WO2016011627A1 - Amplitude-preserved static correction method for magnetic data - Google Patents
Amplitude-preserved static correction method for magnetic data Download PDFInfo
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- the present invention relates to geophysical exploration methods, and is an electromagnetic survey data including data processing techniques of magnetotelluric (MT), audio earth magneto (AMT), and continuous profile magnetotelluric (CEMP).
- MT magnetotelluric
- AMT audio earth magneto
- CEMP continuous profile magnetotelluric
- BACKGROUND OF THE INVENTION The static effect in electromagnetic exploration refers to the distortion of an electric field caused by the accumulation of polarized charges at a resistivity interface due to the presence of a local electrical inhomogeneity in the vicinity, thereby generating an additional electric field proportional to the external electric field. , and has nothing to do with frequency.
- MT magnetotelluric data
- the logarithmic domain resistivity curve translates along the vertical axis, and the phase curve is essentially unaffected.
- the present invention is directed to the defect that the effect of electromagnetic data static correction is not good after using the conventional filtering method, and provides a static correction of electromagnetic data for the purpose of overcoming the defect that the apparent resistivity curve shape can be changed and achieving the amplitude retention. method.
- the invention is implemented by the following steps:
- the magnetotelluric data collected in the work area determine a stable electrical layer with depth and resistivity, obtain the corresponding frequency band on the electromagnetic data curve, and do two apparent resistivity curves for all the measuring points on the electromagnetic data line on the frequency band. Average, calculate flat
- the resistivity data is uniform; the electromagnetic data includes magnetotelluric data (MT), audio magnetotelluric data (AMT), and continuous section method magnetotelluric data (CEMP).
- the average includes the arithmetic mean and the geometric mean.
- the calculated flat resistivity data is:
- the filtering includes two-dimensional median filtering, two-dimensional spatial filtering, three-dimensional median filtering, and three-dimensional spatial filtering.
- / 2 are the selected frequency point numbers respectively
- pf and ⁇ ( ) are the measured apparent resistivity values of the XY and YX modes of the first measuring frequency of the first measuring point, respectively
- a ⁇ , ⁇ are Calculate the apparent resistivity arithmetic or geometric mean of the pre-filtered XY and YX modes, and the apparent resistivity arithmetic or geometric mean of the calculated filtered XY and YX modes, respectively.
- K and the amplitude-preserving correction factor of the XY and YX curves of the first measuring point are respectively calculated according to the following formula to obtain the two curves of the apparent resistivity data "' and ⁇ after the final amplitude-correction correction, and the static correction is completed.
- FIG. 1 is a basic flow chart of an electromagnetic data amplitude correction static correction method. detailed description
- FIG. 1 is a flow chart showing the implementation of the amplitude-preserving static correction method. The specific method is:
- the calculated flat resistivity data is: Where P fj and ⁇ ( ) are the measured values of the measured values of the ⁇ and ⁇ modes of the first frequency of the first measuring point, respectively, and “ m is the selected frequency point number, which is 5 and 9 respectively in this example. 2) Use the following formula to obtain the initial correction factor for the two curves of each measurement point;
- the filtering includes two-dimensional median filtering, two-dimensional spatial filtering, three-dimensional median filtering, and three-dimensional spatial filtering.
- Ppsi and ⁇ P are the amplitude-corrected back-view resistivity data of the final XY and YX curves.
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Abstract
Description
一种电磁数据的保幅静校正方法 Method for preserving static correction of electromagnetic data
技术领域 本发明涉及地球物理勘探方法, 是一种电磁勘探数据, 包括大地电磁 (MT)、 音频大地电 磁 (AMT)和连续剖面法大地电磁 (CEMP)的数据处理技术。 背景技术 电磁法勘探中的静态效应是指由于近表存在局部电性不均匀体时, 电阻率分界面上极化 电荷的堆集引起电场的畸变, 由此产生一个与外电场成正比的附加电场, 且与频率无关。 对 于大地电磁数据 (MT), 表现在单点曲线上, 就是对数域电阻率曲线沿纵轴产生平移, 相位曲 线基本上不受影响。 表现在视电阻率断面图上, 就是电阻率值出现直立的陡变带, 俗称 "挂 面条"现象, 而相应的相位拟断面图上就没有这种现象。表现在单频点的视电阻率平面图上, 就是存在很多 "畸变点"现象。 静态效应的强度可达两三个数量级, 在推断深度时可引起很 大误差, 并使构造解释复杂化, 因此在反演解释之前需进行静校正。 目前, 静校正的方法很多, 为了压制静态效应, 不断提高 MT的应用效果, 国内外很多 专家发表了相关论文, 提出了滤波法、 理论计算法、 瞬变电磁校正法、 地表电阻率校正法、 高频电磁函数向上延拓法等。 这些方法大部分都是基于二维 MT静校正, 各种校正方法的原 理和对资料的要求不同, 在实际应用中都受到一定程度的限制。 由于滤波法易于实现, 处理 速度快, 在 MT/CEMP资料的静校正处理中应用最为广泛。 但是经过滤波法处理后, 很多测 点的视电阻率曲线形态会被改变, 尤其是在山前带、 地表岩性突变带等地方表现明显, 实践 中静校正效果不好。 发明内容 本发明针对采用传统的滤波法进行电磁数据静校正后效果不好的缺陷, 提供一种可以克 服视电阻率曲线形态会被改变的缺陷、 达到保幅的目的电磁数据的保幅静校正方法。 本发明采用以下步骤实现: TECHNICAL FIELD The present invention relates to geophysical exploration methods, and is an electromagnetic survey data including data processing techniques of magnetotelluric (MT), audio earth magneto (AMT), and continuous profile magnetotelluric (CEMP). BACKGROUND OF THE INVENTION The static effect in electromagnetic exploration refers to the distortion of an electric field caused by the accumulation of polarized charges at a resistivity interface due to the presence of a local electrical inhomogeneity in the vicinity, thereby generating an additional electric field proportional to the external electric field. , and has nothing to do with frequency. For magnetotelluric data (MT), on a single point curve, the logarithmic domain resistivity curve translates along the vertical axis, and the phase curve is essentially unaffected. It is manifested in the apparent resistivity cross-section, that is, the resistivity value shows an upright abrupt zone, commonly known as the "hanging noodle" phenomenon, and there is no such phenomenon on the corresponding phase pseudo-section. On the apparent resistivity plan of a single frequency point, there are many "distortion points" phenomena. The intensity of static effects can be up to two or three orders of magnitude, causing large errors in inferring depth and complicating structural interpretation, so static correction is required before inversion interpretation. At present, there are many methods for static correction. In order to suppress static effects and continuously improve the application effect of MT, many experts at home and abroad have published related papers, and proposed filtering methods, theoretical calculation methods, transient electromagnetic correction methods, surface resistivity correction methods, The high frequency electromagnetic function is extended upwards and the like. Most of these methods are based on two-dimensional MT static correction. The principles of various calibration methods and the requirements for data are different, and they are subject to a certain degree of limitation in practical applications. Because the filtering method is easy to implement and the processing speed is fast, it is the most widely used in the static correction processing of MT/CEMP data. However, after the filtering method, the apparent resistivity curve shape of many measuring points will be changed, especially in the piedmont belt and the surface lithologic mutation zone. In practice, the static correction effect is not good. SUMMARY OF THE INVENTION The present invention is directed to the defect that the effect of electromagnetic data static correction is not good after using the conventional filtering method, and provides a static correction of electromagnetic data for the purpose of overcoming the defect that the apparent resistivity curve shape can be changed and achieving the amplitude retention. method. The invention is implemented by the following steps:
1 )根据工区采集的大地电磁数据, 确定一个深度和电阻率稳定的电性层, 得到电磁数据 曲线上对应的频段, 对频段上电磁数据测线上所有测点的两支视电阻率曲线做平均, 计算平 均视电阻率数据 ; 所述的电磁数据包括大地电磁数据 (MT)、 音频大地电磁数据 (AMT)、 连续剖面法大地电 磁数据 (CEMP)。 所述的平均包括算术平均和几何平均。 所述的计算平 电阻率数据 是: 1) According to the magnetotelluric data collected in the work area, determine a stable electrical layer with depth and resistivity, obtain the corresponding frequency band on the electromagnetic data curve, and do two apparent resistivity curves for all the measuring points on the electromagnetic data line on the frequency band. Average, calculate flat The resistivity data is uniform; the electromagnetic data includes magnetotelluric data (MT), audio magnetotelluric data (AMT), and continuous section method magnetotelluric data (CEMP). The average includes the arithmetic mean and the geometric mean. The calculated flat resistivity data is:
其中, 、 分别为第 i个测点第 )个频率 的 XY和 YX模式实测视电阻 率值, "和 m为选定的频点号。 Where, , are the measured apparent resistivity values of the XY and YX modes of the first frequency of the i-th measuring point, respectively, and " m is the selected frequency point number.
