CN111830581A - Open hole differential conductivity processing method - Google Patents
Open hole differential conductivity processing method Download PDFInfo
- Publication number
- CN111830581A CN111830581A CN201910303691.5A CN201910303691A CN111830581A CN 111830581 A CN111830581 A CN 111830581A CN 201910303691 A CN201910303691 A CN 201910303691A CN 111830581 A CN111830581 A CN 111830581A
- Authority
- CN
- China
- Prior art keywords
- difference
- conductivity
- stratum
- waveform
- depth
- 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.)
- Pending
Links
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V3/00—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
- G01V3/18—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging
- G01V3/26—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device
- G01V3/28—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for well-logging operating with magnetic or electric fields produced or modified either by the surrounding earth formation or by the detecting device using induction coils
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Remote Sensing (AREA)
- Life Sciences & Earth Sciences (AREA)
- Electromagnetism (AREA)
- Environmental & Geological Engineering (AREA)
- Geology (AREA)
- General Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- Geophysics (AREA)
- Geophysics And Detection Of Objects (AREA)
Abstract
A kind of open hole differential conductivity processing method, it is the well stratum physical parameter measurement technical field of the casing in the petroleum engineering well logging construction, this method can remove all unnecessary signals (including the secondary field response of liquid, cement sheath in the well) in the response by the waveform subtraction of the adjacent depth measurement of the same source distance, get the secondary field difference of the stratum (area) measured by two depth points of interval delta depth; deconvolution inversion is carried out by using the response difference (replacing the difference of the apparent conductivity) and the difference of the differential geometric factors, a stratum conductivity curve is reduced, and the problem of solving the stratum conductivity curve by using a differential inversion method is solved; under the condition that the source distance of the differential geometric factor is correctly selected, the formation conductivity can be completely reduced, and the formation resolution is improved.
Description
Technical Field
The invention belongs to the technical field of measurement of formation physical parameters of a cased well in logging construction of petroleum engineering, and particularly relates to a method for processing differential conductivity of an open hole well.
Background
In the exploration and development of petroleum, well logging is a very important means of assessing hydrocarbon reservoirs. In the aspect of a logging technology, a transient electromagnetic logging technology is developed and perfected by using a geophysical prospecting method, a transmitted signal is a step signal, transient excitation is adopted, and transient response waveforms of different source distances in a well are measured. The transmitted electromagnetic signal forms an eddy current in the medium outside the well, a secondary field generated by the eddy current is received by the receiving coil again, and the formation conductivity information is contained in the secondary field.
The received signals also include directly coupled signals (i.e., primary field) and secondary field signals, and the conventional method cannot eliminate the primary field irrelevant to the formation conductivity, so that the secondary field and the apparent conductivity cannot be acquired, and further the formation conductivity cannot be obtained. The waveform measured by the same source distance and the adjacent depth is subtracted to remove all useless signals (the primary field and the secondary field response of liquid and cement sheath in the well) in the response and obtain the secondary field difference of the stratum (area) measured by the adjacent two depth points.
Disclosure of Invention
Aiming at the problem in the prior art that the actual formation conductivity cannot be reduced due to the limitation of knowledge of the secondary field difference, the invention provides a method for processing the open hole differential conductivity, which deduces the relationship between the difference and the visual conductivity and the formation conductivity sequence on the basis of the secondary field difference measured by two adjacent depth points, reduces a formation conductivity curve by using a deconvolution method, and reduces a formation resistivity curve by calculating the reciprocal.
The specific method principle and description of the open hole differential conductivity processing method are as follows:
step one, transient electromagnetic logging is excited by adopting a step signal, and electromagnetic induction signals excited by an eddy current field with an interval delta depth are taken according to the characteristics of waveforms, namely transient electromagnetic induction receiving waveforms, wherein the induced electromotive force U of a receiving coil comprises information of a primary field and a secondary field, and a waveform 3 is obtained by using a signal waveform 1 and a waveform 2 with the interval delta depth to make a difference, because the primary fields with different depths are the same at the same moment, the primary field is eliminated in the waveform 3, and only the secondary field difference with the interval delta depth is left;
subtracting transient electromagnetic induction receiving waveforms of two depth points with the interval delta to obtain a response difference waveform 3, wherein the primary fields of the adjacent depth points are equal in size and same in phase, so that the primary fields can be eliminated by difference making, and the obtained receiving waveform difference is the product of the difference of the conductivity of view and the constant of a known instrument;
step three, obtaining the difference of the visual conductivity and the known difference geometric factor gΔPerforming deconvolution inversion on the difference to obtain a stratum conductivity curve, wherein sigma is the stratum conductivity curve;
step four, debugging a proper differential geometric factor gΔBecause the source distances L of the geometric factors are different, the shapes of the geometric factors are also inconsistent, the results obtained by inversion are also different, the correct geometric factors are obtained by debugging, and the deconvolution result is closest to the stratum conductivity curve;
and step five, obtaining the stratum conductivity after the steps one, two, three and four are executed, and comparing the stratum conductivity with an original curve.
