CN104422970A - Amplitude-preserving static correcting method for electromagnetic data - Google Patents

Amplitude-preserving static correcting method for electromagnetic data Download PDF

Info

Publication number
CN104422970A
CN104422970A CN201310397685.3A CN201310397685A CN104422970A CN 104422970 A CN104422970 A CN 104422970A CN 201310397685 A CN201310397685 A CN 201310397685A CN 104422970 A CN104422970 A CN 104422970A
Authority
CN
China
Prior art keywords
rho
data
apparent resistivity
log
curves
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201310397685.3A
Other languages
Chinese (zh)
Other versions
CN104422970B (en
Inventor
胡祖志
何展翔
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
China National Petroleum Corp
BGP Inc
Original Assignee
China National Petroleum Corp
BGP Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by China National Petroleum Corp, BGP Inc filed Critical China National Petroleum Corp
Priority to CN201310397685.3A priority Critical patent/CN104422970B/en
Publication of CN104422970A publication Critical patent/CN104422970A/en
Application granted granted Critical
Publication of CN104422970B publication Critical patent/CN104422970B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Geophysics And Detection Of Objects (AREA)
  • Measurement Of Resistance Or Impedance (AREA)

Abstract

The invention belongs to the technology of electromagnetic exploitation data processing. The technology comprises the following steps of collecting electromagnetic data, determining an electric layer with stable depth and resistivity, averaging two branches of apparent resistivity curves of all detecting points on an electromagnetic data detecting line on a corresponding frequency range, and calculating average apparent resistivity data; obtaining the primary correction factors of two branches of curves of each detecting point, correcting the primary correction factors to obtain data of the two branches of apparent resistivity curve, selecting a frequency range again, respectively calculating the average values of apparent resistivity of the two branches of curves of each detecting point within the frequency range before filtration and after filtration, obtaining amplitude-preserving correction factors of the two branches of curves of each detecting point, and calculating to obtain the apparent resistivity data of the two branches of curves after final amplitude-preserving correction. The defect that the configuration of the apparent resistivity curves is changed after the traditional filtration method is used can be overcome, particularly at the places, such as a mountain front and an earth surface lithologic character mutation region, the effect is obviously improved, and the aim of keeping amplitude is fulfilled.

