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1.
A dense seismic network (～100 stations) was operated in the Koyna-Warna region from January 2010 to May 2010, that allow us to collect 400 high-quality local earthquake data of magnitude less than 4. In this region, the fault structure and tectonic setting that accommodate the induced seismicity is not well understood. To investigate the seismotectonics of the region, we have inverted 7826 P- and 7047 S-P arrival times for 3-D Vp and Vp/Vs tomographic models along with hypocenters parameters in the region. Although, Dixit et al. (2014) have performed 3-D local earthquake tomography with double-difference tomography code using catalog differential time data. In this paper, Simulps14 code on the same data set is applied. For better approach P arrival time and S-P travel times are inverted directly for Vp, Vp/Vs variations and earthquake locations. High Vp ～5.9 to 6.5 and low to high Vp/Vs ～1.69-1.74 imaged in the hypocenter region. These features interpreted as a fluid bearing rock mass under high pore pressure. It is also observed that below the trap basement form a local topography depression between the Koyna and Warna Reservoirs. To the South of the Warna reservoir, intense seismic activity defines a major cluster of ～ 5 km width at 3 to7 km deep, located under the trap, where the basement is deepening. Such regions are inferred to be associated with the seismically active faults zones. The obtain velocity anomalies are reliable down to a depth of 10 km. This is also confirmed by the analysis of three resolution parameters viz. Hit count, Derivative Weight sum (DWS) and Resolution Diagonal Elements (RDE). 相似文献
2.
对紧邻发震断裂带的崩滑体进行动力响应分析时,考虑断裂带宏观破裂机制,即带状震源形成的地震动力作用对斜坡的影响更符合实际。依据汶川地震震源破裂机制与其空间位置差异,将该带状震源从发震断裂起破点至终破点依次分段为逆冲震源、逆冲兼少量走滑震源、逆冲兼走滑震源与走滑兼少量逆冲震源,基于此对汶川地震触发的四川安县大光包崩滑体在龙门山发震断裂带即带状震源作用下的动力响应特征进行了离散元数值模拟,揭示了其动力形成机制、触发主控因素和损伤、崩滑及堆积动态特征。研究表明：（1）依据该崩滑体离散元数值模型临界崩滑状态形成时间与此时发震断裂带破裂前锋所处位置关系,可判断其临界破坏是受到逆冲兼少量走滑震源引起的地震动力作用所致,而临界崩滑之前的坡体损伤主要由纯逆冲震源所致,其后的抛射碰撞破碎与堆积则主要受临界破坏时的地震惯性力和自身重力耦合作用所致,但由逆冲兼走滑与走滑兼少量逆冲震源形成的地震力仅对上述两个破坏过程起到了一定影响;（2）该崩滑体在带状震源作用下的动力响应过程为：在损伤至崩滑临界破坏阶段,坡体整体向其临空面发生了较大程度的水平位移后,潜在滑床又向坡体临空面反方向发生了一定程度的水平位移,致使潜在滑体完全破碎并处于与滑床彻底分离的临界状态;在坡体崩滑抛射阶段,坡体滑床发生了相当规模的反方向水平位移,其后滑床又开始做向坡体临空面方面的水平位移并直至其总体位移为0,而在此过程中竖向位移相对较小。对滑体而言,其在损伤、临界崩滑和抛射阶段则主要做向其临空面的水平位移,直至堆积自稳阶段其位移趋于稳定;（3）该坡体的损伤和临界崩滑破坏主要受纯逆冲震源及其少量走滑震源形产生的水平地震力作用所致,而在坡体抛射碰撞破碎与堆积阶段,滑体的动力响应主要是基于地形因素控制上的地震惯性力与自身重力作用所致,而后两种类型震源机制形成的水平和竖向地震力仅起到一定影响。 相似文献
3.
