CN106873038A - A kind of method that Depth Domain seismic wavelet is extracted in the geological data from Depth Domain - Google Patents
A kind of method that Depth Domain seismic wavelet is extracted in the geological data from Depth Domain Download PDFInfo
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Abstract
本发明实现了一种利用岭回归法,从深度域地震数据中提取深度域地震子波的方法,它包括以下步骤:1)从某口井的测井数据中获得深度、速度和密度信息,由此计算出对应的反射系数r;2)从叠前深度偏移地震数据中抽取该井的井旁地震道集s,并选取一个常速度vc作为标准速度,对选取的井旁地震道集s进行速度、深度参数的变换,使其符合线性时不变条件,得到变换后的井旁地震道集s';3)将反射系数r映射到变换后的深度位置上成为r';4)选取合适的岭参数α,用岭回归方法提取地震子波。本发明的方法是直接利用深度域地震数据提取深度域地震子波,且提取的深度域地震子波精度高,而不需要对深度域地震数据进行时间至深度域、深度至时间域的相互转换。
The present invention realizes a method for extracting depth-domain seismic wavelets from depth-domain seismic data by utilizing the ridge regression method, which includes the following steps: 1) obtaining depth, velocity and density information from the logging data of a certain well, From this, the corresponding reflection coefficient r is calculated; 2) Extract the side-well seismic gather s of the well from the pre-stack depth migration seismic data, and select a constant velocity v c as the standard velocity. Set s to transform the velocity and depth parameters, so that it conforms to the linear time-invariant condition, and obtain the transformed side-hole seismic gather s'; 3) Map the reflection coefficient r to the transformed depth position to become r'; 4 ) select the appropriate ridge parameter α, and use the ridge regression method to extract the seismic wavelet. The method of the present invention directly uses the depth-domain seismic data to extract the depth-domain seismic wavelet, and the extracted depth-domain seismic wavelet has high precision, without the mutual conversion of the depth-domain seismic data from time to depth domain and from depth to time domain .
Description
技术领域technical field
本发明涉及石油地震勘探数据处理与解释领域,特别是关于一种从深度域地震数据中提取深度域地震子波的方法。The invention relates to the field of petroleum seismic exploration data processing and interpretation, in particular to a method for extracting depth-domain seismic wavelets from depth-domain seismic data.
背景技术Background technique
叠前深度偏移技术在实际地震勘探中已得到了成功的应用,而且叠前深度偏移比叠前时间偏移在成像质量上具有更大的优势,为了从叠前深度偏移得到的深度域地震资料中反演地层的弹性参数,需要直接利用深度域测井数据和深度域地震子波生成深度域合成地震记录,用深度域合成地震记录标定深度域地震资料,从而开展储层预测等。深度域地震子波的提取是深度域地震参数反演、反褶积、地震正演等处理工作中的一个非常关键的部分,深度域地震子波提取的好坏直接关系到深度域地震资料的可用性和价值。Prestack depth migration technology has been successfully applied in actual seismic exploration, and prestack depth migration has a greater advantage in imaging quality than prestack time migration. In order to obtain depth from prestack depth migration To invert the elastic parameters of formations from seismic data in the deep domain, it is necessary to directly use the logging data in the depth domain and seismic wavelets in the depth domain to generate synthetic seismic records in the depth domain, and use the synthetic seismic records in the depth domain to calibrate the seismic data in the depth domain, so as to carry out reservoir prediction, etc. . The extraction of depth-domain seismic wavelets is a very critical part of the processing work such as depth-domain seismic parameter inversion, deconvolution, and seismic forward modeling. The quality of depth-domain seismic wavelet extraction is directly related to the quality of depth-domain seismic data. availability and value.
传统的地震子波提取算法主要是从时间域地震数据中提取的时间域地震子波,通常是基于褶积模型的,褶积模型的基本假设是线性时不变,即子波在传播过程中是稳定的,不变的,因此,要进行褶积运算必须满足线性时不变系统的条件。而在深度域中,地下不同空间和深度位置的地震波传播速度不同,地震波形必然发生变化,且地震子波的波数和地震波传播速度成反比,因此,深度域中的地震波场是不满足时不变特性的,因此,传统的地震子波提取算法在深度域中是不符合褶积运算条件的,也不可能直接在深度域地震数据中提取深度域地震子波。The traditional seismic wavelet extraction algorithm is mainly to extract the time-domain seismic wavelet from the time-domain seismic data, usually based on the convolution model. The basic assumption of the convolution model is linear time invariant, that is, the wavelet in the propagation process It is stable and invariant, therefore, the conditions of linear time-invariant system must be satisfied in order to perform convolution operation. In the depth domain, the propagation velocity of seismic waves in different spaces and depths of the underground is different, and the seismic waveform will inevitably change, and the wave number of the seismic wavelet is inversely proportional to the propagation velocity of the seismic wave. Therefore, the seismic wave field in the depth domain is not satisfied. Therefore, the traditional seismic wavelet extraction algorithm does not meet the convolution operation conditions in the depth domain, and it is impossible to directly extract the depth domain seismic wavelet from the depth domain seismic data.
