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1.
A method for three-dimensional (3D) ray tomography that uses the data on the travel time residuals of body waves is suggested. The underlying assumption of the method is smoothness of horizontal velocity variations. The region under study is divided into layers, and the velocity correction in each layer is assumed to only depend on the horizontal coordinates. The starting velocity model is specified as a function of depth. The numerical implementation of the method is noticeably simpler if the velocity-depth distribution is described by a linear function. The solution is determined by minimizing the functional that contains the sum of the integrals of the square gradients of the velocity corrections. The procedure is reduced to solving the two-dimensional (2D) problem in a way similar to the way previously developed for surface wave tomography (Ditmar and Yanovskaya, 1989). The obtained solution is smoothed, and the degree of smoothing is estimated jointly with the reconstruction of the solution. This approach does not require adaptive parameterization of the medium, i.e., division of the region into the blocks each of which is intersected by a sufficiently large number of rays. The efficiency of the method is demonstrated by the example of synthetic data and on the data on real traveltime residuals of the P waves in the Black Sea basin.  相似文献   

2.
Non‐uniqueness occurs with the 1D parametrization of refraction traveltime graphs in the vertical dimension and with the 2D lateral resolution of individual layers in the horizontal dimension. The most common source of non‐uniqueness is the inversion algorithm used to generate the starting model. This study applies 1D, 1.5D and 2D inversion algorithms to traveltime data for a syncline (2D) model, in order to generate starting models for wave path eikonal traveltime tomography. The 1D tau‐p algorithm produced a tomogram with an anticline rather than a syncline and an artefact with a high seismic velocity. The 2D generalized reciprocal method generated tomograms that accurately reproduced the syncline, together with narrow regions at the thalweg with seismic velocities that are less than and greater than the true seismic velocities as well as the true values. It is concluded that 2D inversion algorithms, which explicitly identify forward and reverse traveltime data, are required to generate useful starting models in the near‐surface where irregular refractors are common. The most likely tomogram can be selected as either the simplest model or with a priori information, such as head wave amplitudes. The determination of vertical velocity functions within individual layers is also subject to non‐uniqueness. Depths computed with vertical velocity gradients, which are the default with many tomography programs, are generally 50% greater than those computed with constant velocities for the same traveltime data. The average vertical velocity provides a more accurate measure of depth estimates, where it can be derived. Non‐uniqueness is a fundamental reality with the inversion of all near‐surface seismic refraction data. Unless specific measures are taken to explicitly address non‐uniqueness, then the production of a single refraction tomogram, which fits the traveltime data to sufficient accuracy, does not necessarily demonstrate that the result is either ‘correct’ or the most probable.  相似文献   

3.
层析成像是现今地震勘探开发处理中的常用手段,针对传统走时层析反演中角度覆盖问题,利用正则化约束加以解决,利用角道集的拾取拟合来判断实验模型的准确性,同时,不再利用原始炮记录拾取剩余时差,利用深度残差与走时残差的线性关系提高走时残差的拾取精度。以三层洼陷模型和实际资料进行试算,结果表明:本方法可以较好地反演更新偏移速度场,得到更精确的偏移成像结果,对于小尺度地质构造可以精细刻画。   相似文献   

4.
罗马尼亚Vancea地震区是大陆上发生与板块磁撞和削减有关的中深部地震活动的地区之一。本文介绍了应用地震层析成象方法研究该地区深部速度结构成果。在研究中使用了地方和区域地震所记录的433个浅源和中部地震的到时资料反演求解深至200km的三维速度结构,在走时和射线路径的计算中利用了有效的三维射线跟踪技术,在反演中采用LSQR算法,高分辨率的地震层析图象揭示了速度结构的广泛不均匀性,结果表明,地震层析  相似文献   