Bthoux Nicole Sue Christian Paul Anne Virieux Jean Frchet Julien Thouvenot Franois Cattaneo Marco 《Tectonophysics》2007,432(1-4):1-19
We investigate how focal solutions and hypocenter locations may depend on the ray tracing algorithm and the strategy of velocity inversion. Using arrival times from a temporary seismological network in the south-western Alps, a local earthquake tomography has been performed by Paul et al. [Paul, A., Cattaneo, M., Thouvenot, F., Spallarossa, D., Béthoux, N., and Fréchet, J., 2001. A three-dimensional crustal velocity model of the south-western Alps from local earthquake tomography. J. Geophys. Res. 106, 19367–19390.] with the method developed by Thurber [Thurber, C.H., 1993. Local earthquake tomography: velocity and Vp/Vs-Theory, in Seismic Tomography: Theory and practice, Iyer, H.M., and Irahara eds., Chapman and Hall, New York, 563–583.]. Another inversion of the same data set is performed here using a different tomography code relying on a shooting paraxial method and cubic interpolation of velocities. The resulting images display the same main features, although Thurber's code appears to be more robust in regions with scarce ray coverage and strong velocity contrasts. Concerning hypocenter location in Piemont units, one major result is the concentration of hypocenters at the boundary between the mantle wedge of the Ivrea body and the European crust. Forty-six focal mechanisms are shown that were computed using both the take-off angles in the minimum 1-D model and in the 3-D velocity structures resulting from the two inversions. The sets of focal solutions are very similar, proving the reliability and the coherency of the focal solutions. The widespread extension in the core of the western Alps is confirmed whereas a few compressive solutions are found east of the Piemont units. These results constrain the sharp change of stress tensor and evidence a decoupling of strain beneath the east of Dora Maira massif up to beneath the north of Argentera massif. On a geodynamical point of view seismicity and focal mechanism distribution are compatible with the present day models published for the western Alps, where the major feature is the lithospheric thickening [Schmid, S.M., and Kissling, E., 2000. The arc of the western Alps in the light of geophysical data on deep crustal structure. Tectonics, 19, 62–85.], implying widespread extension in the core of the western Alps [Sue, C., Thouvenot, F., Fréchet, J., and Tricart, P., 1999. Widespread extension in the core of the western Alps revealed by earthquake analysis. J. Geophys. Res., 104, 25611–25622.]. However the existence of compressive events dealing at depth with the boundary of Ivrea body allows to postulate that this geological structure is still tectonically active. Even if field work has not shown this so far, the Insubric line appears to extend toward the south at depth, as a blind fault, and to play a key role in the dynamics of the south-western Alps. 相似文献
4.
Shuzo Asano Hiroshi Okada Susumu Kubota Sadaomi Suzuki Toshikatsu Yoshii 《Tectonophysics》1973,20(1-4):137-145
The crustal structure of the Matsushiro area, Central Japan, was studied in two profiles, A and B, with the explosion seismic method to obtain a better understanding of the physical processes of the Matsushiro Swarm Earthquakes. The layer with a velocity of 6.0 km/sec is extremely shallow and becomes deeper west of Chikuma River and around the southeastern end of profile B; there exists a faultlike structure in the most active area. The comparison of hypocenter distributions with the crustal structure shows that almost all swarm earthquakes have their hypocenters below the 6.0 km/sec layer and are confined to the region where this 6.0 km/sec layer is shallow. The velocity gradient in the 6.0 km/ sec layer is determined with certainty by the time-term analysis.
In the seismically most active region the anomalous structure is derived not only from the traveltime analysis but also from the amplitude studies; that is, the velocity and the Q-value are smaller than in other regions. 相似文献
5.
The April 2006 earthquake sequence near Zakynthos (Western Greece) is analysed to identify the fault plane(-s). The sequence (33 events) was relocated to assess physical insight into the hypocenter uncertainty. Moment tensor solution of three major events was performed, simultaneously with the determination of the centroid position. Joint analysis of the hypocenter position, centroid position and nodal planes indicated sub-horizontal fault planes. Moment tensor solutions of 15 smaller events were performed under assumption that the source positions are those of the hypocenters (without seeking centroids). Their focal mechanisms are highly similar and agree with the analysis of the three major events. The preferable seismotectonic interpretation is that the whole sequence activated a single sub-horizontal fault zone at a depth of about 13 km, corresponding to the interplate subduction boundary. Considering that the Ionian Sea is a high-seismicity area, the identification of the seismic fault is significant for the seismic hazard investigation of the region. 相似文献
6.