传统的时间域地震子波提取方法可分为两类:一是确定性方法,即利用测井资料计算出反射系数,再结合井旁地震道求取子波;二是统计性方法,即利用统计性原理,对子波做出某种假设,利用地震道信号提取子波。两类方法各有优点和缺点,确定性方法的优点在于无需对地层脉冲响应做任何假设,也可提取出较准确的子波,缺点是受测井资料的影响较大;统计性方法在没有测井资料的情况下,直接利用地震道信号的统计特性也能提取子波,缺点是需要对地层脉冲响应做出一些统计性的假设。The traditional time-domain seismic wavelet extraction methods can be divided into two categories: one is the deterministic method, that is, using the logging data to calculate the reflection coefficient, and then combining the seismic traces beside the well to obtain the wavelet; the other is the statistical method, that is, using Statistical principle, making certain assumptions about wavelets, and extracting wavelets using seismic trace signals. The two types of methods have their own advantages and disadvantages. The advantage of the deterministic method is that it can extract more accurate wavelets without making any assumptions about the formation impulse response. The disadvantage is that it is greatly affected by the logging data; In the case of well logging data, wavelets can also be extracted by directly using the statistical properties of seismic trace signals. The disadvantage is that some statistical assumptions about the formation impulse response need to be made.
发明内容Contents of the invention
针对上述问题,本发明的目的是提供一种基于岭回归的方法,从深度域地震数据中直接提取深度域地震子波,而不需要再进行时间至深度、深度至时间的转换。In view of the above problems, the purpose of the present invention is to provide a method based on ridge regression, which can directly extract depth-domain seismic wavelets from depth-domain seismic data without the need for time-to-depth and depth-to-time conversions.
为实现上述目的,本发明采取以下技术方案:一种从深度域地震数据中提取深度域地震子波的方法,其包括以下步骤:⑴从某口井测井数据中获得深度、速度和密度信息,由此计算出对应的反射系数r;⑵从叠前深度偏移地震数据中挑选这口井的井旁地震道集s,同时选取一个常速度vc,并以该常速度为标准速度,对选取的井旁地震道集s进行速度、深度参数的变换,使其符合线性时不变的条件,得到变换后的井旁地震道集s';⑶将反射系数r映射到变换后的深度位置上成为r';⑷选取合适的岭参数α,用岭回归方法提取深度域地震子波。To achieve the above object, the present invention adopts the following technical solutions: a method for extracting depth-domain seismic wavelets from depth-domain seismic data, which includes the following steps: (1) obtaining depth, velocity and density information from certain well logging data , so as to calculate the corresponding reflection coefficient r; (2) Select the wellside seismic gather s of this well from the pre-stack depth migration seismic data, and select a constant velocity v c at the same time, and take this constant velocity as the standard velocity, Transform the velocity and depth parameters of the selected side-hole seismic gather s to make it conform to the linear time-invariant condition, and obtain the transformed side-hole seismic gather s'; (3) map the reflection coefficient r to the transformed depth The position becomes r'; (4) select the appropriate ridge parameter α, and use the ridge regression method to extract the seismic wavelet in the depth domain.
上述步骤⑵是根据下式对深度域井旁地震道的速度、深度进行变换,使其满足线性时不变的条件:The above step (2) is to transform the velocity and depth of the side-hole seismic trace in the depth domain according to the following formula, so that it satisfies the linear time-invariant condition:
式中,d是测井数据的深度采样间隔,dc是d变换后的深度值,vc是标准常速度,vmax是测井速度数据中记录到的最大速度。然后,以变换后的采样间隔dc对井旁地震道集s进行重新采样,从而将s变换为s'。In the formula, d is the depth sampling interval of the logging data, d c is the depth value after d transformation, v c is the standard constant velocity, and v max is the maximum velocity recorded in the logging velocity data. Then, the downhole seismic gather s is resampled with the transformed sampling interval dc, thereby transforming s into s'.
上述步骤⑶的实现,是由步骤⑴中计算得到的反射系数对应的深度:The realization of the above step (3) is the depth corresponding to the reflection coefficient calculated in step (1):
经过步骤⑵变换后的深度为:The depth after step (2) transformation is:
式中,n是测井数据的深度采样点数,h是测井数据记录的深度位置,hc是变换后的深度位置。将反射系数r映射到变换后的深度位置时,反射系数的值不变,即r=r'。In the formula, n is the number of depth sampling points of well logging data, h is the depth position of well logging data record, and h c is the depth position after transformation. When the reflection coefficient r is mapped to the transformed depth position, the value of the reflection coefficient remains unchanged, that is, r=r'.
上述步骤⑷中,经过变换后的深度域地震褶积模型用以下向量形式表示:In the above step (4), the transformed depth-domain seismic convolution model is expressed in the following vector form:
S=RWS=RW
式中,S是由变换后的井旁地震道集s'构建的列向量,R是由深度变换后的反射系数r'构建的Toeplitz矩阵,W是待求取的深度域地震子波向量。In the formula, S is a column vector constructed from the transformed side-hole seismic gather s', R is the Toeplitz matrix constructed from the depth-transformed reflection coefficient r', and W is the depth domain seismic wavelet vector to be obtained.
为了得到上式中W的唯一解,本发明方法采用岭回归的方法,即对下式的无约束最小化问题进行优化:In order to obtain the unique solution of W in the above formula, the method of the present invention adopts the method of ridge regression, promptly optimizes the unconstrained minimization problem of following formula:
min||S-RW||2+α||W2||min||S-RW|| 2 +α||W 2 ||
式中,α为岭参数,α>0。In the formula, α is the ridge parameter, α>0.
在实际计算中可以通过选择合适的α值,利用下式来求解上式最小化问题的解析解W:In actual calculation, the analytical solution W of the minimization problem of the above formula can be solved by using the following formula by selecting an appropriate value of α:
W=(RRT+αI)-1RTSW=(RR T +αI) -1 R T S
本发明由于采取以上技术方案,其优点是可以直接利用深度域地震数据提取深度域地震子波。Due to the adoption of the above technical scheme, the present invention has the advantage that it can directly use the depth domain seismic data to extract the depth domain seismic wavelet.
附图说明Description of drawings
图1是合成深度域地质模型及深度域地震记录,其中图1a是包含多个地层的深度域速度模型,横坐标为纵波速度,单位是米/秒,纵坐标为深度,单位是米,深度采样间隔为1米;图1b是与图1a对应的深度域合成地震记录,纵坐标为深度,单位是米。Figure 1 is a synthetic depth-domain geological model and depth-domain seismic records, in which Figure 1a is a depth-domain velocity model containing multiple formations, the abscissa is the P-wave velocity, the unit is m/s, the ordinate is the depth, the unit is m, and the depth The sampling interval is 1 meter; Fig. 1b is the depth-domain synthetic seismic record corresponding to Fig. 1a, and the ordinate is depth, and the unit is meter.
图2是对图1中的深度域合成地震记录提取深度域地震子波的结果。其中,图2a对比了本发明的方法提取的深度域地震子波(显示为实线)以及合成深度域地震记录中所用的原始深度域地震子波(显示为虚线),横坐标为深度,单位是米,纵坐标为振幅;图2b对比了本发明的方法提取的深度域地震子波(显示为实线)以及合成深度域地震记录中所用的原始深度域地震子波(显示为虚线)的波数谱,横坐标为波数,单位是米分之一,纵坐标为振幅。Fig. 2 is the result of extracting depth-domain seismic wavelets from the depth-domain synthetic seismic records in Fig. 1 . Wherein, Fig. 2 a compares the depth-domain seismic wavelet (shown as a solid line) extracted by the method of the present invention and the original depth-domain seismic wavelet (shown as a dotted line) used in the synthetic depth-domain seismic record, the abscissa is depth, and the unit is meter, and the ordinate is the amplitude; Fig. 2 b compares the depth domain seismic wavelet (shown as a solid line) extracted by the method of the present invention and the original depth domain seismic wavelet (shown as a dotted line) used in the synthetic depth domain seismic record Wavenumber spectrum, the abscissa is the wavenumber, the unit is one centimeter, and the ordinate is the amplitude.
