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CN114200541B - Three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraint - Google Patents

Three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraint Download PDF

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CN114200541B
CN114200541B CN202111459209.0A CN202111459209A CN114200541B CN 114200541 B CN114200541 B CN 114200541B CN 202111459209 A CN202111459209 A CN 202111459209A CN 114200541 B CN114200541 B CN 114200541B
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张镕哲
李桐林
邓馨卉
何浩源
康鑫泽
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Jilin University
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Abstract

一种基于余弦点积梯度约束的三维重磁联合反演方法,包括基于几何格架法的重力、重力梯度和磁法三维正演快速算法;依据余弦定理推导出三维余弦点积梯度函数,基于截断高斯牛顿法的三维联合反演算法,该方法既能避免存储雅克比矩阵,又能减少共轭梯度法求解线性方程时正演计算的次数。在传统重力和磁法数据中又加入了全张量重力梯度数据,能够进一步改善重磁联合反演的分辨能力;将上述正演、结构耦合方式以及联合反演算法相结合应用于重力、重力梯度和磁法数据中,充分发挥三方面的优势,有效地改善三维重磁联合反演的计算效率、内存消耗和分辨能力。

Figure 202111459209

A 3D gravity-magnetism joint inversion method based on cosine dot product gradient constraints, including gravity, gravity gradient and magnetic method 3D forward modeling fast algorithm based on geometric grid method; 3D cosine dot product gradient function is derived based on the law of cosines, based on A three-dimensional joint inversion algorithm of the truncated Gauss-Newton method, which can not only avoid storing the Jacobian matrix, but also reduce the number of forward calculations when the conjugate gradient method is used to solve linear equations. The full tensor gravity gradient data is added to the traditional gravity and magnetic method data, which can further improve the resolution ability of the gravity-magnetic joint inversion; In the gradient and magnetic method data, the advantages of the three aspects are fully utilized to effectively improve the calculation efficiency, memory consumption and resolution ability of the 3D gravity-magnetic joint inversion.

Figure 202111459209

Description

一种基于余弦点积梯度约束的三维重磁联合反演方法A 3D Gravity-Magnetic Joint Inversion Method Based on Cosine Dot Product Gradient Constraint

技术领域technical field

本发明涉及一种三维重磁数据联合反演的处理技术领域,特别提出了一种基于余弦点积梯度约束的高精度高效率三维重磁联合反演方法。The invention relates to the processing technical field of a joint inversion of three-dimensional gravity and magnetic data, and particularly proposes a high-precision and high-efficiency three-dimensional gravity and magnetic joint inversion method based on cosine dot product gradient constraints.

背景技术Background technique

随着勘探目标越来越深,勘探环境越来越复杂,单凭一种地球物理数据很难精准地推测出地下目标体的属性信息,多种地球物理方法综合解释势必会成为地球物理勘探发展的重要趋势,而联合反演是多种地球物理方法综合解释的有效方法之一,是降低反演多解性、提高多种数据利用率和改善反演模型结构不一致等问题的有效手段。交叉梯度联合反演不依赖于先验岩石物性关系,且不需要对初始模型做出任何假设,是一种灵活有效的联合反演方法,该方法已经应用到两种或多种地球物理方法中。然而,交叉梯度函数直接将不同数量级和单位的模型参数进行叉乘,只考虑梯度方向是否平行,忽略了不同模型参数梯度幅值对不同区域交叉梯度约束权重的影响,以及三维情况下需要计算多个分量增加了计算复杂性。因此,如何构建不同地球物理模型参数之间的耦合关系,以及如何提高联合反演的精度和效率是目前联合反演研究的关键所在。As the exploration target gets deeper and the exploration environment becomes more and more complex, it is difficult to accurately infer the attribute information of the underground target body based on a single geophysical data. Joint inversion is one of the effective methods for comprehensive interpretation of multiple geophysical methods, and it is an effective means to reduce inversion multi-solutions, improve the utilization of multiple data, and improve the inconsistency of inversion model structures. The cross-gradient joint inversion does not depend on the prior petrophysical relationship, and does not need to make any assumptions about the initial model. It is a flexible and effective joint inversion method, which has been applied to two or more geophysical methods. . However, the cross-gradient function directly cross-multiplies model parameters of different orders of magnitude and units, only considering whether the gradient directions are parallel, ignoring the influence of different model parameter gradient amplitudes on the cross-gradient constraint weights of different regions, and the need to calculate more in three-dimensional cases. components increase the computational complexity. Therefore, how to construct the coupling relationship between parameters of different geophysical models, and how to improve the accuracy and efficiency of joint inversion are the key points of joint inversion research.

