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CN114966874A - A Synthesis Method of Frequency Domain Electromagnetic Method Time Series Data Based on Forward Modeling - Google Patents

A Synthesis Method of Frequency Domain Electromagnetic Method Time Series Data Based on Forward Modeling Download PDF

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CN114966874A
CN114966874A CN202210250539.7A CN202210250539A CN114966874A CN 114966874 A CN114966874 A CN 114966874A CN 202210250539 A CN202210250539 A CN 202210250539A CN 114966874 A CN114966874 A CN 114966874A
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陈小斌
王培杰
张赟昀
刘钟尹
蔡军涛
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Abstract

The invention is suitable for the technical field of electromagnetic sounding, and provides a forward-modeling-based method for synthesizing time series data of a frequency domain electromagnetic method, which comprises the following steps: step 1: performing electromagnetic forward calculation in a frequency domain to obtain field intensity values of a plurality of frequencies; step 2: segmenting the time sequence of each frequency, and calculating to obtain a field value which changes along with time; and step 3: synthesizing the segmented time sequences of each frequency, and splicing the segmented time sequences; and 4, step 4: and overlapping the spliced time series of each frequency to form complete time series data and outputting the complete time series data. By adopting the time sequence synthesis technology, time sequences corresponding to forward modeling results of various theoretical models can be synthesized. The result of the geoelectromagnetic method calculation shows that the time sequence obtained by synthesis meets the basic characteristics of the frequency domain electromagnetic method, and the processing result of the signal is completely consistent with the model response.

Description

一种基于正演的频率域电磁法时间序列数据的合成方法A Synthesis Method of Frequency Domain Electromagnetic Method Time Series Data Based on Forward Modeling

技术领域technical field

本发明属于电磁测深技术领域,涉及一种基于正演的频率域电磁法时间序列数据的合成方法。The invention belongs to the technical field of electromagnetic sounding, and relates to a method for synthesizing time series data based on a forward modeling frequency domain electromagnetic method.

背景技术Background technique

频率域电磁法(Frequency Domain Electromagnetic Method)是一系列利用天然源和人工源的频率域电磁场研究地球内部电性结构的地球物理方法的统称,包括大地电磁测深法(Magnetotelluric,MT)、音频大地电磁测深法(Audio Magnetotelluric,AMT)、可控源音频大地电磁测深法(Controlled Source Audio Magnetotelluric,CSAMT)等。Frequency Domain Electromagnetic Method (Frequency Domain Electromagnetic Method) is a general term for a series of geophysical methods that use the frequency domain electromagnetic fields of natural and artificial sources to study the electrical structure of the earth's interior, including magnetotelluric (MT), audio geodetic methods. Electromagnetic bathymetry (Audio Magnetotelluric, AMT), Controlled Source Audio Magnetotelluric bathymetry (Controlled Source Audio Magnetotelluric, CSAMT) and so on.

其基本原理是:依据不同频率的电磁波在导电媒质中具有不同趋肤深度的原理,在地表测量由高频至低频的天然源(人工源)的电磁场响应序列,经过相关的资料处理来获得大地由浅至深的电性结构。它有不受高阻层屏蔽、对高导层分辨能力强,横向分辨能力较强等优点,也有纵向分辨能力随着深度增加而迅速减弱等缺点。其主要步骤是:数据采集、数据处理、反演解释。The basic principle is: According to the principle that electromagnetic waves of different frequencies have different skin depths in conductive media, the electromagnetic field response sequence of natural sources (artificial sources) from high frequency to low frequency is measured on the surface, and the earth is obtained through relevant data processing. Electrical structure from shallow to deep. It has the advantages of not being shielded by high-resistance layers, strong ability to distinguish high-conductivity layers, and strong lateral resolution. The main steps are: data acquisition, data processing, inversion interpretation.

频率域电磁法采集得到电磁场的时间序列,需要先通过傅里叶变换得到频率域场值,才能进行下一步处理解释,电磁场时间序列易受干扰影响,从而影响后续数据处理和解释的准确性。现有数据处理方法亟需理论时间序列数据作为标准进行检验。当前频率域电磁法内各种去噪方法蓬勃发展,但对于不同数据,各种处理方法的效果不尽相同,同一数据不同方法处理结果也不一样,需要寻找一个合理的方法建立标准数据来检验各种数据处理方法的处理效果。在不同的频率域电磁法中,有些方法的信号对其他方法而言是噪声。例如线源信号,在可控源电磁法中是信号,而在天然源的大地电磁法中是噪声。本技术可以同时合成天然源和人工源的信号,因此可以用于信噪分离技术的研究。The time series of the electromagnetic field collected by the frequency domain electromagnetic method needs to be obtained by Fourier transform to obtain the frequency domain field value before the next step of processing and interpretation. The electromagnetic field time series is easily affected by interference, which affects the accuracy of subsequent data processing and interpretation. Existing data processing methods urgently need theoretical time series data to be tested as a standard. At present, various denoising methods in the frequency domain electromagnetic method are booming, but for different data, the effects of various processing methods are not the same, and the processing results of different methods for the same data are also different. It is necessary to find a reasonable method to establish standard data to test The processing effect of various data processing methods. In different frequency domain electromagnetic methods, the signal of some methods is noise to other methods. For example, a line source signal is a signal in the controlled source electromagnetic method, but is noise in the natural source magnetotelluric method. This technology can simultaneously synthesize natural and artificial signals, so it can be used for the research of signal-to-noise separation technology.