5.
To analyse and invert refraction seismic travel time data, different approaches and techniques have been proposed. One common approach is to invert first‐break travel times employing local optimization approaches. However, these approaches result in a single velocity model, and it is difficult to assess the quality and to quantify uncertainties and non‐uniqueness of the found solution. To address these problems, we propose an inversion strategy relying on a global optimization approach known as particle swarm optimization. With this approach we generate an ensemble of acceptable velocity models, i.e., models explaining our data equally well. We test and evaluate our approach using synthetic seismic travel times and field data collected across a creeping hillslope in the Austrian Alps. Our synthetic study mimics a layered near‐surface environment, including a sharp velocity increase with depth and complex refractor topography. Analysing the generated ensemble of acceptable solutions using different statistical measures demonstrates that our inversion strategy is able to reconstruct the input velocity model, including reasonable, quantitative estimates of uncertainty. Our field data set is inverted, employing the same strategy, and we further compare our results with the velocity model obtained by a standard local optimization approach and the information from a nearby borehole. This comparison shows that both inversion strategies result in geologically reasonable models (in agreement with the borehole information). However, analysing the model variability of the ensemble generated using our global approach indicates that the result of the local optimization approach is part of this model ensemble. Our results show the benefit of employing a global inversion strategy to generate near‐surface velocity models from refraction seismic data sets, especially in cases where no detailed a priori information regarding subsurface structures and velocity variations is available.  相似文献   

6.
张兵  王华忠 《地球物理学报》2019,62(7):2633-2644
复杂地表探区,尤其是盆山过渡区的油气勘探是我国也是世界上油气勘探的重点区域,但是此类区域油气地震勘探中满足精确地震成像的速度建模一直是个没有很好解决的问题.本文提出了一种综合性的数据域初至波走时与成像域反射波走时联合层析复杂地表浅中深层速度建模方法,并针对联合层析速度反演解的非唯一性问题,深入地分析了层析反演中正则化的本质意义,指出了建立构造特征正则化方法的具体技术路线,提出了联合层析的实现流程及策略.理论和实际数据试验表明,本文提出的数据域初至走时与成像域反射走时联合层析浅中深层速度建模技术避免了常规建模方法中浅层速度模型与中深层速度模型的融合问题,较好地解决了传统成像域反射层析对近地表模型的不可控更新问题,整体提升了深度域浅中深层速度模型的建模精度,进而提高了复杂地表、复杂构造区的地震成像质量.  相似文献   

7.
立体层析成像是一种新的地震反射波层析成像方法,能为叠前深度偏移提供较为精确的宏观速度模型。本文研究了立体层析成像的实现方法,包括斜率与走时数据的拾取、离散速度模型构建和初始化、射线参数的确定、斜率和走时及射线计算以及反演问题解法等,建立立体层析成像的算法流程。并通过对Marmousi模型试验,对立体层析成像运行所需的主要参数,如初始速度模型、拾取数据量、离散网格尺寸、速度平滑权重等进行测试和分析,总结这些不同参数对立体层析反演结果的影响规律,用以指导生产实践。  相似文献   

8.
Reflection tomography is the industry standard tool for velocity model building, but it is also an ill‐posed inverse problem as its solution is not unique. The usual way to obtain an acceptable result is to regularize tomography by feeding the inversion with some a priori information. The simplest regularization forces the solution to be smooth, implicitly assuming that seismic velocity exhibits some degree of spatial correlation. However, velocity is a rock property; thus, the geometry and structure of rock formations should drive correlation in velocity depth models. This observation calls for constraints driven by geological models. In this work, we present a set of structural constraints that feed reflection tomography with geometrical information. These constraints impose the desired characteristics (flatness, shape, position, etc.) on imaged reflectors but act on the velocity update. Failure to respect the constraints indicates either velocity inaccuracies or wrong assumptions concerning the constraints. Reflection tomography with structural constraints is a flexible framework that can be specialized in order to achieve different goals: among others, to flatten the base of salt bodies or detachment surfaces, to recover the horizontalness of oil–water contacts, or to impose the co‐location of the same imaged horizon between PP and PS images. The straightforward application of structural constraints is that of regularizing tomography through geological information, particularly at the latest stages of the depth imaging workflow, when the depth migration structural setting reached a consistent geological interpretation. Structural constraints are also useful in minimizing the well‐to‐seismic mis‐ties. Moreover, they can be used as a tool to check the consistency of interpreters' hypothesis with seismic data. Indeed, inversion with structural constraints will preserve image focusing only if the interpreters' insights are consistent with the data. Results from synthetic and real data demonstrate the effectiveness of reflection tomography with structural constraints.  相似文献   

