳具有异常低的P波速度和泊松比,暗示其下方上地壳以α-相长英质组分为主;而剖面东北上地壳相对较高的P波速度和泊松比则暗示其物质组成以花岗岩-花岗闪长岩为主.研究区下地壳的P波速度和泊松比分别介于6.25~6.75 km/s和0.24~0.26 km/s之间,暗示其上部组成以花岗岩相的片麻岩为主,而下部组成则以角闪石类岩石为主.红河断裂两侧地壳速度显著不同,从浅到深其速度差异逐渐变弱,但红河断裂两侧地壳厚度变化较大.而小江断裂下方两侧地壳速度和地壳厚度变化并没有红河断裂那么明显.  相似文献   

11.
杨峰  黄金莉 《地球物理学报》2013,56(5):1487-1496
本文收集了首都圈地区40个测点的石油地震叠加速度资料,经常规处理后得到各测点下方速度随深度变化的曲线;对9条人工地震测深剖面的解释结果进行数字化处理获得各剖面下方离散的速度数据;应用上述资料和专业地质建模软件构建了首都圈地区(115.50°E-117.60°E,38.40°N-40.75°N)范围内上地壳高精度三维P波速度模型.结果表明:华北盆地为隆坳相间区,从东至西依次是黄骅坳陷、沧县隆起和冀中坳陷,上地壳速度结构十分复杂;结晶基底的埋深变化剧烈,冀中坳陷下最深处可达10 km,沿构造走向整体呈西南深、东北浅的趋势,沧县隆起下埋深约2~4 km,黄骅坳陷下最深处则达9 km,剧烈的基底起伏反映出盆地内部不同次级构造单元的差异沉降和中、新生代以来强烈的拉张构造运动.太行山、燕山隆起下的基底埋深较盆地区浅,体现出隆起区新生代以来的抬升构造运动.本文首次将石油地震叠加速度资料用于首都圈地壳速度模型的构建,与以往用人工地震测深资料得到的模型相比,本文结果对华北盆地复杂的上地壳结构刻画得更为细致.  相似文献   

12.
腾冲火山区地壳结构的人工地震探测   总被引:12,自引:3,他引:9  
介绍在腾冲地区完成的由一条近南北方向纵测线和两条近东西向的非纵测线组成的人工地震测深工程以及对纵测线资料解释的初步结果。上地壳的平均速度为5.9km/s,顶界面深度为23km左右;中地壳可分为2层,平均速度为6.17km/s;纵线的平均地壳厚度为40km。在团田至腾冲之间的基底速度相当低(5.80km/s)。在腾冲与固东之间的中地壳界面有局部上拱现象。局部地区的地壳速度偏低以及壳低界面上拱可能与岩  相似文献   

13.
A 3-D velocity structure of the crust has been constructed for almost the entire Baltic Shield area from data of extensive deep seismic studies on the shield. The construction involved a revision of all primary data (record sections and observed traveltime curves) obtained in this region over 50 years of research. Comparative analysis of wave fields revealed that three reference reflectors traceable throughout the shield area are K1 (a boundary velocity of 6.4–6.5 km/s), K2 (~6.8 km/s), and the mantle surface M (8.0–8.2 km/s). The resulting 3-D velocity structure is represented in the form of structural maps of these surfaces and a velocity distribution scheme in the upper crust. Using this general basic model, seismic cross sections are constructed by means of mathematical modeling along all profiles. They showed that, in addition to the main layers and reflectors above the K1 boundary, a lower velocity layer is traceable almost everywhere and the majority of deep faults flatten out toward this layer. On the whole, lateral variations in the velocity structure of the crust are small up to a depth of 40 km. The variations are most significant in the M topography: its average depth being 40–45 km, two deep (down to 50–60 km) depressions exist in southern Finland and the Baltic region. The origin of this depression filled with high velocity (7.2–7.4 km/s) rocks remains unclear.  相似文献   

14.
依据穿过巴颜喀拉地块的北部、秦岭地块、祁连地块、海原弧形构造区和鄂尔多斯地块的玛沁-兰州-靖边人工地震剖面的P波、S波的速度结构和泊松比结构,对青藏高原东北缘的地壳组成进行研究,并探讨其动力学过程. 首先,系统地归纳总结出一套将地震测深得到的原位P波速度校正到实验室温压条件下波速的具体可行的方法,利用大地热流值求取地壳不同深度的温度是该方法的关键. 然后,将上述剖面的原位P波速度校正到600 MPa和室温条件下,结合泊松比与相同温压条件下的实验室岩石波速测量结果进行对比,确定研究区的岩性组成. 结果表明,青藏高原东北缘地壳平均P波校正波速为6.43 km/s,地壳整体像上地壳一样呈酸性. 巴颜喀拉地块和秦岭地块南部的下地壳底部缺失校正速度Vp>6.9 km/s的基性岩,下地壳中酸性互层,下地壳整体呈酸性. 其他地块下地壳底部有2~10 km厚的校正速度Vp>6.9 km/s的基性岩,下地壳整体呈中性. 最后,根据青藏高原东北缘地壳结构和组成的研究成果,支持地壳增厚主要发生在下地壳的观点;提出巴颜喀拉地块和秦岭地块南部曾发生过下地壳拆沉作用,并导致高原的加速隆升.  相似文献   