发明内容SUMMARY OF THE INVENTION

本发明实施例的目的在于提供一种基于正演的频率域电磁法时间序列数据的合成方法,旨在模拟频率域电磁法的时间序列信号,模拟各种噪声的影响特征,为研究电磁法时间域、频率域和空间上的分布特征和传播规律,提供技术支撑。对于不同数据,各种处理方法的效果不尽相同,同一数据不同方法处理结果也不一样,本发明可以合理地建立标准数据来检验各种数据处理方法的处理效果。The purpose of the embodiments of the present invention is to provide a method for synthesizing time series data based on the frequency domain electromagnetic method based on forward modeling, which aims to simulate the time series signal of the frequency domain electromagnetic method, and simulate the influence characteristics of various noises, so as to study the electromagnetic method time series. The distribution characteristics and propagation laws in the domain, frequency domain and space provide technical support. For different data, the effects of various processing methods are not the same, and the processing results of the same data by different methods are also different. The present invention can reasonably establish standard data to test the processing effects of various data processing methods.

本发明实施例是这样实现的,一种基于正演的频率域电磁法时间序列数据的合成方法,包括以下步骤:The embodiments of the present invention are implemented in this way, a method for synthesizing time series data based on a forward modeling frequency domain electromagnetic method, comprising the following steps:

步骤1:进行频率域电磁法正演计算,得到若干个频率的场强值;Step 1: Perform forward calculation of frequency domain electromagnetic method to obtain field strength values of several frequencies;

步骤2:对每一频率的时间序列分段,计算得到随时间变化的场值;Step 2: Segment the time series of each frequency, and calculate the field value that changes with time;

步骤3:合成每个频率的分段时间序列,把分段时间序列拼接起来;Step 3: Synthesize the segmented time series of each frequency, and splicing the segmented time series together;

步骤4:把每个频率的拼接时间序列叠加,形成完整的时间序列数据并输出。Step 4: Superimpose the spliced time series of each frequency to form complete time series data and output.

进一步的技术方案,所述步骤1的具体步骤包括:Further technical solutions, the specific steps of the step 1 include:

步骤1.1:设计待研究的理论模型;Step 1.1: Design the theoretical model to be studied;

步骤1.2:对于简单模型直接采用解析法求解,对于不能解析求解的复杂模型,按以下步骤进行;Step 1.2: For simple models, use the analytical method to solve them directly. For complex models that cannot be solved analytically, follow the steps below;

步骤1.2.1:对模型进行网格剖分,设计测点,并将测点数记为M;Step 1.2.1: Mesh the model, design measuring points, and record the number of measuring points as M;

步骤1.2.2:根据研究的频段和采样率,设计频率表,共N个频点,记为ω[j],j=1…N;Step 1.2.2: According to the researched frequency band and sampling rate, design a frequency table with a total of N frequency points, denoted as ω[j], j=1...N;

步骤1.2.3:对该模型的每个频点进行频率域电磁法正演计算,得到每个测点处的电磁场值,每个频点都需要正演两次,一次E极化的场源,一次H 极化的场源,正演得到的电场、磁场值为AE[i,j]和AH[i,j],其中上标EH代表正演中E极化和H极化,i=1…M,j=1…N,A∈{Ex,Ey,Hx,Hy,Hz};Step 1.2.3: Perform forward calculation of frequency domain electromagnetic method for each frequency point of the model to obtain the electromagnetic field value at each measurement point. Each frequency point needs to be forward modeled twice, once for the E-polarized field source , the field source of primary H polarization, the electric field and magnetic field values obtained by forward modeling are A E [i,j] and A H [i,j], where superscript E and H represent E polarization and H pole in forward modeling , i=1...M, j=1...N, A∈{Ex, Ey, Hx, Hy, Hz};

进一步的技术方案,所述步骤1.2中不限定具体的正演方法,采用针对简单模型的解析法,或者数值模拟方法如有限差分法和有限单元法,或者使用现有开源软件如ModEM等计算,或者使用现有商业软件如COMSOL等计算,从而得到测点处的电磁场值。For a further technical solution, the specific forward modeling method is not limited in the step 1.2, and the analytical method for a simple model, or a numerical simulation method such as the finite difference method and the finite element method, or an existing open source software such as ModEM is used to calculate, Or use existing commercial software such as COMSOL to calculate the electromagnetic field value at the measuring point.

进一步的技术方案,所述步骤2的具体步骤包括:对于每个频率f,将待合成的时间序列切分为多段,每段长度不固定,用于模拟场源随时间的变化。本发明不限定具体的每段长度,可根据具体的研究目标设定。为保证时间序列能完整描述频谱信息,也保证数据处理时能恢复频谱信息,每段长度应大于该频率所对应的一个周期的长度(1/f),若长度太小则视为噪声。本发明的最佳实例中的分段长度为符合高斯分布的随机数,均值设为8/f,方差设为 4/f。随机长度的参数也不固定,为保证合成数据响应稳定,建议均值在4/f 以上。E极化和H极化的分段可以不同,最终时间序列被分为CE段和CH。对每段时间序列,生成随机复数RE[k,j],k=1…CE和RH[k,j],k=1…CH,然后对每个测点计算AE[k,i,j]=AE[i,j]*RE[k,j]和AH[k,i,j]=AH[i,j]*RH,得到各分段的 E极化场值和H极化场值,并计算其振幅|A|和相位