2) 利用以下公式求取各个测点两支曲线的初步校正因子; 其中, 和 分别为第 个测点 XY和 YX模式数据的初步校正因子, 为由 (4)式获 得的计算平均值, 其它参数的含义与 (4)式相同。 2) Use the following formula to obtain the initial correction factor for the two curves of each measurement point; Wherein, and the preliminary correction factor for the first measurement point XY and YX mode data respectively, is the calculated average value obtained by the equation (4), and the meanings of the other parameters are the same as the equation (4).
3 ) 按照以下公式进行初步校正, 得到校正后的两支视电阻率曲线数据^^和 p = 10 * *(log pfY + kfY ), = 10 * *(log p + k ) (6) 再对 Af , P 分别进行滤波, 获得滤波后的视电阻率曲线数据 和 其它参数的含 义与 (4)、 (5)式相同。 所述的滤波包括二维中值滤波、 二维空间滤波、 三维中值滤波和三维空间滤波。 3) Perform a preliminary correction according to the following formula to obtain the corrected two apparent resistivity curve data ^^ and p = 10 * *(lo g pf Y + kf Y ), = 10 * *(lo g p + k ) ( 6) Filter Af and P separately, and obtain the filtered apparent resistivity curve data and other parameters with the same meanings as (4) and (5). The filtering includes two-dimensional median filtering, two-dimensional spatial filtering, three-dimensional median filtering, and three-dimensional spatial filtering.
4 ) 重新选择一个频率段, 按照步骤 1 ) 至 3 ) 分别计算出滤波前和滤波后各个测点两支 曲线在该频段范围内视电阻率的算术或者几何平均值 xy, p , 和 nf l 4) Reselect a frequency segment and calculate the arithmetic or geometric mean xy , p , and the apparent resistivity of the two curves of each of the measured points before and after filtering according to steps 1) to 3). Nf l
Σ ) ∑ ( ,) Σ ) ∑ ( ,)
其中, 和" /2分别为选定的频点号, p f 、 ^^( )分别为第 个测点第 ·/个频率 的 XY和 YX模式实测视电阻率值, A^、 ^^分别为计算的滤波前 XY和 YX模式的视 电阻率算术或者几何平均值, 和 分别为计算的滤波后 XY和 YX模式的视电阻率算 术或者几何平均值。 Wherein, and " / 2 are the selected frequency point numbers respectively, pf and ^^( ) are the measured apparent resistivity values of the XY and YX modes of the first measuring frequency of the first measuring point, respectively, A^, ^^ are Calculate the apparent resistivity arithmetic or geometric mean of the pre-filtered XY and YX modes, and the apparent resistivity arithmetic or geometric mean of the calculated filtered XY and YX modes, respectively.
按照以下公式求取各个测点两支曲线的保幅校正因子: fsi ^ = log ^ -log Calculate the amplitude correction factor of the two curves of each measuring point according to the following formula: fsi ^ = log ^ -log
(9) 其中, K 和 分别为第 个测点的 XY和 YX曲线的保幅校正因子 按照以下公式计算获得最终的保幅校正后两支曲线视电阻率数据 " '和^ ,完成静校 正。 (9) where K and the amplitude-preserving correction factor of the XY and YX curves of the first measuring point are respectively calculated according to the following formula to obtain the two curves of the apparent resistivity data "' and ^ after the final amplitude-correction correction, and the static correction is completed.
PZ = 10 * *dog + ), PZ = 10 * *(log + k ) (10) PZ = 10 * *dog + ), PZ = 10 * *( lo g + k ) (10)
Ppsi和 ίΠ P 就是最终的 XY和 YX曲线的保幅校正后视电阻率数据. 与背景技术相比, 本发明可以克服应用传统的滤波方法后视电阻率曲线形态会被改变的 缺陷, 尤其是在山前带、 地表岩性突变带等地方, 效果改善明显, 达到保幅的目的。 附图说明 图 1为电磁数据保幅静校正方法基本流程图。 具体实施方式 Ppsi and Π P are the amplitude-corrected back-resistivity data of the final XY and YX curves. Compared with the background art, the present invention can overcome the drawback that the shape of the back-resistivity curve can be changed by applying the conventional filtering method, especially In the mountain front belt, the surface lithology mutation zone, etc., the effect is improved obviously, and the purpose of maintaining the amplitude is achieved. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a basic flow chart of an electromagnetic data amplitude correction static correction method. detailed description
下面将结合本发明实施例中的附图, 对本发明实施例中的技术方案进行清楚、 完整地描 述, 显然, 所描述的实施例仅仅是本发明一部分实施例, 而不是全部的实施例。 基于本发明 中的实施例, 本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例, 都属于本发明保护的范围。 以下结合附图和实验实例详细说明本发明。 图 1是保幅静校正方法实施的流程图。 具体方法是: The technical solutions in the embodiments of the present invention are clearly and completely described in the following with reference to the accompanying drawings in the embodiments of the present invention. It is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments obtained by those of ordinary skill in the art based on the embodiments of the present invention without creative efforts, All fall within the scope of protection of the present invention. The invention will be described in detail below with reference to the accompanying drawings and experimental examples. Figure 1 is a flow chart showing the implementation of the amplitude-preserving static correction method. The specific method is:
1 )根据工区采集的大地电磁数据, 确定一个深度和电阻率稳定的电性层, 得到电磁数据 曲线上对应的频段, 如选取第 5号到第 9号频率段, 则公式 (4)中" =5, ^ =9。 对频段上电磁 数据测线上所有测点的两支视电阻率曲线做平均, 计算平均视电阻率数据 ; 所述的电磁数据包括大地电磁数据 (MT)、 音频大地电磁数据 (AMT)、 连续剖面法大地电 磁数据 (CEMP)。 所述的平均包括算术平均和几何平均。 所述的计算平 电阻率数据 是: 其中, P fj 、 ^ ( )分别为第 个测点第 ·个频率 的 χγ和 γχ模式实测视电阻 率值, "和 m为选定的频点号, 在本例子中分别为 5和 9。 2) 利用以下公式求取各个测点两支曲线的初步校正因子; 1) According to the magnetotelluric data collected in the work area, determine a stable electrical layer with depth and resistivity, and obtain the corresponding frequency band on the electromagnetic data curve. For example, if the frequency band No. 5 to No. 9 are selected, then in formula (4) =5, ^ = 9. Average the apparent resistivity curves of all the measuring points on the electromagnetic data line on the frequency band, and calculate the average apparent resistivity data; the electromagnetic data includes magnetotelluric data (MT), audio ground Electromagnetic data (AMT), continuous section method magnetotelluric data (CEMP). The average includes arithmetic mean and geometric mean. The calculated flat resistivity data is: Where P fj and ^ ( ) are the measured values of the measured values of the χγ and γχ modes of the first frequency of the first measuring point, respectively, and “ m is the selected frequency point number, which is 5 and 9 respectively in this example. 2) Use the following formula to obtain the initial correction factor for the two curves of each measurement point;
kf = log P - log^ -, k = log P - log Kf = log P - log^ -, k = log P - log
m - n + l m - n + l (5) 其中, 和 分别为第 个测点 XY和 YX模式数据的初步校正因子, 为由 (4)式获 得的计算平均值, 其它参数的含义与 (4)式相同。 m - n + lm - n + l (5) where , and the initial correction factor for the first measurement point XY and YX mode data, respectively, is the calculated average value obtained by equation (4), and the meanings of other parameters are (4) The same formula.