Description

A kind of guarantor's width static correcting method of electromagnetic data
Technical field
The present invention relates to geophysical exploration method, is a kind of electromagnetic survey data, comprises the data processing technique of mt (MT), audio magnetotelluric method (AMT) and continuous profiling mt (CEMP).
Background technology
Static relays in electromagnetic prospecting refer to due to closely show to exist local electrically heterogeneous body time, on resistivity interphase, the heap of polarization charge causes the distortion of electric field, produces an additional electric field be directly proportional to external electric field thus, and irrelevant with frequency.For magnetotelluric data (MT), show on single-point curve, be exactly that log-domain resistivity curve produces translation along the longitudinal axis, phase curve is substantially unaffected.Show on apparent resistivity section diagram, be exactly that upright abrupt change band appears in resistivity value, be commonly called as " vermicelli bar " phenomenon, and corresponding phase place pseudosection map does not just have this phenomenon.Showing on the apparent resistivity planimetric map of single-frequency point, is exactly there is a lot " distortional point " phenomenon.The intensity of static relays can reach two or three orders of magnitude, can cause very big error, and making structure elucidation complicated, therefore needing to carry out static correction before inversion interpretation when inferring the degree of depth.
At present, the method of static correction is a lot, in order to suppress static relays, improves constantly the effect of MT, lot of domestic and international expert has delivered correlative theses, proposes filter method, theoretical calculation, transient electromagnetic correction method, subsurface resistivities correction method, high-frequency electromagnetic function upward continuation method etc.These method major parts are all based on two-dimentional MT static correction, and the principle of various bearing calibration is different with to the requirement of data, are all subject to restriction to a certain extent in actual applications.Because filter method is easy to realize, processing speed is fast, is most widely used in the static corrections processing of MT/CEMP data.But after filtering after method process, the apparent resistivity curve form of a lot of measuring point can be changed, especially in local performances such as mountain front, Lithology sudden change bands obviously, in practice, static correction effect is bad.
Summary of the invention
The present invention is directed to and adopt traditional filter method to carry out the bad defect of effect after electromagnetic data static correction, provide a kind of can overcome apparent resistivity curve form can reformed defect, reach guarantor's width static correcting method of the object electromagnetic data of guarantor's width.
The present invention adopts following steps to realize:
1) according to the magnetotelluric data that work area gathers, determine a degree of depth and the stable electric layers of resistivity, obtain frequency range corresponding on electromagnetic data curve, do on average to two apparent resistivity curves of measuring points all on electromagnetic data survey line in frequency range, calculate Average apparent resistivity data
Described electromagnetic data comprises magnetotelluric data (MT), audio-frequency magnetotelluric magnetic data (AMT), continuous profiling magnetotelluric data (CEMP).
Described on average comprises arithmetic mean and geometric mean.
Described calculating Average apparent resistivity data be:
Wherein, be respectively i-th measuring point jth frequency f jxY and YX pattern measured visual resistivity value, n and m is selected frequency point number.
2) following formula is utilized to ask for the preliminary corrections factor of each measuring point two curves;
k i XY = log ρ i a - log Σ j = n m ρ i XY ( f j ) m - n + 1 , k i YX = log ρ i a - log Σ j = n m ρ i YX ( f j ) m - n + 1 - - - ( 5 )
Wherein, with be respectively the preliminary corrections factor of i-th measuring point XY and YX mode data, the calculating mean value that (4) formula of serving as reasons obtains, the implication of other parameter is identical with (4) formula.
3) carry out preliminary corrections according to following formula, obtain two apparent resistivity curve data after correcting with
ρ si XY = 10 * * ( log ρ i XY + k i XY ) , ρ si YX = 10 * * ( log ρ i YX + k i YX ) - - - ( 6 )
Right again carry out filtering respectively, obtain filtered apparent resistivity curve data with the implication of other parameter and (4), (5) formula are identical.
Described filtering comprises two dimension median filter, two-dimensional space filtering, three-dimensional medium filtering and three dimensions filtering.
4) frequency band is reselected, according to step 1) to 3) calculate before filtering respectively and the arithmetic of each measuring point two curves apparent resistivity in this band limits or geometrical mean after filtering with
ρ si aXY = Σ j = nf 1 nf 2 ρ si XY ( f j ) nf 2 - nf 1 + 1 , ρ si aYX = Σ j = nf 1 nf 2 ρ si YX ( f j ) nf 2 - nf 1 + 1 - - - ( 7 )
ρ fsi aXY = Σ j = nf 1 nf 2 ρ fsi XY ( f j ) nf 2 - nf 1 + 1 , ρ fsi aYX = Σ j = nf 1 nf 2 ρ fsi YX ( f j ) nf 2 - nf 1 + 1 - - - ( 8 )