Figure RE-GDA0003657246670000031
使得每段时间序列中的电磁场的强度和极化方向都不同。In a further technical solution, the specific steps of step 2 include: for each frequency f, dividing the time series to be synthesized into multiple segments, and the length of each segment is not fixed, so as to simulate the variation of the field source with time. The present invention does not limit the specific length of each segment, which can be set according to specific research objectives. In order to ensure that the time series can completely describe the spectrum information, and also ensure that the spectrum information can be recovered during data processing, the length of each segment should be greater than the length of a cycle corresponding to the frequency (1/f), and if the length is too small, it is regarded as noise. In the best example of the present invention, the segment length is a random number conforming to a Gaussian distribution, the mean value is set to 8/f, and the variance is set to 4/f. The parameters of random length are also not fixed. In order to ensure the stable response of synthetic data, it is recommended that the average value be above 4/f. The segments of E -polarization and H-polarization can be different, and the final time series is divided into CE segments and CH . For each time series, generate random complex numbers RE [k,j], k=1... C E and RH [k,j], k=1... CH , and then calculate A E [k for each measurement point ,i,j]=A E [i,j]*R E [k,j] and A H [k,i,j]=A H [i,j]*R H , obtain the E pole of each segment and H-polarization field values, and calculate their amplitude |A| and phase
Figure RE-GDA0003657246670000031
The intensity and polarization direction of the electromagnetic field in each time series are different.

进一步的技术方案,所述步骤3的具体步骤为:对于每个频率,利用步骤 2中计算的振幅|A|和相位

Figure RE-GDA0003657246670000032
按照式
Figure RE-GDA0003657246670000033
计算每个分段时间序列,然后把这些分段时间序列收尾相连拼接起来,得到aE(j,t)和aH(j,t) 二者叠加得到a(j,t),计算公式为a(j,t)=aE(j,t)+aH(j,t)。为了减小时间序列拼接产生的信号阶跃,可以在拼接前对每段时间序列进行加窗处理,本发明不限定具体的窗函数,本发明的最佳实例中的使用的是汉宁窗。计算公式为aw(j,t)=a(j,t)*w(j,t),其中w(j,t)为窗函数,aw(j,t)为加窗后的分段时间序列。In a further technical solution, the specific steps of step 3 are: for each frequency, use the amplitude |A| and phase calculated in step 2
Figure RE-GDA0003657246670000032
According to the formula
Figure RE-GDA0003657246670000033
Calculate each segmented time series, and then splicing these segmented time series at the end to obtain a E (j, t) and a H (j, t) The superposition of both to obtain a (j, t), the calculation formula is a(j,t)= aE (j,t) +aH (j,t). In order to reduce the signal step generated by time series splicing, each time series can be windowed before splicing. The present invention does not limit the specific window function, and the Hanning window is used in the best example of the present invention. The calculation formula is a w (j, t)=a(j, t)*w(j, t), where w(j, t) is the window function, and a w (j, t) is the windowed segment sequentially.

进一步的技术方案,所述步骤2和步骤3是一种利用分段拼接,合成极化方向随时间变化的电磁场方法。本技术不限定具体如何实现极化方向的变化。In a further technical solution, the steps 2 and 3 are a method of synthesizing an electromagnetic field in which the polarization direction changes with time by using segmented splicing. The present technology does not limit how to realize the change of the polarization direction.

进一步的技术方案,所述步骤4的具体步骤为:把每个频点对应的拼接时间序列信号叠加得到总的时间序列,计算公式为

Figure RE-GDA0003657246670000041
In a further technical solution, the specific steps of the step 4 are: superimposing the spliced time series signals corresponding to each frequency point to obtain a total time series, and the calculation formula is:
Figure RE-GDA0003657246670000041

本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法,采用本方法所述的时间序列合成技术,合成各种理论模型的时间序列。结果表明合成得到的时间序列满足频率域电磁法信号的基本特征,信号的处理结果与模型响应完全一致。因此本方法合成的时间序列可以作为数据标准,对频率域电磁法数据处理方法研究具有重大意义。The embodiment of the present invention provides a method for synthesizing time series data based on the frequency domain electromagnetic method based on forward modeling, using the time series synthesis technology described in the method to synthesize time series of various theoretical models. The results show that the synthesized time series satisfies the basic characteristics of the frequency domain electromagnetic method signal, and the processing result of the signal is completely consistent with the model response. Therefore, the time series synthesized by this method can be used as the data standard, which is of great significance to the research on the data processing method of the frequency domain electromagnetic method.

附图说明Description of drawings

图1为本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法的大地电磁时间序列信号和频谱;Fig. 1 is a kind of magnetotelluric time series signal and frequency spectrum based on a method for synthesizing time series data of frequency domain electromagnetic method provided by an embodiment of the present invention;

图2为本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法的时间序列合成技术流程图;2 is a flow chart of a time series synthesis technology of a method for synthesizing time series data based on a forward modeling frequency domain electromagnetic method provided by an embodiment of the present invention;

图3为本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法中的一种二维理论模型;FIG. 3 is a two-dimensional theoretical model in a method for synthesizing time series data based on forward modeling based on frequency domain electromagnetic method provided by an embodiment of the present invention;

图4为本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法中的二维模型的网格剖分和测点设计;Fig. 4 is the grid division and measuring point design of a two-dimensional model in a forward modeling-based frequency-domain electromagnetic method time series data synthesis method provided by an embodiment of the present invention;

图5为本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法中的各频点正弦信号及其叠加信号;FIG. 5 is a sinusoidal signal of each frequency point and a superimposed signal thereof in a method for synthesizing time series data based on a forward modeling frequency domain electromagnetic method provided by an embodiment of the present invention;

图6为本发明实施例提供的一种基于正演的频率域电磁法时间序列数据的合成方法合成得到的时间序列和处理结果。FIG. 6 is a time series and a processing result synthesized by a method for synthesizing time series data based on a forward modeling based on a frequency domain electromagnetic method provided by an embodiment of the present invention.