Noelynna T. Ramos Carla B. Dimalanta Glenda M. Besana Rodolfo A. Tamayo Jr Graciano P. Yumul Jr. Victor B. Maglambayan 《Resource Geology》2005,55(3):199-206
Abstract. High seismic activity in the Philippines originates from tectonic convergence related to surface and subsurface seismotectonic features. Based on earthquake data, the archipelago can be divided into the seismically-active Philippine Mobile Belt and the aseismic North Palawan Block. The latter represents a rifted continental fragment of the Eurasian margin that juxtaposed with the rest of island arc units in central Philippines. Earthquake hypocenter plots on planar and in vertical profiles show that the seismic events are associated with known seismotectonic features. In addition, data suggest that the collision zone between the North Palawan Block and the Philippine Mobile Belt is characterized by a decreased amount of hypocenters at > 100 km depths. Although field evidence favors the presence of a subducted slab or slabs beneath western central Philippines, these are difficult to image using the present seismicity distribution dataset. 相似文献
7.
Local and regional minimum 1D models for earthquake location and data quality assessment in complex tectonic regions: application to Switzerland 总被引：1，自引：0，他引：1
One-dimensional (1D) velocity models are still widely used for computing earthquake locations at seismological centers or
in regions where three-dimensional (3D) velocity models are not available due to the lack of data of sufficiently high quality.
The concept of the minimum 1D model with appropriate station corrections provides a framework to compute initial hypocenter
locations and seismic velocities for local earthquake tomography. Since a minimum 1D model represents a solution to the coupled
hypocenter-velocity problem it also represents a suitable velocity model for earthquake location and data quality assessment,
such as evaluating the consistency in assigning pre-defined weighting classes and average picking error. Nevertheless, the
use of a simple 1D velocity structure in combination with station delays raises the question of how appropriate the minimum
1D model concept is when applied to complex tectonic regions with significant three-dimensional (3D) variations in seismic
velocities. In this study we compute one regional minimum 1D model and three local minimum 1D models for selected subregions
of the Swiss Alpine region, which exhibits a strongly varying Moho topography. We compare the regional and local minimum 1D
models in terms of earthquake locations and data quality assessment to measure their performance. Our results show that the
local minimum 1D models provide more realistic hypocenter locations and better data fits than a single model for the Alpine
region. We attribute this to the fact that in a local minimum 1D model local and regional effects of the velocity structure
can be better separated. Consequently, in tectonically complex regions, minimum 1D models should be computed in sub-regions
defined by similar structure, if they are used for earthquake location and data quality assessment. 相似文献
8.
9.
复杂的浅层气云使地下波场严重扭曲,地震剖面呈现模糊带,影响工区的构造认识和储层描述。品质因子Q是地震波在地层中的衰减属性,Q深度偏移是考虑了地层吸收衰减的偏移成像技术,是提高气云区成像质量的有效方法;但是当浅层气云和深层底辟构造复杂发育时,常规Q场建模的精度往往不能满足Q偏移精细建模的需求。为解决以上难题,本文创新性地提出了全波形反演（full wave inversion, FWI）约束Q场建模技术思路：基于常规网格层析建立初始速度模型,利用FWI技术精细刻画速度异常进而约束Q模型的建立。这一“常规层析-FWI-Q反演”迭代的技术思路在白云凹陷Q深度偏移成像中得到成功应用,不仅提高了气云模糊区的成像质量,而且避免了油气勘探认识的多解性,证明了FWI约束Q场建模和Q深度偏移技术方法对改善复杂气云发育区的成像有效性。 相似文献
10.