发明内容Contents of the invention

本发明的目的在于提供一种基于余弦点积梯度约束的高精度高效率三维重磁联合反演方法,以解决现有的重磁联合反演计算速度慢、内存消耗大等问题。The purpose of the present invention is to provide a high-precision and high-efficiency three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraints, so as to solve the problems of slow calculation speed and large memory consumption of the existing gravity-magnetic joint inversion.

如图1所示,本发明包括如下步骤:As shown in Figure 1, the present invention comprises the following steps:

1)输入重力、重力梯度和磁法的观测数据,输入密度和磁化强度的初始模型和参考模型,期望拟合差和最大迭代次数;1) Input the observed data of gravity, gravity gradient and magnetic method, input the initial model and reference model of density and magnetization, expected fitting difference and maximum number of iterations;

2)构建基于余弦点积梯度约束的三维重磁联合反演目标函数Φg(mg)和Φκ(mκ);2) Construct the 3D gravity-magnetic joint inversion objective functions Φ g (m g ) and Φ κ (m κ ) based on cosine dot product gradient constraints;

3)计算正则化因子和结构约束权重因子;3) Calculate the regularization factor and the structural constraint weight factor;

4)计算重磁数据协方差矩阵、模型积分灵敏度矩阵、聚焦加权矩阵、以及计算余弦点积梯度函数及其雅克比矩阵;4) Calculate the gravity and magnetic data covariance matrix, model integral sensitivity matrix, focus weighting matrix, and calculate the cosine dot product gradient function and its Jacobian matrix;

5)利用截断高斯牛顿法对余弦点积梯度约束的三维重磁联合反演目标函数优化求解,获得密度和磁化强度模型更新量;5) Using the truncated Gauss-Newton method to optimize and solve the objective function of the three-dimensional gravity-magnetic joint inversion constrained by the gradient of the cosine dot product, and obtain the update amount of the density and magnetization model;

6)计算密度和磁化强度更新模型的正演响应,并求解重磁方法每次迭代的拟合差,如果每种方法都满足期望拟合差或者达到最大迭代次数,则联合反演迭代结束。6) Calculate the forward modeling response of the density and magnetization update model, and solve the fitting difference of each iteration of the gravity and magnetic method. If each method meets the expected fitting difference or reaches the maximum number of iterations, the joint inversion iteration ends.

本发明的有益效果:Beneficial effects of the present invention:

1、本发明的余弦点积梯度函数,在三维情况下不需要计算多个分量,简化了计算传统交叉梯度函数的复杂性和提高了结构耦合的计算效率。同时,避免模型参数数量级和量纲差异带来的计算影响,更适合于大数据量三维多参数联合反演计算。1. The cosine dot product gradient function of the present invention does not need to calculate multiple components in a three-dimensional case, which simplifies the complexity of calculating traditional cross gradient functions and improves the calculation efficiency of structural coupling. At the same time, it avoids the calculation impact caused by the magnitude and dimension differences of model parameters, and is more suitable for large-scale three-dimensional multi-parameter joint inversion calculations.

2、本发明的截断高斯牛顿法是高斯牛顿法和共轭梯度法的结合体,该方法应用于联合反演中既能避免存储雅克比矩阵,又可以大大的减少正演计算次数,能够有效地改善三维重磁联合反演的计算效率和内存消耗。2. The truncated Gauss-Newton method of the present invention is a combination of the Gauss-Newton method and the conjugate gradient method. When this method is applied to the joint inversion, it can avoid storing the Jacobian matrix, and can greatly reduce the number of forward calculations, which can effectively The computational efficiency and memory consumption of 3D gravity-magnetic joint inversion can be greatly improved.

3、本发明在传统重力和磁法数据中又加入了全张量重力梯度数据,能够进一步改善重磁联合反演的分辨能力。3. The present invention adds full tensor gravity gradient data to the traditional gravity and magnetic method data, which can further improve the resolving power of gravity-magnetic joint inversion.