Wherein, nf1 and nf2 is respectively selected frequency point number, be respectively a si measuring point jth frequency f jxY and YX pattern measured visual resistivity value, be respectively apparent resistivity arithmetic or the geometrical mean of XY and YX pattern before the filtering of calculating, with be respectively apparent resistivity arithmetic or the geometrical mean of XY and YX pattern after the filtering of calculating.
5) guarantor's width correction factor of each measuring point two curves is asked for according to following formula:
k fi XY = log ρ si aXY - log ρ fsi aXY , k fi YX = log ρ i aYX - log ρ fsi aYX - - - ( 9 )
Wherein, with be respectively guarantor's width correction factor of XY and the YX curve of i-th measuring point.
6) obtain final guarantor's width according to following formulae discovery and correct rear two curve apparent resistivity datas with complete static correction.
ρ psi XY = 10 * * ( log ρ si XY + k fi XY ) , ρ psi YX = 10 * * ( log ρ si YX + k fi YX ) - - - ( 10 )
Wherein, with the guarantor's width being exactly final XY and YX curve corrects rear apparent resistivity data.
Compared with background technology, the present invention can to overcome after the traditional filtering method of application apparent resistivity curve form can reformed defect, especially in places such as mountain front, Lithology sudden change bands, obviously effect improved, reaches the object of guarantor's width.
Accompanying drawing explanation
Fig. 1 is then for electromagnetic data protects width static correcting method basic flow sheet.
Embodiment
Be below the specific embodiment of the invention, Fig. 1 is the process flow diagram protecting the enforcement of width static correcting method.
Concrete grammar is:
1) according to the magnetotelluric data that work area gathers, determine a degree of depth and the stable electric layers of resistivity, obtain frequency range corresponding on electromagnetic data curve, as chosen No. 5 to No. 9 frequency band, then n=5, m=9 in formula (4).Do on average to two apparent resistivity curves of measuring points all on electromagnetic data survey line in frequency range, calculate Average apparent resistivity data
Described electromagnetic data comprises magnetotelluric data (MT), audio-frequency magnetotelluric magnetic data (AMT), continuous profiling magnetotelluric data (CEMP).
Described on average comprises arithmetic mean and geometric mean.
Described calculating Average apparent resistivity data be:
Wherein, be respectively i-th measuring point jth frequency f jxY and YX pattern measured visual resistivity value, n and m is selected frequency point number, is respectively 5 and 9 in the present example.
2) following formula is utilized to ask for the preliminary corrections factor of each measuring point two curves;
k i XY = log ρ i a - log Σ j = n m ρ i XY ( f j ) m - n + 1 , k i YX = log ρ i a - log Σ j = n m ρ i YX ( f j ) m - n + 1 - - - ( 5 )
Wherein, with be respectively the preliminary corrections factor of i-th measuring point XY and YX mode data, the calculating mean value that (4) formula of serving as reasons obtains, the implication of other parameter is identical with (4) formula.
3) carry out preliminary corrections according to following formula, obtain two apparent resistivity curve data after correcting with
ρ si XY = 10 * * ( log ρ i XY + k i XY ) , ρ si YX = 10 * * ( log ρ i YX + k i YX ) - - - ( 6 )
Right again carry out filtering respectively, as in the present example, adopt two dimension median filter, medium filtering window selection is (5,3), obtains filtered apparent resistivity curve data with the implication of other parameter and (4), (5) formula are identical.
Described filtering comprises two dimension median filter, two-dimensional space filtering, three-dimensional medium filtering and three dimensions filtering.
4) frequency band is reselected, if No. 7 frequency is to No. 13 frequency band, namely the nf1=7 in formula (7) and formula (8), nf2=13, according to step 1) to 3) calculate before filtering respectively and the arithmetic of each measuring point two curves apparent resistivity in this band limits or geometrical mean after filtering with
ρ si aXY = Σ j = nf 1 nf 2 ρ si XY ( f j ) nf 2 - nf 1 + 1 , ρ si aYX = Σ j = nf 1 nf 2 ρ si YX ( f j ) nf 2 - nf 1 + 1 - - - ( 7 )
ρ fsi aXY = Σ j = nf 1 nf 2 ρ fsi XY ( f j ) nf 2 - nf 1 + 1 , ρ fsi aYX = Σ j = nf 1 nf 2 ρ fsi YX ( f j ) nf 2 - nf 1 + 1 - - - ( 8 )
Wherein, nf1 and nf2 is respectively selected frequency point number, is respectively 7 and 13 in the present example, be respectively a si measuring point jth frequency f jxY and YX pattern measured visual resistivity value, be respectively apparent resistivity arithmetic or the geometrical mean of XY and YX pattern before the filtering of calculating, with be respectively apparent resistivity arithmetic or the geometrical mean of XY and YX pattern after the filtering of calculating.
5) guarantor's width correction factor of each measuring point two curves is asked for according to (9) with the formula:
k fi XY = log ρ si aXY - log ρ fsi aXY , k fi YX = log ρ i aYX - log ρ fsi aYX - - - ( 9 )
Wherein, with be respectively guarantor's width correction factor of XY and the YX curve of i-th measuring point.
6) calculate the final guarantor's width of acquisition according to formula (10) and correct rear two curve apparent resistivity datas with complete and protect width static correction.
ρ psi XY = 10 * * ( log ρ si XY + k fi XY ) , ρ psi YX = 10 * * ( log ρ si YX + k fi YX ) - - - ( 10 )
Wherein, with the guarantor's width being exactly final XY and YX curve corrects rear apparent resistivity data.