Compared with the prior art, the open hole differential conductivity processing method has the beneficial effects that:
(1) signals of the receiving coil comprise primary field (useless signals) and secondary field signals, and the traditional method cannot eliminate the primary field irrelevant to the formation conductivity, so that the secondary field and the formation conductivity information cannot be acquired. According to the invention, all useless signals (including cased hole response and secondary field response of liquid and cement sheath in a well) in response can be removed by subtracting waveforms measured at the same source distance and adjacent depths, so that the secondary field difference of the stratum (region) measured by two points with the interval delta depth is obtained;
(2) the invention further indicates that the secondary field difference can be described by the difference of the geometric factors, the response difference is the secondary field difference, the secondary field difference is in direct proportion to the difference of the apparent conductivity, and the difference of the apparent conductivity can be regarded as the convolution result of the formation conductivity and the geometric factor difference; deconvolution is carried out by using the response difference (replacing the difference of the apparent conductivity) and the longitudinal differential geometric factor difference, and a formation conductivity curve is restored;
(3) when the source distance of the differential geometric factor is properly selected, the formation conductivity curve can be completely reduced, the formation resolution is improved, and the exploration of the residual oil layer is facilitated.
Drawings
FIG. 1 is a process data flow diagram of the present invention;
FIG. 2 is a doll differential geometry map with a source spacing of 0.6 m;
FIG. 3 is a plot of the difference in the formation conductivity curve and the waveform of two depth points spaced Δ =0.1m apart;
FIG. 4 is a graph of deconvolution with a differential geometry factor of 0.5m source-to-source distance and a waveform difference plot of two depth points spaced Δ =0.1 m;
fig. 5 is a graph of deconvolution performed with a geometric factor difference of 0.6m source distance and a waveform difference plot of two depth points spaced by Δ =0.1 m.
Detailed Description
The invention is further described with reference to the following figures and specific data processing examples, but the scope of the invention is not limited thereto.
The key point of the invention is that a useless primary field signal is eliminated by a method of making difference between waveforms of two depth points with the interval delta =0.1m, and the difficulty is that information of the stratum conductivity is extracted in an electromagnetic induction signal with large amplitude by a data processing mode. The problem that primary field signals cannot be processed is solved, and the convolution relation between the difference of the apparent conductivity and the difference of the longitudinal geometric factor is connected according to the linear relation between the difference of the response waveforms and the difference of the apparent conductivity, so that a formation conductivity curve is obtained, and the distribution of the residual oil layer can be evaluated.
Referring first to fig. 1, the steps of the processing method are shown, including the steps of:
step one, as shown in FIG. 2, obtaining a doll differential geometric factor graph with a source distance of 0.6m through definition calculation;
step two, as shown in fig. 3, subtracting the received waveforms of two depth points with an interval Δ =0.1m to obtain a curve of the difference of the received waveforms (response difference), wherein the difference is in direct proportion to the difference of the apparent conductance;
step three, as shown in fig. 4, deconvolution inversion is carried out on the selected differential geometric factor with the source distance of 0.5m, and the large fluctuation can be seen, and the fluctuation of the maximum value exceeds the amplitude of the real stratum;
step four, the difference of the differential geometric factors of the source distances of 0.6m is selected in fig. 5 to perform deconvolution inversion, so that the variation trends of the inverted and reduced stratum and the real stratum are the same, the amplitude is slightly deviated due to the initial value selection, and the source distance selection can be considered to be correct.