附图说明Description of drawings

图1为基于余弦点积梯度约束的三维重磁联合反演方法流程图;Figure 1 is a flow chart of the three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraints;

图2为三维地下网格剖分示意图;Figure 2 is a schematic diagram of three-dimensional underground grid division;

图3为密度和磁化强度理论模型示意图;Fig. 3 is the schematic diagram of density and magnetization theoretical model;

图4为三维重磁反演密度模型示意图;Figure 4 is a schematic diagram of a three-dimensional gravity and magnetic inversion density model;

图5为三维重磁反演磁化强度模型示意图。Fig. 5 is a schematic diagram of a three-dimensional gravity and magnetic inversion magnetization model.

具体实施方式Detailed ways

如图1所示,一种基于余弦点积梯度约束的三维重磁联合反演方法,包括如下步骤:As shown in Figure 1, a 3D gravity-magnetic joint inversion method based on cosine dot product gradient constraints includes the following steps:

1)输入重力、重力梯度和磁法的观测数据,输入密度和磁化强度的初始模型和参考模型,期望拟合差和最大迭代次数;1) Input the observed data of gravity, gravity gradient and magnetic method, input the initial model and reference model of density and magnetization, expected fitting difference and maximum number of iterations;

2)构建基于余弦点积梯度约束的三维重磁联合反演目标函数Φg(mg)和Φκ(mκ);2) Construct the 3D gravity-magnetic joint inversion objective functions Φ g (m g ) and Φ κ (m κ ) based on cosine dot product gradient constraints;

3)计算正则化因子和结构约束权重因子;3) Calculate the regularization factor and the structural constraint weight factor;

4)计算重磁数据协方差矩阵、模型积分灵敏度矩阵、聚焦加权矩阵、以及计算余弦点积梯度函数及其雅克比矩阵;4) Calculate the gravity and magnetic data covariance matrix, model integral sensitivity matrix, focus weighting matrix, and calculate the cosine dot product gradient function and its Jacobian matrix;

5)利用截断高斯牛顿法对余弦点积梯度约束的三维重磁联合反演目标函数优化求解,获得密度和磁化强度模型更新量;5) Using the truncated Gauss-Newton method to optimize and solve the objective function of the three-dimensional gravity-magnetic joint inversion constrained by the gradient of the cosine dot product, and obtain the update amount of the density and magnetization model;

6)计算密度和磁化强度更新模型的正演响应,并求解重磁方法每次迭代的拟合差,如果每种方法都满足期望拟合差或者达到最大迭代次数,则联合反演迭代结束。6) Calculate the forward modeling response of the density and magnetization update model, and solve the fitting difference of each iteration of the gravity and magnetic method. If each method meets the expected fitting difference or reaches the maximum number of iterations, the joint inversion iteration ends.

步骤1)中,输入重力、重力梯度和磁法的观测数据,观测数据通过建立密度和磁化强度理论模型计算正演响应获得。In step 1), the observation data of gravity, gravity gradient and magnetic method are input, and the observation data are obtained by establishing a theoretical model of density and magnetization to calculate the forward response.

步骤2)中,构建基于余弦点积梯度约束的三维重磁联合反演目标函数如下:In step 2), the objective function of the 3D gravity-magnetic joint inversion based on the cosine dot product gradient constraint is constructed as follows:

Figure BDA0003387544240000041
Figure BDA0003387544240000041

Figure BDA0003387544240000042
Figure BDA0003387544240000042

其中,Cdg为重力及重力梯度观测数据dg的数据协方差矩阵;C为磁法观测数据dκ的数据协方差矩阵;Cmg和C分别为密度mg和磁化强度mκ的模型协方差矩阵,mgref和mκref为参考模型,设置为上一次迭代得到的模型;λg,λκ,βg和βg为权重因子;fg(mg)和fκ(mκ)分别表示为重力及重力梯度和磁法的正演响应,td(mg,mκ)为余弦点积梯度函数表达式如下:Among them, C dg is the data covariance matrix of gravity and gravity gradient observation data d g ; C is the data covariance matrix of magnetic observation data d κ ; C mg and C are the density m g and magnetization m κ respectively Model covariance matrix, m gref and m κref are reference models, set to the model obtained in the last iteration; λ g , λ κ , β g and β g are weighting factors; f g (m g ) and f κ (m κ ) are respectively the forward modeling response of gravity and gravity gradient and magnetic method, and t d (m g ,m κ ) is the cosine dot product gradient function. The expression is as follows:

Figure BDA0003387544240000043
Figure BDA0003387544240000043

其中,ε为很小的常数,

Figure BDA0003387544240000044
Figure BDA0003387544240000045
为密度和磁化强度模型梯度,|·|为范数。Among them, ε is a very small constant,
Figure BDA0003387544240000044
and
Figure BDA0003387544240000045
is the density and magnetization model gradient, |·| is the norm.