9.
高级  张海江 《地球物理学报》2016,59(11):4310-4322
在利用不同的地球物理勘探方法对地下复杂介质成像时,因观测系统的非完备性及数据本身对某些岩石物性的不敏感性,单独成像的结果存在较大的不确定性和不一致性.对于地震体波走时成像与直流电阻率成像,均面临着成像阴影区问题.对于地震走时成像,地震射线对低速区域覆盖较差形成阴影区,造成低速区域分辨率降低.对于电阻率成像,电场线在高阻区域分布较少,造成高阻区域分辨率较低.为了提高地下介质成像的精度,Gallado和Meju(2003)提出了基于交叉梯度结构约束的联合地球物理成像方法.在要求不同的物性模型拟合各自对应的数据同时,模型之间的结构要求一致,即交叉梯度趋于零.为了更有效地实现基于交叉梯度的结构约束,我们提出了一种新的交替结构约束的联合反演流程,即交替反演不同的数据而且在反演一种数据时要求对应的模型与另一个模型结构一致.新的算法能够更容易地把单独的反演系统耦合在一起,而且也更容易建立结构约束和数据拟合之间的平衡.基于新的联合反演流程,我们测试了基于交叉梯度结构约束的二维跨孔地震走时和直流电阻率联合成像.合成数据测试表明,我们提出的交替结构约束流程能够很好地实现基于交叉梯度结构约束的联合成像.与单独成像结果相比,地震走时和全通道电阻率联合成像更可靠地确定了速度和电阻率异常.  相似文献   

10.
针对鄂尔多斯盆地西缘黄土塬区复杂地表和复杂地下构造导致难以准确成像问题,采用浅层潜水波层析反演(DWT)速度建模技术,同时辅以中深层反射波层析成像技术,形成一套实用叠前深度偏移速度建模方法。首先生成一个基于钻井和解释信息的起始近地表速度,其次利用潜水波层析反演建立初始近地表模型,将其与常规处理获得的中深层速度模型进行匹配拼接,建立起初始的起伏地表全速度模型,然后在此基础上利用基于反射波的网格层析进行中深层速度建模,经过多轮次迭代,最终获得可靠的高精度速度模型。鄂尔多斯盆地西缘MJT工区地震资料的成像处理验证了这一套速度建模技术的有效性,地下构造成像更合理也更精确。   相似文献   

11.
A method is presented for deriving 1-D velocity depth models from earthquake bulletin data. The models can be used as initial models for more advanced modelling techniques such as tomographic inversion. The method is useful when there is little or no refraction and long-range reflection survey data. The bulletin travel times are subjected to an analysis of variance, where they are separated into source, distance, and receiving station terms. The distance terms describe the variation of travel time with distance, and the associated trend lines allow 1-D velocity models for the crustal layers to be determined. The velocity models provide an average crustal model for the region derived from local data. This does not include superficial layers which are necessarily poorly determined. Earthquake bulletin P-wave data from propagation paths across three different regions of the UK are employed to illustrate the use of the technique.  相似文献   

12.
多层介质中利用sPn与Pn到时差确定震源深度的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
王瑶  万永革 《地震工程学报》2021,43(6):1294-1302
为利用sPn与Pn波的走时差测定震源深度,进一步提高地震震源深度的测定精度,推导多层介质下sPn与Pn波的走时差与震源深度的关系,发现走时差与震中距无关,只与震源深度及区域地壳速度模型有关。震源在同一层中,走时差曲线的斜率不变,而当震源位于不同层中时,sPn-Pn走时差曲线的斜率不同,并呈分段直线的走时差曲线形态。地壳速度结构纵向越不均匀,多层和单层介质下利用sPn-Pn走时差计算的震源深度误差就越大,走时曲线的各分段直线斜率相差越大;探讨地壳中sPn与Pn波传播路径相同但波速不同的单层地壳速度模型,发现单层介质下波速越大,测定的震源深度越大;对于同一地区相同的地壳分层结构,测得的震源深度随着泊松比的增大而减小。基于前人给出的中国五个典型块体多层平均地壳模型,给出sPn-Pn走时差与震源深度计算公式速查表。  相似文献   