日本列岛下太平洋俯冲板块的精细结构 总被引：1，自引：0，他引：1
尽管许多学者对日本列岛下的太平洋俯冲板块做了大量的研究,但板块内部的结构(比如板块厚度,板块内地震波速度随深度的变化以及洋壳的俯冲情况等)仍然不太清楚。利用日本地区密集台网收集到的中深和深发地震到时数据来探讨上述问题。采用三维射线追踪正演模拟法,首先利用333个远震计算得到了日本地区太平洋板块的厚度为85km;然后利用3283个地震(震源深度大于40km)的130227条P波到时进一步研究板块内部的精细结构。结果显示,沿深度方向6个地层段(间隔100km)内的速度扰动值分别为5.5%,4.0%,3.5%,2.5%,2.0%和6.0%,在40～500km范围内速度扰动随深度的增加而减小,这与温度随深度的变化情况相一致。当深度大于500km时,速度扰动突然增大到6.0%,分析认为该异常可能由发生在东亚大陆边缘下方的深发地震无法精确定位导致的。最后利用40～500km深度范围内的近震测试得到日本东北和北海道地区下方洋壳俯冲的深度均为110km,平均厚度分别为7.5km和5km,相对于一维模型的速度扰动分别为1%和-3%。这说明洋壳在俯冲到110km以深时,由于受温度和压力的影响,逐渐脱水、变质,直至与板块融合。通过分析震源与洋壳的位置关系,本研究认为北海道地区比东北地区下方的俯冲洋壳可能含有更多的流体(比如水),导致两地区洋壳内的速度相差如此之大。此外,因为日本南部与洋壳对应的区域多为海洋,观测台站较少,所以本研究无法测试得到该区域内的洋壳俯冲情况。 相似文献
11.
井间地震走时波形层析成像方法 总被引：2，自引：1，他引：2
提出了井间地震走时波形顺序反演方法。该方法先利用井间地震走时反演得到速度模型的低频成分 ,然后用井间地震波形反演获得速度模型的高频成分。数值模型试验和实际应用结果表明 ,该方法反演稳健 ,提高了走时成像的分辨率 ,克服了波形成像易于陷入局部极小的缺陷 ,实现了快速高分辨率成像。 相似文献
12.
井地联合提取VTI介质各向异性参数 总被引：2，自引：0，他引：2
在新疆塔里木盆地某地区的宽方位三维地震数据中,VTI介质火成岩的各向异性和垂向速度变化引起非双曲线时差。通过对实际资料的系统分析,我们不能利用DMO反演法,移动震源VSP反演法和多偏移距VSP初至旅行时反演法提取Thomsen参数用于各向异性地震资料的处理。因此本文提出一个新的方法:运用地震资料和零偏移距VSP井求取火成岩的各向异性参数δ;在比较精确确定火成岩地层深度和厚度的情况下,利用偏移距VSP井,求取了各向异性参数ε,从而获得火成岩的瞬时各向异性参数η;充分考虑VTI介质垂向速度变化对时差曲线的影响,获得了各向异性参数ηeff。最后,利用所提取的各向异性参数,进行VTI介质各向异性速度分析和成像,成像质量得到明显改善。 相似文献
13.
为了深入了解日本东北俯冲带的地震构造及火山活动,利用布设在日本列岛上密集地震台网所记录到的高质量浅震及深震到时数据,反演求得了该区域地壳及上地幔的三维P波和S波速度结构。为了最大程度地利用地震数据提取模型空间中更为精细的速度结构信息,采用不规则网格模型采进行地震层析成像反演。所得的高分辨率成像结果清晰地显示,2008年岩手地震(M 7.2)位于高低速异常的转换区,而且震源区的地壳介质非均匀性极强。在震源区的下地壳及上地幔顶部存在着明显的低速异常,可能代表了岛弧岩浆和流体在该深度处的储集。研究结果表明,2008年岩手地震的产生受到了来自上地幔楔的岩浆和流体的影响,且这些岩浆和流体与俯冲太平洋板块的脱水作用有着密切的联系。 相似文献
14.
为了避免单一物探方法在地质反演解释中存在的多解性弊端,本文介绍了以电成像法为主、浅层地震反射波法为辅的综合物探方法对隐伏断层进行探测的应用实例,首先,通过电成像法查找断层破碎带的位置走向,然后利用浅层地震反射波法精确查明断层的产状、性质、位置及断距等地质参数,并对两种方法的探测成果进行综合对比分析,推断该隐伏断层为走向近东西向,倾向近南北向的正断层,断层落差约4.2m,其上断点埋深约17.9m。经钻孔验证表明,电成像与浅层地震联合方法在浅覆盖区隐伏断层探测中具有精确、可靠、经济的优势,该方法具有较强的应用价值。 相似文献
15.