步骤3)中,计算正则化因子和结构约束权重因子。In step 3), the regularization factor and structural constraint weight factor are calculated.

设置初始正则化因子λg=0.1;λκ=0.001。随着迭代的增加,模型约束项可能会增加,为了确保目标函数的收敛在全区最小,此时需要修正正则化因子,表达式如下:Set initial regularization factors λ g =0.1; λ κ =0.001. With the increase of iterations, the model constraints may increase. In order to ensure that the convergence of the objective function is the smallest in the whole area, the regularization factor needs to be corrected at this time. The expression is as follows:

Figure BDA0003387544240000046
Figure BDA0003387544240000046

Figure BDA0003387544240000047
Figure BDA0003387544240000047

为了保障联合反演迭代收敛,我们会在拟合差增大或拟合差变化缓慢时,按比例减小正则化因子:In order to ensure the iterative convergence of the joint inversion, we will reduce the regularization factor proportionally when the fitting difference increases or the fitting difference changes slowly:

Figure BDA0003387544240000051
Figure BDA0003387544240000051

其中,k为迭代次数,q为缩放因子,设q=0.6;Among them, k is the number of iterations, q is the scaling factor, set q=0.6;

结构约束权重因子计算表达式如下:The calculation expression of structural constraint weight factor is as follows:

Figure BDA0003387544240000052
Figure BDA0003387544240000052

Figure BDA0003387544240000053
Figure BDA0003387544240000053

其中,Cg和Cκ为密度和磁化强度结构约束的加权系数。where C g and C κ are weighting coefficients for density and magnetization structural constraints.

步骤4)中,计算重磁数据协方差矩阵、模型积分灵敏度矩阵、聚焦加权矩阵、以及计算余弦点积梯度函数及其雅克比矩阵;In step 4), calculate the gravity and magnetic data covariance matrix, model integral sensitivity matrix, focus weighting matrix, and calculate the cosine dot product gradient function and its Jacobian matrix;

数据协方差矩阵为重力、重力梯度和磁法数据噪声误差对角逆矩阵,没有噪声干扰时,表示为单位对角矩阵。聚焦矩阵的计算表达式如下:The data covariance matrix is the inverse diagonal matrix of the noise error of gravity, gravity gradient and magnetic method data. When there is no noise interference, it is expressed as a unit diagonal matrix. The calculation expression of the focusing matrix is as follows:

Ws=(m22)(-1/2) (9)W s =(m 22 ) (-1/2) (9)

模型积分灵敏度矩阵表达式如下:The model integral sensitivity matrix expression is as follows:

Figure BDA0003387544240000054
Figure BDA0003387544240000054

其中,A为雅克比矩阵。Among them, A is the Jacobian matrix.

余弦点积梯度函数计算表达式如下:The calculation expression of the cosine dot product gradient function is as follows:

Figure BDA0003387544240000055
Figure BDA0003387544240000055

其中,ηg和ηκ为归一化算子,模型参数mg和mκ的第二个下角标c、b、d和r分别表示三维网格不同位置的单元,Δx,Δy,Δz表示为不同方向网格单元间距离,如图2所示。Among them, η g and η κ are normalization operators, the second subscripts c, b, d and r of the model parameters m g and m κ represent the units at different positions of the three-dimensional grid respectively, and Δx, Δy, Δz represent is the distance between grid cells in different directions, as shown in Figure 2.

余弦点积梯度函数的雅克比矩阵表达式如下:The Jacobian matrix expression of the cosine dot product gradient function is as follows:

Figure BDA0003387544240000061
Figure BDA0003387544240000061

其中,Bg和Bκ分别余弦点积梯度约束函数对密度和磁化强度的偏导数,即雅克比矩阵。Among them, B g and B κ are the partial derivatives of the cosine dot product gradient constraint function with respect to density and magnetization, respectively, namely the Jacobian matrix.