3 ) 按照以下公式进行初步校正, 得到校正后的两支视电阻率曲线数据^^和^^ : p = 10 * *(log pfY + k ), = 10 * *(log p + k ) (6) 再对 , P 分别进行滤波, 如在本例子中, 采用二维中值滤波, 中值滤波窗口选择为 (5,3), 获得滤波后的视电阻率曲线数据 和 ; 其它参数的含义与 (4)、 (5)式相同。 所述的滤波包括二维中值滤波、 二维空间滤波、 三维中值滤波和三维空间滤波。 4)重新选择一个频率段,如第 7号频率到第 13号频率段,即公式 (7)和公式 (8)中的^ ^1 ?, nf2=n, 按照步骤 1) 至 3) 分别计算出滤波前和滤波后各个测点两支曲线在该频段范围内 视电阻率的算术或者几何平均值 xy, p , ^ 和^ : nfl nfl 3) Perform preliminary correction according to the following formula to obtain the corrected two apparent resistivity curve data ^^ and ^^ : p = 10 * *(log pf Y + k ), = 10 * *(log p + k ) ( 6) Then, P is separately filtered, as in this example, using two-dimensional median filtering, the median filtering window is selected as (5,3), obtain the filtered apparent resistivity curve data and; the meanings of other parameters are the same as (4) and (5). The filtering includes two-dimensional median filtering, two-dimensional spatial filtering, three-dimensional median filtering, and three-dimensional spatial filtering. 4) Reselect a frequency segment, such as the frequency from the 7th to the 13th frequency, ie ^^ 1 ?, nf2 =n in the formula (7) and the formula (8), and calculate according to steps 1) to 3) respectively. The arithmetic or geometric mean of the apparent resistivity of the two curves of each measurement point before and after filtering, xy , p , ^ and ^ : nfl nfl
nfl nfl aXY _ j:nfl aYX _ j:nfl Nfl nfl aXY _ j:nfl aYX _ j:nfl
fSl ~ nfl- nf l + l' Ρ ' ~ nf2-nf\ + \ (8) 其中, 和" /2分别为选定的频点号, 在本例子中分别为 7和 13, P " 分别为第 个测点第 个频率 的 χγ和 γχ模式实测视电阻率值, ρ 、 ^分别为计算 的滤波前 χγ和 γχ模式的视电阻率算术或者几何平均值, 和 分别为计算的滤波后f Sl ~ nfl- nf l + l' Ρ ' ~ nf2-nf\ + \ (8) where, and " / 2 are the selected frequency points respectively, in this example, 7 and 13, respectively. P " is the measured apparent resistivity value of the χγ and γχ modes of the first frequency of the first measuring point, respectively, ρ and ^ are the calculated apparent resistivity arithmetic or geometric mean values of the pre-filtering χγ and γχ modes, respectively, and calculated separately. After filtering
ΧΥ和 ΥΧ模式的视电阻率算术或者几何平均值。 The apparent resistivity arithmetic or geometric mean of the ΧΥ and ΥΧ modes.
5) 按照以公式 (9)求取各个测点两支曲线的保幅校正因子: 其中, 和 分别为第 个测点的 XY和 YX曲线的保幅校正因子 5) Calculate the amplitude correction factor of the two curves of each measuring point according to formula (9): Where, and the amplitude correction factor of the XY and YX curves of the first measurement point respectively
6) 按照公式 (10)计算获得最终的保幅校正后两支曲线视电阻率数据 " '和^ V, 完成保 幅静校正。 6) Calculate the apparent resistivity data " ' and ^ V of the two curves after the final amplitude correction according to formula (10), and complete the amplitude correction.
P = 10 * *dog + ), PZ =10* *(log A + k ) P = 10 * *dog + ), PZ =10* *(lo g A + k )
(10) (10)
Ppsi和 ίΠ P 就是最终的 XY和 YX曲线的保幅校正后视电阻率数据. 以上所述的具体实施例, 对本发明的目的、技术方案和有益效果进行了进一步详细说明, 所应理解的是, 以上所述仅为本发明的具体实施例而已, 并不用于限定本发明的保护范围, 凡在本发明的精神和原则之内, 所做的任何修改、 等同替换、 改进等, 均应包含在本发明的 保护范围之内。 Ppsi and Π P are the amplitude-corrected back-view resistivity data of the final XY and YX curves. The specific embodiments described above further explain the objectives, technical solutions and beneficial effects of the present invention. It should be understood that The above descriptions are only specific embodiments of the present invention, and are not intended to limit the scope of the present invention. Any modifications, equivalent substitutions, improvements, etc., made within the spirit and scope of the present invention are intended to be included within the scope of the present invention.
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| CN106547020B (en) * | 2015-09-17 | 2018-10-02 | 中国石油化工股份有限公司 | A kind of relative amplitude preserved processing method of seismic data |
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