15.
我国西北地区地壳中的高速夹层   总被引:13,自引:1,他引:13       下载免费PDF全文
在我国西北地区的柴达木盆地东部和甘肃地区,在距离炮点40互100公里处,能够接收到不少能量较强的地壳深界面反射波。另外还发现一种与一般反射波性质不同的波,其视速度特大,视速度随距离的变化不大,而且有较明显的终点;其吋距曲线与一般深界面反射波的时距曲线相交。根据它的特征可以判断地壳中存在具有速度梯度的高速夹层.求得的夹层参数为: 甘肃地区柴达木盆地东部覆盖层厚度 18.8公里 30.5公里覆盖层平均速度 5.5公里/秒 5.3公里/秒夹层厚度 6.0公里 3.2公里夹层速度 7.5-8.5公里/秒 7.5-8.0公里/秒夹层的上下界面均为强反射面,可以产生多次反射波。分別利用相邻两个反射波可以求得各层参数,并能避免射线折射的影响。甘肃地区和柴达木盆地东部的地壳厚度分別为51和52公里。地壳中有高速夹层的存在,可以更好地说明P~*速度分散的原因,而且也能够解释Lg波的传播机制。  相似文献   

16.
福州盆地及其周围地区地壳深部结构与构造的初步研究   总被引:20,自引:4,他引:20  
1986-1988年,福建省地震局在福州盆地及其周围地区完成了五条地震测深剖面:宁德-永春剖面;洪懒-宁德剖面;莲峰-福州(尚干)剖面;南平-永泰-平潭非纵剖面;并在宁德-古田-嵩口首次试验扇形剖面观测系统,结果表明,扇形剖面对确定断裂是有效的. 根据对地震波走时的正、反演计算,用理论地震图和射线追踪方法进一步修改和完善,得到了福州盆地及其周围地区地壳深部为高、低速相间的速度分布特征.地壳介质速度为6.40km/s,在中地壳普遍发育一层速度为5.80-5.90 km/s、厚度约5.0 km的低速层.Moho面深度30-33 km,福州盆地为一Moho面隆起区,隆起幅度达3.0 km.北西向断裂发育,其中,闽江断裂在纵剖面和扇形剖面均有明显的反映,并切割到Moho面2.0-3.0 km. 反射波谱频方法计算得到福州盆地地壳Q值仅120-150,比邻近地区明显偏低,中地壳低速层Q值为40-80,是一典型的低速-高导-低Q(高衰减)结构层,此层上界面埋深14-15 km,与居里面埋深较一致.这些结果为福州地区的地热资源远景预测和开发提供了地壳深部结构和某些地球物理场背景.  相似文献   

17.
tudyoncrustmantletectonicsanditsvelocitystructurealongtheBeijingHuailaiFengzhenprofileZHIPINGZHU(祝治平)XIANKANGZHANG(张先康)...  相似文献   

18.
Analysis of the refracted arrivals on a seismic reflection profile recorded along the wall of a tunnel at an iron mine near Thabazimbi, South Africa, shows variations in P-wave velocity in dolomite away from the de-stressed zone that vary between 4.4 and 7.2 km/s, though values greater than 5.8 km/s predominate along most of the profile. The seismic velocities at the tunnel wall, however, vary between 4.2 and 5.2 km/s. Time–depth terms are in the range from 0.1 to 0.9 ms, and yield thicknesses of the zone disturbed by the tunnel excavations of between 2 and 9 m. The very low seismic velocities away from the tunnel wall in two regions are associated with alcoves or ‘cubbies’ involving offsets in the wall of up to 10 m. The large variations in seismic velocity resolved over distances less than 15 m with signals of wavelength around 6–9 m are attributed to variations in the sizes and concentrations of fracture systems and cracks, and in the degree of groundwater saturation of the fracture systems. The results suggest that seismic velocity variations from reflection surveys may also assist modelling studies of the stress regime in deep mines, particularly if both P and S wave velocity variations can be determined. The seismic velocity variations inferred also show that application of refraction static corrections in the processing of ‘in-mine’ seismic reflection profiles is as important as in surface surveys, because of the higher frequencies of the seismic energy recorded in the deep mine environment.  相似文献   

19.
(王椿镛,张先康,林中洋,李学清)CharacteristicofcrustalstructureintheShulufaultbasinanditsvicinity¥Chun-YongWANGI;Xian-KangZHANG;Zhong-YangL...  相似文献   

20.
渡口及其邻近地区地壳浅层结构的研究   总被引:5,自引:5,他引:5       下载免费PDF全文
为了研究攀枝花-西昌构造带的地壳与上地幔顶部结构,在西起丽江东至者海全长350km的测线上进行了爆炸地震探测。本文利用所取得的六条地震记录剖面的Pg波组,研究测线下方地壳浅层结构。采用层状垂直梯度和横向不均匀模型,用理论走时和射线追踪方法来拟合实测Pg走时资料。得到深度为10km范围的地壳浅层结构和速度分布。 结果表明,该区地表P波速度以渡口至华坪一带为最高,达6.00km/s。向东西两侧逐步减小,东至者海为5.20km/s,西至丽江降为3.50km/s。局部地段因构造影响速度值有些起伏。从浅层结构和速度分布可见,该区存在箐河-程海、绿汁江、安宁河和甘洛-小江等深断裂带,并向地壳深部延伸。等速度线图表明,该区上地壳中有一高速岩体存在。攀枝花钒、钛、铁矿的富集以及其他热液型矿床的分布很可能与此有关。  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号