步骤5)中,利用截断高斯牛顿法对余弦点积梯度约束的三维重磁联合反演目标函数优化求解,获得密度和磁化强度模型更新量如下:In step 5), the truncated Gauss-Newton method is used to optimize and solve the objective function of the three-dimensional gravity-magnetic joint inversion constrained by the gradient of the cosine dot product, and the updated quantities of the density and magnetization models are obtained as follows:

Figure BDA0003387544240000062
Figure BDA0003387544240000062

Figure BDA0003387544240000063
Figure BDA0003387544240000063

其中,k为迭代次数,

Figure BDA0003387544240000064
Ag和Aκ为重磁正演响应雅克比矩阵。Among them, k is the number of iterations,
Figure BDA0003387544240000064
A g and A κ are Jacobian matrices of gravity and magnetic forward modeling responses.

公式(13)和(14)不直接求解,而是利用共轭梯度法近似求解高斯牛顿迭代线性方程,并通过一个强迫项来控制求解的精度,强迫项表达式如下:Formulas (13) and (14) are not solved directly, but the Gauss-Newton iterative linear equation is approximated by using the conjugate gradient method, and the accuracy of the solution is controlled by a forcing term. The expression of the forcing term is as follows:

Figure BDA0003387544240000065
Figure BDA0003387544240000065

Figure BDA0003387544240000066
Figure BDA0003387544240000066

步骤6)中,计算密度和磁化强度更新模型的正演响应,并求解重磁方法每次迭代的拟合差;In step 6), the forward modeling response of the density and magnetization update model is calculated, and the fitting difference of each iteration of the gravity and magnetic method is solved;

通过分析地下模型单元与观测点之间的位置关系,可以发现同一层各模型单元与观测点之间的相对位置关系存在等价性,利用这个等价关系,只对每一层第一个模型单元进行几何格架核函数计算,得到该单元的核函数矩阵,而该层其他模型单元的核函数矩阵可以通过几何格架的等效性进行查找获得,从而快速计算重磁正演响应;拟合差计算的表达式如下:By analyzing the positional relationship between the underground model unit and the observation point, it can be found that there is an equivalence between the relative positional relationship between the model units and the observation point on the same layer. Using this equivalence relationship, only the first model of each layer Calculate the kernel function of the geometric grid to obtain the kernel function matrix of the unit, and the kernel function matrix of other model units in this layer can be obtained by searching the equivalence of the geometric grid, so as to quickly calculate the gravity and magnetic forward modeling response; The expression for calculating the difference is as follows:

Figure BDA0003387544240000067
Figure BDA0003387544240000067

其中,d为观测数据,f为正演响应,N为观测点个数。如果每种方法都满足期望拟合差或者达到最大迭代次数,则联合反演迭代结束。Among them, d is the observation data, f is the forward modeling response, and N is the number of observation points. If each method meets the expected poor fit or reaches the maximum number of iterations, the joint inversion iteration ends.

下面对本发明提供的基于余弦点积梯度约束的三维重磁联合反演方法进行验证。The three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraints provided by the present invention is verified below.

如图3所示,建立了一个双异常体组合模型;模型中包含了两个大小相同埋深不同的异常体,两个异常体的大小为200m×200m×200m,剩余密度为1g/cm3和磁化强度为1A/m。地下模型空间尺度x,y,z为1000m×1000m×600m,将地下模型剖分为20×20×12个紧密排列的规则立方体单元,每个单元大小为50m×50m×50m,背景剩余密度为0g/cm3,背景磁化强度为0.001A/m,地面观测点个数为20×20,观测点位于网格中心。As shown in Figure 3, a double anomalous body combination model is established; the model includes two anomalous bodies with the same size and different buried depths, the size of the two anomalous bodies is 200m×200m×200m, and the residual density is 1g/cm 3 and a magnetization of 1A/m. The spatial scale x, y, z of the underground model is 1000m×1000m×600m, the underground model is divided into 20×20×12 closely arranged regular cubic units, each unit size is 50m×50m×50m, and the residual density of the background is 0g/cm 3 , the background magnetization is 0.001A/m, the number of ground observation points is 20×20, and the observation points are located in the center of the grid.