具体实施方式Detailed ways

为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。In order to make the objectives, technical solutions and advantages of the present invention clearer, the present invention will be further described in detail below with reference to the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are only used to explain the present invention, but not to limit the present invention.

以下结合大地电磁法时间序列合成的具体实施例对本发明的具体实现进行详细描述。The specific implementation of the present invention will be described in detail below with reference to specific embodiments of magnetotelluric method time series synthesis.

前提条件:Preconditions:

合成时间序列数据符合天然源大地电磁信号的基本特征,合成数据经过常规数据处理流程处理后得到的阻抗响应和设计模型的理论响应一致,合成数据应与现有实测数据相似,可被成熟的数据处理软件处理,并得到一致的响应。构建理论模型进行正演,合成时间序列,对合成时间序列进行数据处理后对比验证,合成数据的响应与理论响应一致。The synthetic time series data conforms to the basic characteristics of natural magnetotelluric signals. The impedance response obtained after the synthetic data is processed by the conventional data processing process is consistent with the theoretical response of the design model. The synthetic data should be similar to the existing measured data and can be used by mature data. Handle software processing and get a consistent response. Build a theoretical model for forward modeling, synthesize time series, and compare and verify the synthetic time series after data processing. The response of the synthetic data is consistent with the theoretical response.

工作原理:working principle:

本发明所述的利用理论模型的正演响应进行时间序列数据合成的方法,设计理论电性结构模型,采用数值模拟方法(有限差分法、有限单元法等),计算出测点处的频域电磁场响应。In the method for synthesizing time series data using the forward response of the theoretical model, the theoretical electrical structure model is designed, and the numerical simulation method (finite difference method, finite element method, etc.) is used to calculate the frequency domain at the measuring point. Electromagnetic field response.

频率域电磁法研究的是任意单频电磁场信号之间的稳定关系。单频信号都可以被表述为具有一定幅度与相位的正弦信号。某频率的电场和磁场信号可以被写作:The frequency domain electromagnetic method studies the stable relationship between any single frequency electromagnetic field signals. A single frequency signal can be expressed as a sinusoidal signal with a certain amplitude and phase. The electric and magnetic field signals of a certain frequency can be written as:

Figure RE-GDA0003657246670000051
Figure RE-GDA0003657246670000051

式(1)中r为位置矢量,Ae和Ah为振幅,ω为角频率,

Figure RE-GDA0003657246670000052
Figure RE-GDA0003657246670000053
为相位。利用欧拉恒等式e=cos(φ)+isin(φ),其中
Figure RE-GDA0003657246670000054
为虚数单位,式(1)可以被写作:In formula (1), r is the position vector, A e and A h are the amplitudes, ω is the angular frequency,
Figure RE-GDA0003657246670000052
and
Figure RE-GDA0003657246670000053
for the phase. Using Euler's identity e =cos(φ)+isin(φ), where
Figure RE-GDA0003657246670000054
is an imaginary unit, equation (1) can be written as:

Figure RE-GDA0003657246670000055
Figure RE-GDA0003657246670000055

式中

Figure RE-GDA0003657246670000056
表示取实部。现定义复变量:in the formula
Figure RE-GDA0003657246670000056
Represents the real part. Now define a complex variable:

Figure RE-GDA0003657246670000061
Figure RE-GDA0003657246670000061

式(2)可以写作:Equation (2) can be written as:

Figure RE-GDA0003657246670000062
Figure RE-GDA0003657246670000062

时间域电磁法的麦克斯韦方程组为:The Maxwell equations of the time-domain electromagnetic method are:

Figure RE-GDA0003657246670000063
Figure RE-GDA0003657246670000063

式(5)中μ为磁导率,ε为介电常数,σ为电导率,J(r,t)为电流源,其形式与式(3)、式(1)中的电磁场相同,对于天然源的频率域电磁法,该项为0。把式(4)带入式(5)可得单频点的时间域麦克斯韦方程为:In formula (5), μ is the magnetic permeability, ε is the permittivity, σ is the electrical conductivity, and J(r, t) is the current source, and its form is the same as the electromagnetic field in formula (3) and formula (1). Frequency domain electromagnetic method of natural sources, this item is 0. Putting Equation (4) into Equation (5), the Maxwell equation in the time domain of a single frequency point can be obtained as:

Figure RE-GDA0003657246670000064
Figure RE-GDA0003657246670000064

式(6)的求解结果取实部,即为(4)式。根据复数的运算法则:The solution result of formula (6) takes the real part, which is formula (4). According to the arithmetic of complex numbers:

Figure RE-GDA0003657246670000065
Figure RE-GDA0003657246670000065

式(6)中各式子两边同除以etωt,最终可以得到:In formula (6), divide both sides of each formula by e tωt , and finally we can get:

Figure RE-GDA0003657246670000071
Figure RE-GDA0003657246670000071

式(8)是与时间无关的频率域的麦克斯韦方程组,也是频率域电磁法正演所需要求解的方程组。上述推导过程表明,如果按照式(8)计算得到E(r)和H(r),可代入式(3)、式(1)即可得到频率为ω/2π的随时间变化的场强值。由式(8) 计算得到频率为ω/2π的H(r)和E(r)的过程为频率域正演过程,已经非常成熟。正演可以得到有限个(N)频率的电磁场,根据式(1)可以得到各频率随时间变化的场强信号,叠加在一起,就可以得到多频点的频率域电磁场信号:Equation (8) is Maxwell's equations in the time-independent frequency domain, and it is also the equations that need to be solved for the forward modeling of the electromagnetic method in the frequency domain. The above derivation process shows that if E(r) and H(r) are calculated according to Equation (8), the time-varying field strength value with frequency ω/2π can be obtained by substituting into Equation (3) and Equation (1). . The process of obtaining H(r) and E(r) with a frequency of ω/2π by formula (8) is a forward modeling process in the frequency domain, which is very mature. The forward modeling can obtain electromagnetic fields with a finite number (N) of frequencies. According to formula (1), the field strength signals of each frequency varying with time can be obtained. By superimposing them together, the frequency domain electromagnetic field signals of multi-frequency points can be obtained:

Figure RE-GDA0003657246670000072
Figure RE-GDA0003657246670000072

如附图1所示,大地电磁实测时间序列信号(A)和该信号的频谱(B),频谱(B)可以通过式(9)计算得到时间序列(A)。As shown in Figure 1, the measured time series signal (A) of magnetotelluric and the frequency spectrum (B) of the signal, the frequency spectrum (B) can be calculated by formula (9) to obtain the time series (A).

参考附图2所示,本发明的时间序列数据合成流程包括以下步骤:Referring to Figure 2, the time series data synthesis process of the present invention includes the following steps:

步骤一:进行大地电磁正演计算,得到若干个频率的场强值。设计合适的待研究模型(附图3),本发明的模型可以为一维、二维或三维模型,对模型进行网格剖分,设计测点(附图4),记测点数为M。根据研究的频段和采样率,设计频率表,共N个频点,记为ω[j],j=1…N。对该模型每个频点进行正演计算,得到每个测点处的电磁场值,每个频点都需要正演两次,一次E 极化的场源,一次H极化的场源。本发明不限定具体的正演方法,采用解析法、或者数值模拟方法如有限差分法和有限单元法,或者使用现有开源软件如ModEM等计算,或者使用现有商业软件如COMSOL等计算,得到测点处的电磁场值。正演得到的电场、磁场值为AE[i,j]和AH[i,j],其中上标EH代表正演中E极化和H极化这两种极化方式,i=1…M,j=1…N,A∈{Ex,Ey, Hx,Hy,Hz}。Step 1: Carry out the magnetotelluric forward calculation to obtain the field strength values of several frequencies. Design a suitable model to be studied (Fig. 3), the model of the present invention can be a one-dimensional, two-dimensional or three-dimensional model, mesh the model, design measuring points (Fig. 4), and the number of measuring points is M. According to the frequency band and sampling rate studied, a frequency table is designed, with a total of N frequency points, denoted as ω[j], j=1...N. Perform forward calculation for each frequency point of the model to obtain the electromagnetic field value at each measurement point. Each frequency point needs to be forward modeled twice, once for the E-polarized field source and once for the H-polarized field source. The present invention does not limit the specific forward modeling method, and adopts analytical method, or numerical simulation method such as finite difference method and finite element method, or uses existing open source software such as ModEM to calculate, or uses existing commercial software such as COMSOL to calculate, to obtain Electromagnetic field value at the measuring point. The electric field and magnetic field values obtained by the forward modeling are A E [i,j] and A H [i,j], where the superscripts E and H represent the two polarization modes of E polarization and H polarization in the forward modeling, i =1...M, j=1...N, A∈{Ex, Ey, Hx, Hy, Hz}.

步骤二:对每一频率的时间序列分段,计算得到随时间变化的场值。对于每个频率f,将待合成的时间序列切分为多段,每段长度不固定,用于模拟场源随时间的变化。本发明不限定具体的每段长度,可根据具体的研究目标设定。为保证时间序列能完整描述频谱信息,也保证数据处理时能恢复频谱信息,每段长度应大于对应频率1个周期的长度(1/f),若长度太小则视为噪声。本发明的最佳实例中的分段长度为符合高斯分布的随机数,均值设为 8/f,方差设为4/f。随机长度的参数也不固定,为保证合成数据响应稳定,建议均值在4/f以上。E极化和H极化的分段可以不同,最终时间序列被分为 CE段和CH。对每段时间序列,生成随机复数RE[k,j],k=1…CE和RH[k,j],k=1… CH,然后对每个测点计算AE[k,i,j]=AE[i,j]*RE[k,j]和AH[k,i,j]=AH[i,j]*RH,得到各分段的E极化场值和H极化场值,并计算其振幅|A|和相位