Claims (5)

1. guarantor's width static correcting method of electromagnetic data, feature adopts following steps to realize:
1) according to the magnetotelluric data that work area gathers, determine a degree of depth and the stable electric layers of resistivity, obtain frequency range corresponding on electromagnetic data curve, do on average to two apparent resistivity curves of measuring points all on electromagnetic data survey line in frequency range, calculate Average apparent resistivity data
2) following formula is utilized to ask for the preliminary corrections factor of each measuring point two curves;
k i XY = log ρ i a - log Σ j = n m ρ i XY ( f j ) m - n + 1 , k i YX = log ρ i a - log Σ j = n m ρ i YX ( f j ) m - n + 1 - - - ( 5 )
Wherein, with be respectively the preliminary corrections factor of i-th measuring point XY and YX mode data, the calculating mean value that (4) formula of serving as reasons obtains, the implication of other parameter is identical with (4) formula;
3) carry out preliminary corrections according to following formula, obtain two apparent resistivity curve data after correcting with
ρ si XY = 10 * * ( log ρ i XY + k i XY ) , ρ si YX = 10 * * ( log ρ i YX + k i YX ) - - - ( 6 )
Right again carry out filtering respectively, obtain filtered apparent resistivity curve data with the implication of other parameter and (4), (5) formula are identical;
4) frequency band is reselected, according to step 1) to 3) calculate before filtering respectively and the arithmetic of each measuring point two curves apparent resistivity in this band limits or geometrical mean after filtering with
ρ si aXY = Σ j = nf 1 nf 2 ρ si XY ( f j ) nf 2 - nf 1 + 1 , ρ si aYX = Σ j = nf 1 nf 2 ρ si YX ( f j ) nf 2 - nf 1 + 1 - - - ( 7 )
ρ fsi aXY = Σ j = nf 1 nf 2 ρ fsi XY ( f j ) nf 2 - nf 1 + 1 , ρ fsi aYX = Σ j = nf 1 nf 2 ρ fsi YX ( f j ) nf 2 - nf 1 + 1 - - - ( 8 )
Wherein, nf1 and nf2 is respectively selected frequency point number, be respectively a si measuring point jth frequency f jxY and YX pattern measured visual resistivity value, be respectively apparent resistivity arithmetic or the geometrical mean of XY and YX pattern before the filtering of calculating, with be respectively apparent resistivity arithmetic or the geometrical mean of XY and YX pattern after the filtering of calculating;
5) guarantor's width correction factor of each measuring point two curves is asked for according to following formula:
k fi XY = log ρ si aXY - log ρ fsi aXY , k fi YX = log ρ i aYX - log ρ fsi aYX - - - ( 9 )
Wherein, with be respectively guarantor's width correction factor of XY and the YX curve of i-th measuring point;
6) obtain final guarantor's width according to following formulae discovery and correct rear two curve apparent resistivity datas with complete static correction;
ρ psi XY = 10 * * ( log ρ si XY + k fi XY ) , ρ psi YX = 10 * * ( log ρ si YX + k fi YX ) - - - ( 10 )
Wherein, with the guarantor's width being exactly final XY and YX curve corrects rear apparent resistivity data.
2. method according to claim 1, feature is that the electromagnetic data described in step 1) comprises magnetotelluric data, audio-frequency magnetotelluric magnetic data, continuous profiling magnetotelluric data.
3. method according to claim 1, feature on average comprises arithmetic mean and geometric mean described in step 1).
4. method according to claim 1, feature is the calculating Average apparent resistivity data described in step 1) be:
Wherein, be respectively i-th measuring point jth frequency f jxY and YX pattern measured visual resistivity value, n and m is selected frequency point number.
5. method according to claim 1, feature is that the filtering described in step 3) comprises two dimension median filter, two-dimensional space filtering, three-dimensional medium filtering and three dimensions filtering.
CN201310397685.3A 2013-09-04 2013-09-04 A kind of guarantor width static correcting method of electromagnetic data Active CN104422970B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201310397685.3A CN104422970B (en) 2013-09-04 2013-09-04 A kind of guarantor width static correcting method of electromagnetic data

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201310397685.3A CN104422970B (en) 2013-09-04 2013-09-04 A kind of guarantor width static correcting method of electromagnetic data

Publications (2)

Publication Number Publication Date
CN104422970A true CN104422970A (en) 2015-03-18
CN104422970B CN104422970B (en) 2017-03-15

Family

ID=52972515

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201310397685.3A Active CN104422970B (en) 2013-09-04 2013-09-04 A kind of guarantor width static correcting method of electromagnetic data

Country Status (1)

Country Link
CN (1) CN104422970B (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104903750A (en) * 2014-07-23 2015-09-09 王雅苹 Amplitude preservation statics method of electromagnetic data
CN110488365A (en) * 2019-09-11 2019-11-22 湖南五维地质科技有限公司 A kind of multipolarization telluric electromagnetic sounding method
CN111965712A (en) * 2020-10-21 2020-11-20 国网江西省电力有限公司电力科学研究院 Method for correcting static effect of controllable source audio magnetotelluric method
CN113484920A (en) * 2021-08-17 2021-10-08 成都理工大学 Two-dimensional structured inversion method for frequency domain electromagnetic sounding data

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4392109A (en) * 1980-11-14 1983-07-05 Mobil Oil Corporation Static correction for magnetotelluric data
CN102495431A (en) * 2011-11-16 2012-06-13 中煤科工集团西安研究院 Data processing method for carrying out static correction on transient electromagnetic data

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4392109A (en) * 1980-11-14 1983-07-05 Mobil Oil Corporation Static correction for magnetotelluric data
CN102495431A (en) * 2011-11-16 2012-06-13 中煤科工集团西安研究院 Data processing method for carrying out static correction on transient electromagnetic data

Non-Patent Citations (6)

