求解波动方程的任意差分精细积分法

在地震偏移成像技术中，常常要反向外推波场，因此涉及到波动方程的数值求解问题。本文提出了一种求解偏微分方程的新的半解析方法——任意差分精细积分(ADPI)法。其大体思路是：空间域上作坐标离散，但不采用古典差分法的等分离散方式，而是一种相对自由的、任意的离散法；时间域上则采用子域精细积分的方法，既保留了精细积分法的高精度，又克服了工作量大、占用存储大等缺点。该方法具有精度高、带宽小、稳定性好等多项突出优点，并且可以灵括处理各类边界条件。本文从简单一维、较普遍一维、以及二维3种情形讨论该方法对波动方程的具体应用，结合实际的算例，详细分析了各种算法的可行性和精度特点。     

高精度有限差分地震波正演方法

三维地震模拟不仅可以更精确地研究地震波的传播规律,而且是三维地震资料处理和解释的工具。本文采用精细积分法用于求解波动方程.对波动方程在空间采用差分格式,时间域采用积分法求解析的方法。文中详细论述了精细积分法的数值方法,并给出了计算公式。理论分析和数值算例的结果表明了用这种混合方法得到的解与精确解十分吻合,比有限差分法具有更高的精度。文中给出的地震波正演模拟算例说明了该方法适用于复杂地表和复杂构造地质体。     

基于精细积分法的三维弹性波数值模拟(英文)

波动方程有限差分法是地震数值模拟中的一种重要的方法,对理解和分析地震传播规律、分析地震属性和解释地震资料有着非常重要的意义。但是有限差分法由于其离散化的思想,产生了不稳定性。精细积分法在有限差分法的基础上,在时间域采用解析解的表达形式,在空间域保留任意差分格式,发展成为半解析的数值方法。本文结合并发展了以往学者的成果,推导了任意精细积分法的三维弹性波正演模拟计算公式,并对其稳定性进行了数值分析。在计算实例中,实现了精细积分法二维和三维弹性波模型的地震正演模拟,对计算结果的分析表明,精细积分法反射信号走时准确,稳定性好,弹性波场相较于声波波场,弹性波波场成分更为丰富,包含了更多波型成分(PP-和PS-反射波、透射波和绕射波),这对实际地震资料的解释和储层分析有重要的意义。实践证明,该方法可直接应用到弹性波的地质模型的数值模拟中。     

基于双差定位法的鄂尔多斯块体西北缘地震精定位研究

针对鄂尔多斯块体西北缘地震活动的复杂性及目前台网定位方法存在偏差的问题,采用双差定位法对2009—2019年发生在鄂尔多斯块体西北缘的地震事件进行重新定位.经研究表明,双差定位之后地震分布更集中,鄂尔多斯块体西缘的地震沿银川吉兰泰断陷带分布,北缘的地震沿河套断陷带分布,地震定位精度明显提高,这与块体周缘复杂的地质构造背...     

塔里木地区勘探地震正演模拟研究

以塔里木前陆盆地地质背景为模型,采用三维任意差分精细积分方法并行算法实现了库车地区三维正演模拟.三维任意差分精细积分方法通过时间域采用局部积分半解析方法求得波动方程的递推算子,与常规的差分法相比计算精度有较大提高;文中计算稳定性根据实际算例进行分析,采用稳定因子约束,得到较好的稳定性;边界条件采用改进的自适应吸收边界,并通过串行程序并行化,大大减少了三维正演模拟的耗时,完成了大数据量三维正演模拟.     

频率波数域内层状地基动力柔度的精细求解

精细积分法既可得到在计算机精度意义下的精确解,又能够保持哈密顿体系的辛结构。其是求解一阶线性常微分方程组的精确数值方法,既可以用于时间域的初值问题,又可以应用于空间域的两点边值问题。运用精细积分法求解微层区段矩阵,并对微层区段矩阵合并得到整个层状地基的区段矩阵,最终得到层状地基的动力柔度值。运用数值算例验证了本文方法的计算精度。     

基于紧凑存储的任意四边形网格有限元法地震波场数值模拟

采用有限元法精确模拟复杂介质条件下的地震波场,一般采用三角单元,但在节点数相同的情况下,三角单元的计算精度不如矩形单元高,采用三角单元模拟复杂界面时,编制确定结构刚度矩阵非零元素位置的程序也较为麻烦。采用矩形单元离散含有倾斜或起伏界面的地质模型时,无法避免绕射噪声,若加密网格又会增加计算量。为此,本文基于任意四边形单元模拟声波的传播,在倾斜或起伏界面条件下,可以有效避免因离散引起的“阶梯状”界面,在不增加计算量以及内存占用的前提下,有效地消除离散绕射噪声。采用对角的集中质量矩阵代替一致质量矩阵,避免矩阵的求逆运算,从而提高显式有限元法的计算效率;对结构刚度矩阵采用紧凑存储格式,每一行需要存储的元素最多为5个,同时零元素不参与运算,既减少内存的占用,又极大地提高计算效率。     