The results of seismic studies on the Friuli May 6, 1976 earthquake based on historical and seismological data collected by the OGS are presented. The epicenter and hypocenter distributions reconstructed from the Friuli networks and from Trieste WWSS Station are examined. The earthquakes of Latisana (1975–1976) are interpreted as the foreshocks of the main shock of May 6. Parameters of larger shocks are calculated. At the end a correlation between the hypocenters and the involved geodynamic structure of the region is proposed. 相似文献
16.
常规AVA三参数反演方法均基于横波速度与纵波速度之比γ为常数这一假设条件,且常被近似地取为0.5。然而在许多情况下γ并不为常数,而是在横向与纵向都渐变。若一概假定γ等于0.5,反演出的岩性参数势必要偏离真实值,因此有必要合理地选择γ。笔者基于贝叶斯理论,提出逐次迭代非线性AVA的反演方法。该方法把γ看成横向与纵向都渐变的反演初始背景,通过给定初始模型计算初始背景γ,并采用逐次迭代的策略求解该反演问题,解决了关于γ的选取问题以及由于引入变γ值而带来的非线性问题,提高了AVA三参数反演结果的精确度。 相似文献
17.
井间地震资料中蕴含丰富的地下储层岩性和物性信息,利用井间地震直达波初至信息,通过层析反演可以得到两井之间的速度剖面。通过对井间地震直达波振幅衰减信息的处理,可以实现井间的吸收衰减层析成像。基于井间地震直达波射线路径的一致性,提出了井间地震时域直达波走时层析反演和频域质心频率衰减层析同步反演方法,增加了约束条件,增强了抗干扰能力。对模型和实际资料的处理结果表明,速度和吸收衰减同步反演方法,提高了速度层析反演精度,得到了对油气更为敏感的衰减属性,增强了井间地震在储层描述和油气预测中的应用能力。 相似文献
18.
介绍了在倾斜均匀各向同性层状介质情况下,根据地震反射走时反演二维地层结构和地层速度的地震射线层析成像方法——走时反演。正演模型射线追踪是根据Fermat原理实现的,即求解满足该原理的非线性方程组得到射线与界面的交点,进而计算相应的走时。反演是先假设一初始模型,用最优化方法使射线追踪走时与观察走时的残差极小。最后计算了分辨矩阵和信息密度矩阵,以评价反演结果。对有噪情形也进行了反演。 相似文献
19.
This paper seeks to reconstruct the parameters of elastic layered media such as P-wave velocity, S-wave velocity, density and thickness from the multioffset seismic reflection data. Since the data are highly non-linear to the low-wavenumber components, the non-linear waveform inversion method, with the aid of generalized ray theory, is proposed to solve this problem in space–time domain. As opposed to the layer-stripping method, the present method attempts to invert all layer parameters simultaneously, thus reducing the cumulative errors resulting from the upper layers. The parameters are inverted by minimizing the weighted square error between the observed data and the calculated data of the layered model, the optimization of which is based on the quasi-Newton method. In synthetic tests, we find that the inverted results are good when the variation of parameters between layers is not too large. The modified method for large variation of parameters is first to fix those of deeper layers and neglect the signals reflected from them, then recover some other parameters simultaneously until those of upper layers attain a stable value, and finally, invert all parameters simultaneously. The results so obtained show a significant improvement. This method was tested to be stable in the presence of noise in seismograms. 相似文献
20.
地震波速层析成像方法研究进展 总被引：3，自引：0，他引：3
本文回顾了利用天然地震观测获取地下速度结构的方法。尽管有不同的新方法涌现,天然地震波速层析成像方法,尤其是多震相联合反演的格点层析成像方法,是当今使用广泛使用的层析成像方法之一,是对地球内部成像的最有效方式。波速层析成像方法的未来发展首先是提高第一手的观测资料,即增加接收地震波信息的地震台站分布密度;同时,通过多种地球物理方法联合反演相互约束可以给出较为严格的地球物理模型,并来降低了地球物理反演和解译的多解性,这是地球物理探测研究的趋势,也是天然地震波速层析成像方法的研究趋势。 相似文献