Figure RE-GDA0003657246670000081
使得每段时间序列中的电磁场的强度和极化方向都不同。Step 2: Segment the time series of each frequency, and calculate the field value that changes with time. For each frequency f, the time series to be synthesized is divided into multiple segments, and the length of each segment is not fixed, which is used to simulate the variation of the field source with time. The present invention does not limit the specific length of each segment, which can be set according to specific research objectives. In order to ensure that the time series can completely describe the spectrum information, and also ensure that the spectrum information can be recovered during data processing, the length of each segment should be greater than the length of one cycle of the corresponding frequency (1/f), and if the length is too small, it is regarded as noise. In the best example of the present invention, the segment length is a random number conforming to a Gaussian distribution, the mean value is set to 8/f, and the variance is set to 4/f. The parameters of random length are also not fixed. In order to ensure the stable response of synthetic data, it is recommended that the average value be above 4/f. The segments of E -polarization and H-polarization can be different, and the final time series is divided into CE segments and CH . For each time series, generate random complex numbers RE [k,j], k=1... CE and RH [k,j], k=1... CH , and then calculate A E [ k for each measurement point ,i,j]=A E [i,j]*R E [k,j] and A H [k,i,j]=A H [i,j]*R H , obtain the E pole of each segment and H-polarization field values, and calculate their amplitude |A| and phase
Figure RE-GDA0003657246670000081
The intensity and polarization direction of the electromagnetic field in each time series are different.

步骤三:合成每个频率的分段时间序列,把分段时间序列拼接起来。对于每个频率,利用步骤2中计算的振幅|A|和相位

Figure RE-GDA0003657246670000082
按照式
Figure RE-GDA0003657246670000083
计算每个分段时间序列,然后把这些分段时间序列收尾相连拼接起来,得到 aE(j,t)和aH(j,t),二者叠加得到a(j,t),计算公式为a(j,t)=aE(j,t)+aH(j,t)。为了减小时间序列拼接产生的信号阶跃,可以在拼接前对每段时间序列进行加窗处理,本发明不限定具体的窗函数,本发明的最佳实例中的使用的是汉宁窗。计算公式为aw(j,t)=a(j,t)*w(j,t),其中w(j,t)为窗函数,aw(j,t)为加窗后的分段时间序列。Step 3: Synthesize the segmented time series of each frequency, and splicing the segmented time series together. For each frequency, use the amplitude |A| and phase calculated in step 2
Figure RE-GDA0003657246670000082
According to the formula
Figure RE-GDA0003657246670000083
Calculate each segmented time series, and then splicing these segmented time series together to obtain a E (j, t) and a H (j, t), which are superimposed to obtain a (j, t), the calculation formula is a(j,t)= aE (j,t) +aH (j,t). In order to reduce the signal step generated by time series splicing, each time series can be windowed before splicing. The present invention does not limit the specific window function, and the Hanning window is used in the best example of the present invention. The calculation formula is a w (j, t)=a(j, t)*w(j, t), where w(j, t) is the window function, and a w (j, t) is the windowed segment sequentially.

步骤四:把每个频率的拼接时间序列叠加,形成完整的时间序列数据并输出,计算公式为

Figure RE-GDA0003657246670000084
附图4展示的是多个频点的正弦信号叠加。Step 4: Superimpose the spliced time series of each frequency to form a complete time series data and output, the calculation formula is
Figure RE-GDA0003657246670000084
FIG. 4 shows the superposition of sinusoidal signals of multiple frequency points.

如果要合成实测数据格式的时间序列,则需要在步骤三之前,为每道电场磁场添加观测系统响应。观测系统响应是指实际的输入信号进入仪器系统后,记录到的信号会受电道电极距、磁探头自响应、仪器自响应以及信号放大器等影响,这些影响在频率域表现为不同频率振幅缩放和相位提前或者滞后的特征。因此,合成实测数据格式的时间序列之前要定义测点的观测系统,得到观测系统的响应,并在计算各频点电场、磁场信号前添加系统响应。令输入信号为S0(ω),仪器记录信号为S(ω),系统响应为r(ω),则有 S(ω)=S0(ω)r(ω),其中r(ω)为复数,其模为信号经过系统后振幅的放大倍数,相位为信号经过系统后相位的滞后。If you want to synthesize the time series of the measured data format, you need to add the observation system response for each electric field and magnetic field before step 3. The observed system response means that after the actual input signal enters the instrument system, the recorded signal will be affected by the distance between the electrodes of the channel, the self-response of the magnetic probe, the self-response of the instrument, and the signal amplifier. and phase advance or lag characteristics. Therefore, before synthesizing the time series of the measured data format, the observation system of the measurement point should be defined, the response of the observation system should be obtained, and the system response should be added before calculating the electric field and magnetic field signals of each frequency point. Let the input signal be S 0 (ω), the instrument recording signal is S(ω), and the system response is r(ω), then S(ω)=S 0 (ω)r(ω), where r(ω) is Complex number, its modulus is the magnification of the amplitude of the signal after passing through the system, and the phase is the lag of the phase after the signal passes through the system.

附图6(A)某个测点合成得到的时间序列,数据保存为凤凰公式MTU-5A 的时间序列格式,并采用商业软件SSMT2000处理得到的结果对比。经过合成时间序列数据处理的测试,说明了本方法合成的理论时间序列可以处理得到准确的响应,可作为大地电磁时间序列处理技术的研究标准。Fig. 6(A) The time series synthesized by a certain measuring point, the data is saved in the time series format of the Phoenix formula MTU-5A, and the results obtained by processing the commercial software SSMT2000 are compared. The test of synthetic time series data processing shows that the theoretical time series synthesized by this method can be processed to obtain accurate responses, which can be used as the research standard of magnetotelluric time series processing technology.