基于波动方程的微地震震源位置、震源时间及VTI介质各向异性参数联合反演

对于非常规油气开发,水力压裂监控的效果取决于对微地震事件的分析、解释.准确的微地震震源位置是关乎施工成败的重要因素.微地震震源位置的准确性与多个参数相关,其不仅依赖于微地震事件的激发时间,同时也依赖于储层介质参数信息,因此进行微地震震源位置、震源时间、储层介质参数的联合反演尤为重要.页岩气储层通常表现出较强的各向异性,...     

Perfectly matched layer boundary conditions for frequency-domain acoustic wave simulation in the mesh-free discretization

Mesh-free discretization, flexibly distributing nodes without computationally expensive meshing process, is able to deal with staircase problem, oversampling and undersampling problems and saves plenty of nodes through distributing nodes suitably with respect to irregular boundaries and model parameters. However, the time-domain mesh-free discretization usually exhibits poorer stability than that in regular grid discretization. In order to reach unconditional stability and easy implementation in parallel computing, we develop the frequency-domain finite-difference method in a mesh-free discretization, incorporated with two perfectly matched layer boundary conditions. Furthermore, to maintain the flexibility of mesh-free discretization, the nodes are still irregularly distributed in the absorbing zone, which complicates the situation of artificial boundary reflections. In this paper, we implement frequency-domain acoustic wave modelling in a mesh-free system. First, we present the perfectly matched layer boundary condition to suppress spurious reflections. Moreover, we develop the complex frequency shifted–perfectly matched layer boundary condition to improve the attenuation of grazing waves. In addition, we employ the radial-basis-function-generated finite difference method in the mesh-free discretization to calculate spatial derivatives. The numerical experiment on a rectangle homogeneous model shows the effectiveness of the perfectly matched layer boundary condition and the complex frequency shifted–perfectly matched layer boundary condition, and the latter one is better than the former one when absorbing large angle incident waves. The experiment on the Marmousi model suggests that the complex frequency shifted–perfectly matched layer boundary condition works well for complicated models.     

Lebedev scheme for the numerical simulation of wave propagation in 3D anisotropic elasticity‡

This paper presents a Lebedev finite difference scheme on staggered grids for the numerical simulation of wave propagation in an arbitrary 3D anisotropic elastic media. The main concept of the scheme is the definition of all the components of each tensor (vector) appearing in the elastic wave equation at the corresponding grid points, i.e., all of the stresses are stored in one set of nodes while all of the velocity components are stored in another. Meanwhile, the derivatives with respect to the spatial directions are approximated to the second order on two‐point stencils. The second‐order scheme is presented for the sake of simplicity and it is easy to expand to a higher order. Another approach, widely‐known as the rotated staggered grid scheme, is based on the same concept; therefore, this paper contains a detailed comparative analysis of the two schemes. It is shown that the dispersion condition of the Lebedev scheme is less restrictive than that of the rotated staggered grid scheme, while the stability criteria lead to approximately equal time stepping for the two approaches. The main advantage of the proposed scheme is its reduced computational memory requirements. Due to a less restrictive dispersion condition and the way the media parameters are stored, the Lebedev scheme requires only one‐third to two‐thirds of the computer memory required by the rotated staggered grid scheme. At the same time, the number of floating point operations performed by the Lebedev scheme is higher than that for the rotated staggered grid scheme.     

盐丘模型 推覆体模型 波动方程 叠前深度偏移

三维波动方程叠前深度偏移是复杂介质中进行构造成像、弹性参数反演的重要环节.由于其技术实现不仅涉及波场延拓理论的创新,而且需要大规模计算,因而研究难度较大. 本文以实验效果的取得为目的,完整地实现了SEG/EAEG盐丘和推覆体模型的三维波动方程辛几何算法的叠前深度偏移成像计算. 文中详细考察了所研制的波动方程三维叠前深度偏移软件系统及其对复杂地质构造的成像能力. 具体包括：1）对于盐丘模型,文中讨论了成像参数的选择、地震子波对成像精度的影响、完成二维及三维叠前深度偏移的比较;2）对推覆体模型,文中进行了脉冲响应测试;3）由两个模型的成像结果可见本文的波动方程三维叠前深度偏移软件系统已具有适应强速度横向变化、复杂构造的成像能力.