13.
Certain degree of smoothness of velocity models is required for most ray‐based migration and tomography. Applying conventional smoothing in model parameters results in offset‐dependent travel‐time errors for reflected events, which can be large even for small contrasts in model parameters between the layers. This causes the shift in both the depth and residual moveout of the migrated images. To overcome this problem in transversely isotropic medium with a vertical symmetry axis, the preserved travel‐time smoothing method was proposed earlier. We extend this method for orthorhombic media with and without azimuthal variation between the layers. We illustrate this method for a single interface between two orthorhombic layers and show that the smoothing‐driven errors in travel time are very small for practical application.  相似文献   

14.
初至波走时层析反演技术作为建立近地表速度模型的重要手段,是解决陆地资料复杂静校正问题的关键技术。而折射波广泛发育的海洋地震资料,对折射波信息的关注与运用并没有得到广泛的重视。本文首次将层析反演方法应用于海洋拖缆地震数据的近海底速度模型的建立。本文方法与陆地资料层析反演的主要区别在于:①在震源信号的最小相位化处理后进行初至时间的拾取,避免了混合相位子波初至拾取不准带来的误差;②以海水深度与海水速度作为反演约束条件,减小了迭代误差。实测二维资料的层析反演结果表明,本文方法可反演出较为精确的海洋地层速度结构。   相似文献   

15.
邓超云 《中国地震》2020,36(2):359-366
近年来,远震走时层析成像方法有了长足的发展,在地下结构反演的研究中获得了众多成果。针对射线在台站下方覆盖率较差而导致远震反演方法对地壳速度约束不足的问题,本文提出了一种新的地壳异常体改正方法——对同一台站的相对走时残差进行求和平均去均值,消除了地壳中复杂的速度异常体对上地幔速度结构反演的干扰,反演结果具有更优的相对走时残差分布,同时反演得到的速度模型具有更小的数据方差。  相似文献   

16.
射线追踪方法是研究地震波在横向非均匀地壳介质中传播的重要方法.本文推导了理论走时对网格化节点速度的偏导数公式,提出了针对深地震宽角反射/折射剖面数据反演的联合迭代法,并使用该方法对横跨龙门山断裂带中段的一条深地震宽角反射/折射剖面进行了反演和解释.首先,对每一炮的观测数据进行一维反演,在此基础上插值出一个粗略的二维速度模型;然后,使用射线追踪方法计算理论走时,再根据理论走时与观测走时的拟合程度对二维模型进行调整,以获得更加接近实际的二维速度模型;最后,利用联合迭代法对观测走时进行反演,经反复迭代使所有接收点理论走时与实测走时的残差平方和最小,最终获取该剖面的二维地壳速度结构.反演结果表明:测线东段的沉积盖层明显厚于中段褶皱带和西部高原,中部褶皱带部分地区出现基岩裸露;构造转换带两侧的地层分界面近于水平层状分布,其西侧的中、下地壳内各存在一个层间速度间断面;构造转换带内存在薄厚不等的低速层,自西向东有增厚趋势.此外,龙门山断裂带的3条主断裂向下深切结晶基底,这是由于西部松潘—甘孜地块自西向东运动,受到刚性扬子地块的阻挡,沿铲式断裂向上爬升所致;而在断层上盘距地表约15 km深处出现的最大剪应力极值区,正是发生汶川MS8.0地震的震源位置.   相似文献   