设计该模型如附图3所示,模型为均匀半空间内含一个矩形异常体,均匀半空间的背景电阻率为100Ω·m,异常体电阻率为10Ω·m,异常体宽10km,厚5km,顶部埋深5km。附图4是该模型网格剖分的核心区域(-20km<X<20km, -40km<Y<0km),核心区域网格向外扩展后,实际模型左右边界分别为-200km 和200km,下边界为-100km,模型最小层厚200m。设计的频率表(共50个频点,频率范围从320Hz至0.00001Hz)用于正演计算。采用有限单元法计算得到每个测点的电磁场值。对每个频点的两个极化方向的时间序列分段,分段长度为高斯分布的随机数,均值设为8/f,方差设为4/f,计算每段的场强值。计算测点A每个频点两个极化方向每段电场、磁场对应的正弦信号。对每段时间序列进行加窗处理,窗函数为汉宁窗。拼接分段时间序列,然后叠加两个极化方向的时间序列形成每个频点的时间序列。把每个频点计算得到的时间域信号叠加在一起,形成包含全部频点信息的时间序列。附图5为测点O 处,Ex、Ey、Hx和Hy前15个的频点对应的正弦曲线(Index=1~15)和叠加曲线(Index=16)。附图6为该点合成的凤凰公司MTU-5A仪器对应的时间序列(A),合成数据采用成熟商业软件SSMT2000处理的结果(B),处理结果与理论响应的对比(C:视电阻率,D:相位)。经过对比发现,结果基本一致,说明本发明的合成数据是正确的。The design of this model is shown in Figure 3. The model is that the uniform half space contains a rectangular abnormal body. The background resistivity of the uniform half space is 100Ω·m, the resistivity of the abnormal body is 10Ω·m, and the abnormal body is 10km wide and 5km thick. , the top is buried at a depth of 5km. Figure 4 shows the core area (-20km<X<20km, -40km<Y<0km) of the mesh division of the model. After the grid of the core area expands outward, the left and right boundaries of the actual model are respectively -200km and 200km. The boundary is -100km, and the minimum layer thickness of the model is 200m. The designed frequency table (50 frequency points in total, frequency range from 320Hz to 0.00001Hz) is used for forward calculation. The electromagnetic field value of each measuring point is calculated by the finite element method. For the time series segments of the two polarization directions of each frequency point, the segment length is a random number of Gaussian distribution, the mean value is set to 8/f, and the variance is set to 4/f, and the field strength value of each segment is calculated. Calculate the sine signal corresponding to each electric field and magnetic field in the two polarization directions of each frequency point of measuring point A. Windowing is performed on each time series, and the window function is Hanning window. Splicing the segmented time series, and then superimposing the time series of the two polarization directions to form the time series of each frequency point. The time domain signals calculated by each frequency point are superimposed together to form a time series containing all frequency point information. Figure 5 shows the sinusoidal curves (Index=1-15) and superimposed curves (Index=16) corresponding to the first 15 frequency points of Ex, Ey, Hx and Hy at the measuring point O. Accompanying drawing 6 is the time series (A) corresponding to the MTU-5A instrument of Phoenix Company synthesized at this point, the synthetic data adopts the result (B) of mature commercial software SSMT2000 processing, the contrast of processing result and theoretical response (C: apparent resistivity, D: Phase). Through comparison, it is found that the results are basically the same, indicating that the synthetic data of the present invention is correct.

以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内所作的任何修改、等同替换和改进等,均应包含在本发明的保护范围之内。The above descriptions are only preferred embodiments of the present invention and are not intended to limit the present invention. Any modifications, equivalent replacements and improvements made within the spirit and principles of the present invention shall be included in the protection of the present invention. within the range.

Claims (7)