图3是利用本发明的方法对某地区海上深度域角度道集地震数据提取深度域地震子波的结果,其中,图3a是该地区的叠前深度域角度道集地震数据,纵坐标为深度,深度范围为3550米~3975米,深度采样间隔为5m,横坐标为角度,单位是度。图3b是利用本发明的方法对图3a的数据提取的深度域地震子波,横坐标为深度,单位是米,纵坐标为振幅。Fig. 3 is the result of using the method of the present invention to extract the depth domain seismic wavelet from the depth domain angle gather seismic data in a certain area, wherein Fig. 3a is the pre-stack depth domain angle gather seismic data in this area, and the ordinate is depth , the depth range is 3550 meters to 3975 meters, the depth sampling interval is 5m, the abscissa is the angle, and the unit is degree. Fig. 3b is a depth-domain seismic wavelet extracted from the data in Fig. 3a by using the method of the present invention, the abscissa is the depth, the unit is meter, and the ordinate is the amplitude.
具体实施方式detailed description
下面结合附图和实施例对本发明进行详细的描述。The present invention will be described in detail below in conjunction with the accompanying drawings and embodiments.
本发明的一种从深度域地震数据中提取深度域地震子波的方法,包括以下步骤:A method of extracting depth-domain seismic wavelets from depth-domain seismic data of the present invention comprises the following steps:
⑴利用处理好的某口井的测井数据的深度、速度和密度信息,根据下式计算反射系数:(1) Using the depth, velocity and density information of the processed logging data of a certain well, calculate the reflection coefficient according to the following formula:
式中,ri是第i层与第i+1层界面的深度域反射系数,ρi是第i层的密度,vi是第i层的速度。In the formula, r i is the depth-domain reflection coefficient of the interface between the i-th layer and the i+1-th layer, ρ i is the density of the i-th layer, and v i is the velocity of the i-th layer.
⑵从叠前深度偏移地震数据中选取该井的井旁地震道集,同时设置一个常速度作为标准速度,根据下式,对深度域井旁地震道集进行速度、深度参数的变换,使其满足线性时不变的条件:(2) Select the wellside seismic gathers of this well from the pre-stack depth migration seismic data, and set a constant velocity as the standard velocity. According to the following formula, the velocity and depth parameters of the depth domain sidehole seismic gathers are transformed, so that It satisfies the linear time invariant condition:
式中,d是测井数据的深度采样间隔,dc是d变换后的深度值,vc是标准常速度,vmax是测井速度数据中记录到的最大速度。然后,以变换后的采样间隔dc对井旁地震道集s进行重新采样,从而将s变换为s'。In the formula, d is the depth sampling interval of the logging data, d c is the depth value after d transformation, v c is the standard constant velocity, and v max is the maximum velocity recorded in the logging velocity data. Then, the downhole seismic gather s is resampled with the transformed sampling interval dc, thereby transforming s into s'.
⑶步骤(1)中反射系数对应的深度为:(3) The depth corresponding to the reflection coefficient in step (1) is:
经过步骤⑵变换后的深度为:The depth after step (2) transformation is:
式中,n是测井数据的深度采样点数,h是测井数据记录的深度位置,hc是变换后的深度位置。将反射系数r映射到变换后的深度位置时,反射系数的值不变,即r=r'。In the formula, n is the number of depth sampling points of well logging data, h is the depth position of well logging data record, and h c is the depth position after transformation. When the reflection coefficient r is mapped to the transformed depth position, the value of the reflection coefficient remains unchanged, that is, r=r'.
⑷经过变换后的深度域的地震褶积模型可以用向量的形式表达为:(4) The transformed seismic convolution model in the depth domain can be expressed in the form of vectors as:
S=RWS=RW
式中,S是由变换后的井旁地震道集s'构建的列向量,R是由深度变换后的反射系数r'构建的Toeplitz矩阵,W是待求取的深度域地震子波向量。In the formula, S is a column vector constructed from the transformed side-hole seismic gather s', R is the Toeplitz matrix constructed from the depth-transformed reflection coefficient r', and W is the depth domain seismic wavelet vector to be obtained.
为了得到上式中W的唯一解,本发明方法采用基于岭回归的方法,即对下式无约束最小化问题进行优化:In order to obtain the unique solution of W in the above formula, the method of the present invention adopts the method based on ridge regression, promptly optimizes the unconstrained minimization problem of following formula:
min||S-RW||2+α||W2||min||S-RW|| 2 +α||W 2 ||
式中,α为岭参数,α>0。In the formula, α is the ridge parameter, α>0.
