扩展的倾斜角和倾斜角总水平导数方法     

王明  郭志宏  骆遥  罗锋 《地球物理学进展》2013,28(3)

为了突出显示重磁场中地质体分布、断裂构造特征等信息,使图像显示错落有序、层次分明、清楚直观,有利于解释人员从不同角度认识重磁场异常特征.本文通过分析倾斜角概念,根据反余切函数特性,提出了扩展的倾斜角(iTdr)和倾斜角总水平导数(iTdr_Thdr)方法,来增强重磁异常信息,突出异常形状特点,以便于识别重磁异常中地质体边界和提取地质体分布、断裂构造平面展布特征等信息.理论模型和实际资料对比分析表明该方法简单、实用、具有较好的识别效果和较高的分辨能力,能够获取丰富的地质信息,对识别地质体边界、划分大地构造单元、确定断裂带和地质构造走向等具有实际意义.  相似文献   

基于CLG光学流和波场分解的逆时偏移角度道集提取方法研究     

吴成梁  王华忠  冯波  盛燊 《地球物理学报》2021,64(4):1375-1388

角度域共成像点道集是衔接叠前地震数据与储层特征的重要桥梁,对地震偏移成像与储层描述具有重要意义.与克希霍夫偏移和单向波动方程偏移相比,逆时偏移是复杂地区最精确的成像方法.高效稳健地生成逆时偏移角度道集目前仍然是一个挑战.本文主要讨论如何采用光学流方法高效、高质量地提取角度道集.在逆时偏移波场外推过程中,光学流方法可以估计波场传播方向.其中Lucas-Kanade(LK)和Horn-Schunck(HS)方法是光学流方法中两种典型的方法.LK光学流方法是一种局部方法,该方法依赖于局部点的梯度值,但是容易出现奇异现象,HS光学流方法属于全局方法,波场方向估计依赖于整个波场,易受噪声影响,对异常值比较敏感,导致整体波场方向计算精度不高.本文提出采用局部和整体结合(Combining Local and Global,CLG)的光学流方法估计波场传播方向.该方法可以有效地提高波场方向的精度,并且简单高效,便于并行处理.对比HS光学流方法,CLG光学流方法几乎不增加额外的计算量.另外,为了弱化光学流方法无法处理波前重叠问题,本文利用解析波场和方向滤波对波场进行方向分解,仅需波场的空间傅里叶变换即可实现任意波场方向分解,将分解后的波场分别估计波场反向,提取成像结果.进一步地,在估计反射张角和方位角时,本文提出有效的归一化方法和改进的最小二乘除法,提高角度估计的精度和稳定性.最后,理论和实际资料例证了本文提出方法的有效性.  相似文献   

河系几何相似性的层次度量方法     

杨飞  王中辉 《地球信息科学学报》2021,23(12):2139-2150

已有的线群目标几何相似性度量方法主要基于数理统计的思想,通过统计整体变化信息计算几何相似性,缺少对局域特征的表达,并不适用于具有高度分形特征的河系。为此,本文将河系几何特征划分为3层次的信息特征：单条河流的形状特征、局部区域的结构特征、全局范围的分布特征。首先,结合角链码法与Hausdorff距离计算单条河流的形状相似度;然后,根据 “二八定律”确定局部特征区域,通过坐标系转换计算M： N的河系局域结构相似度;最后综合整体描述子得到全局分布相似度,并在该基础上,构建差异指标进行河系多尺度相似性计算与综合质量评价。实验表明,该方法的计算结果优于均值指标法,能有效应用于制图综合的质量评价。  相似文献   