首先,对比重力和磁法单独反演和联合反演结果,验证余弦点积梯度联合反演算法的有效性。然后,在重磁联合反演中加入重力梯度数据进行余弦点积梯度联合反演计算,验证算法的分辨能力和计算效率。上述所有方法均在截断高斯牛顿法的框架下开展,初始模型均设为均匀半空间0g/cm3的剩余密度模型和0.001A/m的磁化强度模型。First, the effectiveness of the cosine dot product-gradient joint inversion algorithm is verified by comparing the results of gravity and magnetic inversion alone and joint inversion. Then, the gravity gradient data is added to the gravity-magnetic joint inversion to carry out the cosine dot product gradient joint inversion calculation to verify the resolution ability and calculation efficiency of the algorithm. All the above methods are carried out under the framework of the truncated Gauss-Newton method, and the initial model is set as the residual density model of the uniform half space 0g/cm 3 and the magnetization model of 0.001A/m.

重力和磁法数据的单独反演结果如图4(a,b,c)和图5(a,b,c)所示。可以发现,重力单独反演密度模型无法恢复出深部异常体的几何轮廓和物性参数值,而磁化强度模型能够较好恢复异常体的几何形态和物性参数值。当加入余弦点积梯度结构约束条件时,重力和磁法数据联合反演结果(图4d,e,f和图5d,e,f)能有效地改善密度模型的分辨率,尤其密度模型深部异常体明显恢复出了异常体的几何形态,并且异常体物性参数值也接近于真实值,相比于单独反演,余弦点积梯度联合反演获得了结构一致性更好的密度和磁化强度模型。最后,又加入重力梯度数据,进行重力、重力梯度和磁法数据的三维余弦点积梯度约束联合反演计算,密度和磁化强度模型如图(4g,h,l)和图(5g,h,l)所示,由于数据量的增加密度模型得到了进一步的改善,与真实密度模型更加吻合,尤其受到余弦点积梯度结构约束的作用,获得了与磁化强度结构一致性更高的模型;同时,本算例计算耗时约为217.5s,最大内存消耗约为0.117GB。相比于传统重磁三维联合反演算法,本发明提出的算法是一种高效率、高分辨率的联合反演算法。The separate inversion results of gravity and magnetic data are shown in Fig. 4(a,b,c) and Fig. 5(a,b,c). It can be found that the gravity inversion density model alone cannot restore the geometric profile and physical parameter values of the deep anomaly, while the magnetization model can better restore the geometric shape and physical parameter values of the anomalous body. When the cosine dot product gradient structure constraints are added, the joint inversion results of gravity and magnetic data (Fig. 4d, e, f and Fig. 5d, e, f) can effectively improve the resolution of the density model, especially the deep anomaly of the density model The geometry of the anomalous body is obviously restored, and the physical parameter values of the anomalous body are also close to the real values. Compared with the single inversion, the cosine dot product gradient joint inversion obtains a density and magnetization model with better structural consistency. . Finally, the gravity gradient data is added to carry out the joint inversion calculation of the three-dimensional cosine dot product gradient constraints of gravity, gravity gradient and magnetic method data. The density and magnetization models are shown in (4g,h,l) and (5g,h, As shown in l), due to the increase in the amount of data, the density model has been further improved, and it is more consistent with the real density model, especially due to the constraints of the cosine dot product gradient structure, a model with higher consistency with the magnetization structure has been obtained; at the same time , the calculation time of this example is about 217.5s, and the maximum memory consumption is about 0.117GB. Compared with the traditional gravity-magnetic three-dimensional joint inversion algorithm, the algorithm proposed by the present invention is a high-efficiency, high-resolution joint inversion algorithm.

Claims (3)