在实际计算中可以通过选择合适的α值,利用下式来求解上式最小化问题的解析解W:In actual calculation, the analytical solution W of the minimization problem of the above formula can be solved by using the following formula by selecting an appropriate value of α:
W=(RRT+αI)-1RTSW=(RR T +αI) -1 R T S
下面通过具体实施例对本发明的一种从深度域地震数据中提取深度域地震子波的方法进行进一步描述。A method for extracting depth-domain seismic wavelets from depth-domain seismic data according to the present invention will be further described below through specific embodiments.
图1a所示是人工合成的深度域多层速度模型,最小层速度为2000米/秒,最大层速度为4200米/秒,深度方向440米,深度采样间隔为1米。图1b是与图1a对应的深度域合成地震记录,从图1b中可见,在深度域中,地震反射子波在反射界面两侧的旁瓣是不对称的,它们与界面两侧地层的速度大小成正比,即地层速度越大,地震反射子波的旁瓣越宽。因此,深度域地震反射波形会随着地层速度的增加而变宽。Figure 1a shows the artificially synthesized multilayer velocity model in the depth domain. The minimum layer velocity is 2000 m/s, the maximum layer velocity is 4200 m/s, the depth direction is 440 meters, and the depth sampling interval is 1 meter. Fig. 1b is the depth-domain synthetic seismic record corresponding to Fig. 1a. It can be seen from Fig. 1b that in the depth domain, the side lobes of seismic reflection wavelets on both sides of the reflection interface are asymmetrical, and they are different from the velocity of the formation on both sides of the interface It is proportional to the size, that is, the greater the formation velocity, the wider the side lobe of the seismic reflection wavelet. Therefore, the depth-domain seismic reflection waveform will broaden as the formation velocity increases.
图2所示是利用本发明的方法,对图1b中的深度域合成地震记录提取深度域地震子波(图中实线表示)的结果,并与合成深度域地震记录所用的深度域原始地震子波(图中虚线表示)进行了比较。在图2a中,本发明的方法提取的深度域地震子波(实线表示)与深度域原始地震子波(虚线表示)的相关系数达到了0.9963;另外,从图2b可见,本发明的方法提取的深度域地震子波的波数谱(实线表示)与深度域原始地震子波的波数谱(虚线表示)的谱分布特征非常接近,说明本发明的方法提取的深度域地震子波具有很高的精度。Figure 2 shows the result of using the method of the present invention to extract the depth-domain seismic wavelet (indicated by the solid line in the figure) from the depth-domain synthetic seismic record in Figure 1b, and compares it with the depth-domain original earthquake used in the synthetic depth-domain seismic record subwaves (indicated by dashed lines in the figure) were compared. In Fig. 2a, the correlation coefficient between the depth domain seismic wavelet (indicated by solid line) extracted by the method of the present invention and the original seismic wavelet in depth domain (indicated by dotted line) has reached 0.9963; in addition, as can be seen from Fig. 2b, the method of the present invention The wavenumber spectrum (represented by the solid line) of the extracted depth-domain seismic wavelet is very close to the spectral distribution characteristics of the wavenumber spectrum (represented by the dotted line) of the original seismic wavelet in the depth domain, indicating that the depth-domain seismic wavelet extracted by the method of the present invention has very high precision.
图3是利用本发明的方法对某地区海上深度域角度道集地震数据提取深度域地震子波的结果,从图3b可见,本发明的方法从实际深度域地震数据中提取的深度域地震子波的质量是很高的。Fig. 3 is the result of using the method of the present invention to extract the depth domain seismic wavelet from the depth domain angle gather seismic data in a certain area. As can be seen from Fig. 3b, the depth domain seismic wavelet extracted by the method of the present invention from the actual depth domain seismic data The wave quality is very high.
上述各实施例仅用于说明本发明,其中方法的各实施步骤等都是可以有所变化的,凡是在本发明技术方案的基础上进行的等同变换和改进,均不应排除在本发明的保护范围之外。The above-mentioned embodiments are only used to illustrate the present invention, and the various implementation steps of the method etc. all can be changed to some extent, and all equivalent transformations and improvements carried out on the basis of the technical solution of the present invention should not be excluded from the scope of the present invention. outside the scope of protection.
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