17.
本文应用层析成像反演方法优化叠前深度偏移速度模型。阐述叠前深度偏移速度建模流程,详细介绍利用两种不同层析反演方法来优化深度域的层速度模型,对同一实际地震资料速度模型建立的应用效果表明,在资料信噪比较高的地区能提供准确解释层位信息的前提下,模型层析反演优化后的速度模型精度要比网格层析反演优化后的速度模型更高,且稳定性强。   相似文献   

18.
使用阻尼最小二乘法进行震源参数和地壳三维速度结构的走时联合反演.所用资料为S波和P波到时差,并用人工地震资料的二维解释结果作为三维速度模型的特定约束条件.为建立初始模型,又利用天然地震构成了准二维剖面.在走时反演基础上,利用遗传算法进行了几个地震事件的波形反演尝试,并对走时反演获得的地壳速度结构模型的局部进行了修正.以34°~42°N,94°~112°E作为研究区域,在该区域中收集了1986年以来大量地震的S波和P波到时差资料,7条人工地震二维速度剖面资料和2个数字化地震台的几个地震的三分向记录资料.对这些资料进行了处理,最后得出了0~25km深度不同截面的速度分布,并对所得结果进行了分析.  相似文献   

19.
本文从误差解析公式及数值模拟计算两种途径讨论了利用常用地方震相Pg,Sg,PmP,Pn,sPL测定震源深度的误差问题,结果表明,两种途径获取的误差值相当。对于上地壳的地震而言,当直达波走时误差处于0.1 s的量级时,若要将误差控制在3 km左右,则应选用震中距为30 km以内的台站;当走时误差处于0.2 s的量级时,若要控制同等误差,则应选用震中距为20 km以内的台站;如果地震位于下地壳,震中距可适当放宽,然而当震中距更大或走时误差更大时,震源深度的误差则近乎成倍增长。PmP,Pn,sPL对上地壳的震源深度测定误差要小于下地壳,同时对误差的控制较好,不会随震中距的增大而快速增大,震中距处于90 km范围以内且走时误差小于0.1 s时的深度误差基本均能控制在3.5 km以内。此外,本文还通过“棋盘格”的方式定量地分析了速度扰动对走时的影响,并以首都圈地区台网布局为基础,分析了加入首波对震源深度测定的改善效果。这两项数值对比结果均表明,在2%的速度扰动下,只要下地壳和莫霍面的速度参数不同时出现过大或过小现象,加入首波后对震源深度的测定误差则基本能控制在3 km以内,且一致性明显地高于单独使用直达波。   相似文献   

20.
In areas of complex geology such as the Canadian Foothills, the effects of anisotropy are apparent in seismic data and estimation of anisotropic parameters for use in seismic imaging is not a trivial task. Here we explore the applicability of common‐focus point (CFP)‐based velocity analysis to estimate anisotropic parameters for the variably tilted shale thrust sheet in the Canadian Foothills model. To avoid the inherent velocity‐depth ambiguity, we assume that the elastic properties of thrust‐sheet with respect to transverse isotropy symmetry axis are homogeneous, the reflector below the thrust‐sheet is flat, and that the anisotropy is weak. In our CFP approach to velocity analysis, for a poorly imaged reflection point, a traveltime residual is obtained as the time difference between the focusing operator for an assumed subsurface velocity model and the corresponding CFP response obtained from the reflection data. We assume that this residual is due to unknown values for anisotropy, and we perform an iterative linear inversion to obtain new model parameters that minimize the residuals. Migration of the data using parameters obtained from our inversion results in a correctly positioned and better focused reflector below the thrust sheet. For traveltime computation we use a brute force mapping scheme that takes into account weakly tilted transverse isotropy media. For inversion, the problem is set up as a generalized Newton's equation where traveltime error (differential time shift) is linearly dependent on the parameter updates. The iterative updates of parameters are obtained by a least‐squares solution of Newton's equations. The significance of this work lies in its applicability to areas where transverse isotropy layers are heterogeneous laterally, and where transverse isotropy layers are overlain by complex structures that preclude a moveout curve fitting.  相似文献   

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