1. A three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraint is characterized by comprising the following steps: the method comprises the following steps:
1) Inputting observation data of gravity, gravity gradient and a magnetic method, inputting an initial model and a reference model of density and magnetization intensity, and expecting a fitting difference and a maximum iteration number;
2) Construction of three-dimensional gravity-magnetic joint inversion target function phi based on cosine dot product gradient constraint g (m g ) And phi κ (m κ );
3) Calculating a regularization factor and a structural constraint weight factor;
4) Calculating a weight magnetic data covariance matrix, a model integral sensitivity matrix, a focusing weighting matrix, and calculating a cosine dot product gradient function and a Jacobian matrix thereof;
5) Utilizing a truncated gauss-newton method to carry out optimization solution on a three-dimensional gravity-magnetic joint inversion target function constrained by cosine dot product gradient, and obtaining the updating amount of a density and magnetization intensity model;
6) Calculating forward response of the density and magnetization updating model, solving fitting difference of each iteration of the gravity and magnetization method, and finishing joint inversion iteration if each method meets expected fitting difference or reaches maximum iteration times;
in the step 2), a three-dimensional gravity-magnetic joint inversion target function based on cosine dot product gradient constraint is constructed as follows:
Figure FDA0004035923540000011
Figure FDA0004035923540000012
wherein, C dg For gravity and gravity gradient observation data d g The data covariance matrix of (a); c For magnetic observation of data d κ The data covariance matrix of (a); c mg And C Respectively is density m g And magnetization m κ Model covariance matrix of (1), m gref And m κref Setting the model obtained by the last iteration as a reference model; lambda [ alpha ] g And λ κ As a regularization factor, beta g And beta g Constraining the weight factor for the structure; f. of g (m g ) And f κ (m κ ) Expressed as the forward response of gravity and gravity gradient and magnetism, respectively, t d (m g ,m κ ) The cross gradient function is a cosine dot product gradient function, a plurality of components do not need to be calculated under the three-dimensional condition, the complexity of calculating the traditional cross gradient function is simplified, and the calculation efficiency of structural coupling is improved; meanwhile, the calculation influence caused by the magnitude order of the model parameters and the dimension difference is avoided, and the method is more suitable for large-data-volume three-dimensional multi-parameter joint inversion calculation; the cosine dot product gradient function is expressed as follows:
Figure FDA0004035923540000021
where, epsilon is a very small constant,
Figure FDA0004035923540000022
and
Figure FDA0004035923540000023
is the density and magnetization model gradient, | · | is a norm;
in step 3), the constraint weight factors of the gravity and magnetic structure are obtained by an adaptive method, and the updating expression of the constraint weight factors of the gravity and magnetic structure in each iteration is as follows:
Figure FDA0004035923540000024
Figure FDA0004035923540000025
wherein, C g And C κ Weighting coefficients for density and magnetization;
in step 4), the cosine dot product gradient function calculation expression is as follows:
Figure FDA0004035923540000026
wherein eta is g And η κ For normalization operator, model parameter m g And m κ The second lower corner marks c, b, d and r respectively represent the units at different positions of the three-dimensional grid, and Δ x, Δ y and Δ z represent the distances between grid units in different directions;
the calculation of the three-dimensional cosine dot product gradient function Jacobian matrix is more complex compared with two-dimensional calculation, each row of non-zero elements of the Jacobian matrix B is changed into eight elements from six elements, and the expression is as follows:
Figure FDA0004035923540000031
wherein, B g And B κ The partial derivatives of the cosine dot product gradient constraint function with respect to density and magnetization, respectively.
2. The three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraint according to claim 1, characterized in that:
in the step 5), solving the joint inversion by using the traditional Gauss-Newton method needs to occupy a large amount of memory space to store the Jacobian matrix; the truncated gauss-newton method is a combination of the gauss-newton method and a conjugate gradient method, each iteration is performed with an external cycle and an internal cycle, the external cycle adopts the gauss-newton method to calculate a coefficient matrix and a right-end term, the internal cycle approximately solves a gauss-newton iteration linear equation by using the conjugate gradient method, and the accuracy of the solution is controlled by a forcing term; the method not only avoids storing the Jacobian matrix, but also can greatly reduce forward calculation times, and can further improve the calculation efficiency and memory consumption when being applied to three-dimensional gravity-magnetic joint inversion with cosine dot product gradient constraint; the coerced expression is as follows:
Figure FDA0004035923540000032
Figure FDA0004035923540000033
wherein min is expressed as the minimum value, k is the iteration number, A g And A κ Is a gravity magnetic forward response Jacobian matrix,
Figure FDA0004035923540000034
3. the three-dimensional gravity-magnetic joint inversion method based on cosine dot product gradient constraint according to claim 1, characterized in that:
in the step 6), a geometric grid method is used for carrying out three-dimensional forward calculation on gravity, gravity gradient and a magnetic method, so that forward calculation time can be greatly reduced; meanwhile, the forward modeling needs to be solved for multiple times by truncating the internal cycle of the Gauss-Newton method, so that the calculation efficiency of the three-dimensional gravity-magnetic joint inversion can be improved from the three aspects of the forward modeling, the coupling mode and the inversion by combining the geometric lattice method with the truncating Gauss-Newton method and the cosine dot product gradient structure constraint.
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