Wide‐azimuth angle gathers for anisotropic wave‐equation migration     

Paul Sava  Tariq Alkhalifah 《Geophysical Prospecting》2013,61(1):75-91

Extended common‐image‐point gathers (CIP) constructed by wide‐azimuth TI wave‐equation migration contain all the necessary information for angle decomposition as a function of the reflection and azimuth angles at selected locations in the subsurface. The aperture and azimuth angles are derived from the extended images using analytic relations between the space‐ and time‐lag extensions using information which is already available at the time of migration, i.e. the anisotropic model parameters. CIPs are cheap to compute because they can be distributed in the image at the most relevant positions, as indicated by the geologic structure. If the reflector dip is known at the CIP locations, then the computational cost can be reduced by evaluating only two components of the space‐lag vector. The transformation from extended images to angle gathers is a planar Radon transform which depends on the local medium parameters. This transformation allows us to separate all illumination directions for a given experiment, or between different experiments. We do not need to decompose the reconstructed wavefields or to choose the most energetic directions for decomposition. Applications of the method include illumination studies in complex areas where ray‐based methods fail, and assuming that the subsurface illumination is sufficiently dense, the study of amplitude variation with aperture and azimuth angles.  相似文献   

弹性矢量波成像域联合层析反演          下载免费PDF全文

秦宁  李振春  张凯  杨晓东 《地球物理学报》2013,56(9):3109-3117

在地震弹性矢量波场框架下,推导了多波联合层析速度反演方程以及走时残差与角道集剩余曲率的转换关系式,提出了一种利用成像域角道集更新P波、S波速度的走时层析反演方法.其实现过程可以概括为:将弹性波多分量数据作为输入,基于高斯束实现矢量波场成像并提取角道集,利用层析反演方程求解慢度更新量,最终获得多波联合反演结果.模型试算和实际资料处理验证了该方法的反演效果,能够为弹性矢量波联合深度偏移提供高质量的叠前速度场.  相似文献   

波动方程叠前深度偏移直接产生角道集          下载免费PDF全文

刘礼农  张辉  张剑锋 《地球物理学报》2013,56(9):3124-3133

基于单程波深度延拓算法,得到震源波场在成像点的入射角度,结合对地层倾角的估计,获得入射地震波与界面法线的夹角.通过运用"保幅"的反褶积成像条件和考虑累加的炮数,解决了炮点覆盖不均匀导致的成像幅值误差问题,进而建议了炮域波动方程叠前深度偏移直接产生角道集的方法和流程.与基于空间移动或时移成像条件的波动方程叠前深度偏移提取角道集的方法相比,本文建议的方法只需少量额外的存储空间,又可补偿观测系统非均匀覆盖对成像幅值的影响;其增加的计算量与炮域偏移算法相比几乎可以忽略.文中算例表明,本文方法提取的角道集可为叠前反演提供较精确的AVO振幅特性.此外,就改善地震成像效果本身而言,提取角道集使得可在波动方程叠前深度偏移中应用剩余动校和拉伸切除技术,从而可更好地保持高频成分并提高成像的信噪比.  相似文献   

河谷地形的地震反应分析   总被引：1，自引：0，他引：1  

盛志强  卢育霞  石玉成  刘琨  万秀红 《地震工程学报》2013,35(1):126-132202

震害现象显示在一些覆盖层很薄的基岩河谷山区地震动分布差异明显.为了厘清各形状要素的均质地形模型对地震动特性的影响,侧重分析了河谷坡角、坡高及不对称坡体等要素对均质体河谷模型的地震动(PGA)的影响.研究结果表明:河谷地形谷底内部的地面运动幅值在坡角40°～50°范围内达到最大值;在高坡角的河谷内波衰减比较慢,波形相对较复杂;在深宽比较小时,高频和低频脉冲的地面加速度峰值都呈现同样的变化趋势,且谷底地面各个位置PGA变化不明显,随着深宽比的增加,高频脉冲的地震反应变化复杂,出现谷底中心加速度幅值大于山脚;河谷的不对称形状对谷底PGA有影响,谷底PGA最大的位置靠近坡高小的一侧,且坡角大的一侧山脚附近谷底PGA要小一些,即坡度和高差越大,会很大程度地增加河谷两侧坡体的临空面,并增大地震加速度的放大系数,凸起地形对地震响应有放大作用,对它附近区域却有抑制作用,而且坡高、坡角越大,抑制作用越明显.  相似文献   