Claims (1)
1. A method for processing open hole differential conductivity is characterized by comprising the following steps: the specific method comprises the following steps:
step one, transient electromagnetic logging is excited by adopting a step signal, and electromagnetic induction signals excited by an eddy current field with an interval delta depth are taken according to the characteristics of waveforms, namely transient electromagnetic induction receiving waveforms, wherein the induced electromotive force U of a receiving coil comprises information of a primary field and a secondary field, and a waveform 3 is obtained by using a signal waveform 1 and a waveform 2 with the interval delta depth to make a difference, because the primary fields with different depths are the same at the same moment, the primary field is eliminated in the waveform 3, and only the secondary field difference with the interval delta depth is left;
subtracting transient electromagnetic induction receiving waveforms of two depth points with the interval delta to obtain a response difference waveform 3, wherein the primary fields of the adjacent depth points are equal in size and same in phase, so that the primary fields can be eliminated by difference making, and the obtained receiving waveform difference is the product of the difference of the conductivity of view and the constant of a known instrument;
step three, obtaining the difference of the visual conductivity and the known difference geometric factor gΔPerforming deconvolution inversion on the difference to obtain a stratum conductivity curve, wherein sigma is the stratum conductivity curve;
step four, debugging a proper differential geometric factor gΔBecause the source distances L of the geometric factors are different, the shapes of the geometric factors are also inconsistent, the results obtained by inversion are also different, the correct geometric factors are obtained by debugging, and the deconvolution result is closest to the stratum conductivity curve;
and step five, obtaining the stratum conductivity after the steps one, two, three and four are executed, and comparing the stratum conductivity with an original curve.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201910303691.5A CN111830581A (en) | 2019-04-16 | 2019-04-16 | Open hole differential conductivity processing method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201910303691.5A CN111830581A (en) | 2019-04-16 | 2019-04-16 | Open hole differential conductivity processing method |
Publications (1)
Publication Number | Publication Date |
---|---|
CN111830581A true CN111830581A (en) | 2020-10-27 |
Family
ID=72915485
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201910303691.5A Pending CN111830581A (en) | 2019-04-16 | 2019-04-16 | Open hole differential conductivity processing method |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN111830581A (en) |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20020173913A1 (en) * | 2001-04-03 | 2002-11-21 | Tabarovsky Leonty A. | Determination of formation anisotropy using multi-frequency processing of induction measurements with transverse induction coils |
CN103352691A (en) * | 2013-07-05 | 2013-10-16 | 天津大学 | Orthogonal dipole acoustic logging sound system receiving device |
CN105487128A (en) * | 2016-01-19 | 2016-04-13 | 中国海洋石油总公司 | Ground device used for relief well electromagnetic detection and positioning tool |
CN109209363A (en) * | 2018-09-14 | 2019-01-15 | 天津大学 | Cross casing stratum differential resistance rate well-logging probe structure |
-
2019
- 2019-04-16 CN CN201910303691.5A patent/CN111830581A/en active Pending
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20020173913A1 (en) * | 2001-04-03 | 2002-11-21 | Tabarovsky Leonty A. | Determination of formation anisotropy using multi-frequency processing of induction measurements with transverse induction coils |
CN103352691A (en) * | 2013-07-05 | 2013-10-16 | 天津大学 | Orthogonal dipole acoustic logging sound system receiving device |
CN105487128A (en) * | 2016-01-19 | 2016-04-13 | 中国海洋石油总公司 | Ground device used for relief well electromagnetic detection and positioning tool |
CN109209363A (en) * | 2018-09-14 | 2019-01-15 | 天津大学 | Cross casing stratum differential resistance rate well-logging probe structure |
Non-Patent Citations (1)
Title |
---|
钱科锋,等: "瞬变电磁测井原理研究V:径向几何因子", 《测井技术》 * |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US8812237B2 (en) | Deep-reading electromagnetic data acquisition method | |
US20200355841A1 (en) | Systems and methods for locating and imaging proppant in an induced fracture | |
CN109001823B (en) | Electromagnetic earth lens detection method and detection device | |
CN107575220B (en) | Through-casing formation differential resistivity logging method | |
ITMI20000463A1 (en) | DETECTIONS FOR DRILLING WELLS THROUGH ELECTROMAGNETIC INDUCTION | |
US9625604B2 (en) | Analyzing subterranean formation with current source vectors | |
US10520635B2 (en) | Apparatus and method for determining earth's near-surface properties with on-time measurements from airborne time-domain electromagnetic data | |
CN111188611B (en) | Method for processing deconvolution resistivity of cased well | |
Gasperikova et al. | Mapping of induced polarization using natural fields | |
CN111538093A (en) | Method for shallow surface detection and transient electromagnetic instrument | |
US10156655B2 (en) | Method and apparatus for measurement of pipe signals for downhole transient electromagnetic processing | |
CN115292890A (en) | Site soil pollutant concentration three-dimensional space prediction method based on multi-source auxiliary data development | |
CN111305813B (en) | Resistivity processing method based on cased well geometric factors | |
Katterbauer et al. | A time domain update method for reservoir history matching of electromagnetic data | |
CN112302636A (en) | Hydraulic fracturing monitoring method and device | |
AU2015218886B2 (en) | Electromagnetic fields using a conductive casing | |
US20170038492A1 (en) | Workflow to Use Borehole Completion as Antenna for Geophysical Applications | |
CN111830581A (en) | Open hole differential conductivity processing method | |
Onegova et al. | 3D simulation of transient electromagnetic field for geosteering horizontal wells | |
EP1247119B1 (en) | Method and apparatus of electrical resistivity measurements in geological formations employing modeling data | |
CN116430464A (en) | Method for improving processing quality of time-frequency electromagnetic method frequency domain data | |
Hickey | Application of Land-Based Controlled Source EM Method to Hydraulic Fracture Monitoring | |
CN113671582B (en) | Electrical source induction-polarization effect detection method based on three-component SQUID | |
US20240085584A1 (en) | System and Method for Combined Streaming Potential and Controlled-Source Electromagnetic Modeling | |
Liu et al. | Joint inversion of induction/lateral/normal logs, case studies at Shenli field site, China |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
WD01 | Invention patent application deemed withdrawn after publication | ||
WD01 | Invention patent application deemed withdrawn after publication |
Application publication date: 20201027 |