1.一种基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,包括以下步骤:1. a frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation, is characterized in that, comprises the following steps: 步骤1:进行频率域电磁法正演计算,得到若干个频率的场强值;Step 1: Perform forward calculation of frequency domain electromagnetic method to obtain field strength values of several frequencies; 步骤2:对每一频率的时间序列分段,计算得到随时间变化的场值;Step 2: Segment the time series of each frequency, and calculate the field value that changes with time; 步骤3:合成每个频率的分段时间序列,把分段时间序列拼接起来;Step 3: Synthesize the segmented time series of each frequency, and splicing the segmented time series together; 步骤4:把每个频率的拼接时间序列叠加,形成完整的时间序列数据并输出。Step 4: Superimpose the spliced time series of each frequency to form complete time series data and output. 2.根据权利要求1所述的基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,所述步骤1的具体步骤包括:2. the frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation according to claim 1, is characterized in that, the concrete steps of described step 1 comprise: 步骤1.1:设计待研究的理论模型;Step 1.1: Design the theoretical model to be studied; 步骤1.2:对于简单模型直接采用解析法求解,对于不能解析求解的复杂模型,按以下步骤进行;Step 1.2: For simple models, use the analytical method to solve them directly. For complex models that cannot be solved analytically, follow the steps below; 步骤1.2.1:对模型进行网格剖分,设计测点,并将测点数记为M;Step 1.2.1: Mesh the model, design measuring points, and record the number of measuring points as M; 步骤1.2.2:根据研究的频段和采样率,设计频率表,共N个频点,记为ω[j],j=1…N;Step 1.2.2: According to the researched frequency band and sampling rate, design a frequency table with a total of N frequency points, denoted as ω[j], j=1...N; 步骤1.2.3:对该模型的每个频点进行频率域电磁法正演计算,得到每个测点处的电磁场值,每个频点都需要正演两次,一次E极化的场源,一次H极化的场源,正演得到的电场、磁场值为AE[i,j]和AH[i,j],其中上标EH代表正演中E极化和H极化,i=1…M,j=1…N,A∈{Ex,Ey,Hx,Hy,Hz}。Step 1.2.3: Perform forward calculation of frequency domain electromagnetic method for each frequency point of the model to obtain the electromagnetic field value at each measurement point. Each frequency point needs to be forward modeled twice, once for the E-polarized field source , the field source of primary H polarization, the electric field and magnetic field values obtained by forward modeling are A E [i,j] and A H [i,j], where superscript E and H represent E polarization and H pole in forward modeling , i=1...M, j=1...N, A∈{Ex, Ey, Hx, Hy, Hz}. 3.根据权利要求1所述的基于理论模型正演计算的频率域电磁法时间序列数据合成方法基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,所述的频率域电磁法包括但不限于大地电磁法、音频大地电磁法、可控源音频大地电磁法以及频率域航空电磁法等所有频率域电磁探测方法。3. The frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation according to claim 1 The frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation is characterized in that, the frequency Domain electromagnetic methods include but are not limited to all frequency-domain electromagnetic detection methods, such as magnetotelluric method, audio-frequency magnetotelluric method, controllable-source audio-frequency magnetotelluric method, and frequency-domain airborne electromagnetic method. 4.根据权利要求2所述的基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,所述步骤1.2中的正演方法包括但不限于解析方法、数值模拟方法、开源软件计算和商业软件计算。4. the frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation according to claim 2, is characterized in that, the forward method in described step 1.2 includes but is not limited to analytical method, numerical simulation method, Open source software computing and commercial software computing. 5.根据权利要求1所述的基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,所述步骤2的具体步骤包括:对于每个频率f,将待合成的时间序列切分为多段,每段长度不固定,用于模拟场源随时间的变化,为保证时间序列能完整描述频谱信息,也保证数据处理时能恢复频谱信息,每段长度应大于该频率所对应的一个周期的长度(1/f),若长度太小则视为噪声,随机长度的参数也不固定,E极化和H极化的分段可以不同,最终时间序列被分为CE段和CH段。对每段时间序列,生成随机复数RE[k,j],k=1…CE和RH[k,j],k=1…CH,j=1…N,然后对每个测点计算AE[k,i,j]=AE[i,j]*RE[k,j]和AH[k,i,j]=AH[i,j]*RH,得到各分段的E极化场值和H极化场值,使得每段时间序列中的电磁场的强度和极化方向都不同。5. The frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation according to claim 1, is characterized in that, the concrete steps of described step 2 comprise: for each frequency f, combine the time to be synthesized The sequence is divided into multiple segments, and the length of each segment is not fixed. It is used to simulate the change of the field source with time. In order to ensure that the time series can completely describe the spectrum information, and also ensure that the spectrum information can be recovered during data processing, the length of each segment should be greater than the frequency specified. The length of a corresponding period (1/f), if the length is too small, it is regarded as noise, and the parameters of random length are not fixed. The segments of E polarization and H polarization can be different, and the final time series is divided into C E segment and CH segment. For each time series, generate random complex numbers RE[k,j], k = 1... CE and RH [k,j], k=1... CH , j=1...N, and then for each measurement Point calculation A E [k,i,j]=A E [i,j]*R E [k,j] and A H [k,i,j]=A H [i,j]*R H , get The E-polarization field value and H-polarization field value of each segment make the intensity and polarization direction of the electromagnetic field in each time series different. 6.根据权利要求1所述的基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,所述步骤3的具体步骤为:对于每个频率,利用步骤2得到的E极化场值和H极化场值(均为复数),分别计算各自的的振幅|A|和相位
Figure FDA0003546654640000021
按照式
Figure FDA0003546654640000022
计算每个分段时间序列,然后把这些分段时间序列收尾相连拼接起来,得到aE(j,t)和aH(j,t),二者叠加得到a(j,t),计算公式为a(j,t)=aE(j,t)+aH(j,t),为了减小时间序列拼接产生的信号阶跃,可以在拼接前对每段时间序列进行加窗处理。
6. the frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation according to claim 1, is characterized in that, the concrete step of described step 3 is: for each frequency, utilize the E obtained in step 2 Polarization field value and H polarization field value (both complex numbers), respectively calculate the respective amplitude |A| and phase
Figure FDA0003546654640000021
According to the formula
Figure FDA0003546654640000022
Calculate each segmented time series, and then splicing these segmented time series together to obtain a E (j, t) and a H (j, t), which are superimposed to obtain a (j, t), the calculation formula is a(j,t)= aE (j,t) +aH (j,t), in order to reduce the signal step generated by time series splicing, each time series can be windowed before splicing.
7.根据权利要求1所述的基于理论模型正演计算的频率域电磁法时间序列数据合成方法,其特征在于,所述步骤4的具体步骤为:把所有频点对应的拼接时间序列信号叠加得到总的时间序列,计算公式为
Figure FDA0003546654640000023
7. the frequency domain electromagnetic method time series data synthesis method based on theoretical model forward calculation according to claim 1, is characterized in that, the concrete step of described step 4 is: the splicing time series signal corresponding to all frequency points is superimposed To get the total time series, the formula is
Figure FDA0003546654640000023
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