基于Chebyshev多项式的非对称走时Kirchhoff叠前时间偏移角道集求取          下载免费PDF全文

刘志远  常旭  刘伊克  王一博  杜向东 《地球物理学报》2013,56(8):2783-2789

地震射线走时的求取方法是叠前时间偏移研究的核心问题之一,也是影响计算时间域角道集角度精确性的关键因素之一.本文基于Kirchhoff叠前时间偏移,应用第一类切比雪夫多项式,对弯曲射线对称走时加以改进,引进非对称项,优化后得到切比雪夫非对称走时方程,与高精度走时进行比较和误差分析,再将该走时求取方法应用于时间域角道集的求取中,得到地下较真实的入射角.通过模型计算和实际地震资料处理证明,此种非对称走时及其角道集的求取方法具有精度高、计算量少的优点.  相似文献   

Nature and onset age of neotectonic regime in the northern core of Isparta Angle,SW Turkey     

Ali Koçyiğit  Şule Gürboğa  Doğan Kalafat 《Geodinamica Acta》2013,26(1-2):52-85

The Isparta Angle (IA) is a reverse Λ-shaped morphotectonic structure located to the north of Antalya Gulf in the Eastern Mediterranean Sea. It resulted from the northward curvature of the originally E–W-trending Tauride orogenic belt owing to the nappe emplacements and related clockwise and anti-clockwise rotations in a time period of Early Paleocene to Early Pliocene. The IA is included in the southwest Anatolian tensional neotectonic domain and characterized by a series of grabens and horsts bounded by active normal faults of dissimilar length and trend. The evolutionary history of the graben-horst system is episodic. It is evidenced by two graben fills. These are older and modern (younger) graben fills separated by an intervening angular unconformity. The modern graben fill is nearly flat-lying (non-deformed) whereas older graben fill was deformed into a series of anticlines and synclines with ENE-trending curvi-linear axes by a short-term compressive tectonic regime operated in NNW–SSE direction during Late Pliocene. The diagnostic structures taking a part in the development of grabens and shaping the northern section of the IA are the margin-boundary normal faults. They occur in numerous single and several fault zones displaying a basin ward facing step-like land shape. Most of fault segments, particularly the master faults, are active and have a capacity of creating destructive earthquakes with a magnitude (up to Mw?=?7.0). This is evidenced by both the historical and instrumental period earthquakes. Both the focal mechanism solution of earthquakes and the stereographic plots of slip-plane data, measured on the active margin-boundary faults of various grabens comprising the IA, on the Schmidt lower hemisphere net obviously reveal that the IA is under the influence of the tensional neotectonic regime, not a compressive tectonic regime, i.e. the sinistral strike-slip shearing along the Pliny arc has not propagated yet onshore, and its commencement age is Early Quaternary.  相似文献   

Geometry of scour hole around, and the influence of the angle of attack on the burial of finite cylinders under combined flows     

Yovanni A. Catao-Lopera  Marcelo H. García 《Ocean Engineering》2007,34(5-6):856-869

Experiments were conducted to investigate the geometry of the scour hole and flow structure around short cylinders under the action of waves alone (WA) and combined flows (CF). The study is aimed at better understanding the dynamics of isolated objects on a sandy floor under oscillatory flows as occurs in shallow water regions in coastal areas. Flow velocities within the fluid core were recorded and 3D mapping of the bottom was performed with sub-aquatic acoustic sensors. Experiments were conducted for cylinder Reynolds wave number and Keulegan-Carpenter number within the ranges 10⁴R_e1.7×10⁵ and 2KC71, respectively. The present experimental evidence shows that the geometric characteristics of the scour hole (length and width) depend primarily on the Keulegan-Carpenter number (KC) and the cylinder aspect ratio (a_r=L_c/D). The effect of variation in the angle of attack of the flow with respect to the cylinder main axis was also investigated. Initial orientations of zero and ninety degrees were found to be stable while cylinders with intermediate initial orientations tended to orientate their main axes perpendicular to the flow direction. The final angle of orientation was found to be primarily a function of the Shields parameter, θ, and the initial angle of attack, α_i.  相似文献