* Cited by examiner, † Cited by third party
Title
ALAN G. JONES: "Static shift of magnetotelluric data and its removal in a sedimentary basin environment", 《GEOPHYSICS》 *
WILLIAM CUMMING ET AL.: "Resistivity Imaging of Geothermal Resources Using 1D, 2D and 3D MT Inversion and TDEM Static Shift Correction Illustrated by a Glass Mountain Case History", 《PROCEEDINGS WORLD GEOTHERMAL CONGRESS 2010 》 *
杨妮妮,等: "两种新方法实现CSAMT静态校正", 《华南地震》 *
汤井田,等: "静效应校正的波数域滤波方法", 《物探与化探》 *
罗延钟,等: "可控源音频大地电磁法的静态效应校正", 《物探与化探》 *
罗志琼: "用电磁阵列剖面法压制MT静态效应影响的研究", 《地球科学 中国地质大学学报》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104903750A (en) * 2014-07-23 2015-09-09 王雅苹 Amplitude preservation statics method of electromagnetic data
WO2016011627A1 (en) * 2014-07-23 2016-01-28 王雅苹 Amplitude-preserved static correction method for magnetic data
CN110488365A (en) * 2019-09-11 2019-11-22 湖南五维地质科技有限公司 A kind of multipolarization telluric electromagnetic sounding method
CN110488365B (en) * 2019-09-11 2021-05-07 湖南五维地质科技有限公司 Multi-polarization magnetotelluric depth measurement method
CN111965712A (en) * 2020-10-21 2020-11-20 国网江西省电力有限公司电力科学研究院 Method for correcting static effect of controllable source audio magnetotelluric method
CN111965712B (en) * 2020-10-21 2021-03-02 国网江西省电力有限公司电力科学研究院 Method for correcting static effect of controllable source audio magnetotelluric method
CN113484920A (en) * 2021-08-17 2021-10-08 成都理工大学 Two-dimensional structured inversion method for frequency domain electromagnetic sounding data
CN113484920B (en) * 2021-08-17 2023-05-19 成都理工大学 Two-dimensional structured inversion method for frequency domain electromagnetic sounding data

Also Published As

Publication number Publication date
CN104422970B (en) 2017-03-15

Similar Documents

Publication Publication Date Title
CN102495431B (en) Data processing method for carrying out static correction on transient electromagnetic data
Fedi et al. Multiscale analysis of potential fields by a ridge consistency criterion: the reconstruction of the Bishop basement
CN102998704A (en) Geophysical exploration seismic data processing method
Kayode et al. Geo-electrical investigation of near surface conductive structures suitable for groundwater accumulation in a resistive crystalline basement environment: a case study of Isuada, southwestern Nigeria
CN104422970A (en) Amplitude-preserving static correcting method for electromagnetic data
CN104656156A (en) Magnetic reference processing method for acquiring data in three dimensions audio-frequency magnetotelluric sounding
CN104903750A (en) Amplitude preservation statics method of electromagnetic data
CN103984011A (en) Dynamic Q compensation shifting method
CN107817526A (en) Prestack seismic gather segmented amplitude energy compensation method and system
Sundararajan et al. VLFPROS—A Matlab code for processing of VLF-EM data
Rajagopalan Analytic signal vs. reduction to pole: solutions for low magnetic latitudes
Ramazi et al. Contribution of geophysical inversion theory and geostatistical simulation to determine geoelectrical anomalies
CN104330826A (en) A method for removing various noises under the condition of complex surface
Dennis et al. Transient electromagnetic surveys for the measurement of near-surface electrical anisotropy
CN103913770A (en) Method for processing seismic data based on VSP data
Siemon Levelling of helicopter-borne frequency-domain electromagnetic data
CN108008456B (en) A method of delineation mesothermal gold deposits deep three-dimensional emphasis U metallogeny Favourable Target Areas
An et al. Auto-pick first breaks with complex raypaths for undulate surface conditions
CN105093318A (en) Self-adaptive wave equation wave field continuation static correction method
CN102608665A (en) Fine treatment technology of data information measured by geophysical prospecting time-domain transient electromagnetic system
Domenzain et al. Joint full-waveform ground-penetrating radar and electrical resistivity inversion applied to field data acquired on the surface
CN105093324B (en) A kind of residual static corrections
CN102937725A (en) Potential field anomaly edge enhancement method based on transition zone and phase congruency
Aizebeokhai et al. Field evaluation of 3D geo-electrical resistivity imaging for environmental and engineering studies using parallel 2D profiles
CN104459792A (en) Edge-preserving filtering method under structure constraints

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant