CN104931821A - Sensor probe for measuring electrical parameters of underground rock - Google Patents
Sensor probe for measuring electrical parameters of underground rock Download PDFInfo
- Publication number
- CN104931821A CN104931821A CN201510306766.7A CN201510306766A CN104931821A CN 104931821 A CN104931821 A CN 104931821A CN 201510306766 A CN201510306766 A CN 201510306766A CN 104931821 A CN104931821 A CN 104931821A
- Authority
- CN
- China
- Prior art keywords
- electrode
- rock
- voltage source
- sensor probe
- guarded
- 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
Abstract
The invention provides a sensor probe for measuring electrical parameters of an underground rock. The sensor probe comprises an emitter electrode, a collector electrode and a voltage source of the emitter electrode, and the voltage source of the emitter electrode is connected with the collector electrode and the emitter electrode via leads. The sensor probe is characterized by also comprising a shielding electrode and a voltage source of the shielding electrode, the shielding electrode is annular, the emitter electrode is arranged in a ring of the shielding electrode, and the voltage source of the shielding electrode is connected with the collector electrode and the shielding electrode via leads. The emitter electrode and the collector electrode are respectively arranged at the two sides of the sampled underground rock opposite to each other, the voltage source of the shielding electrode is loaded on the shielding electrode, and thus, current flowing out of the emitter electrode can penetrate a conductive slurry in parallel and reaches the collector electrode in the rock. The sensor probe can measure underground core samples in real time, and accurately and effectively obtains core information of the stratum in real time.
Description
Background technology
Core electrical quantity has very important meaning for correction logging trace, and traditional core electric parameter measurement method needs to measure sending ground experiment room after core sample collection back to.Measure the sensor probe adopted and comprise emitting electrode and passive electrode, emitting electrode and passive electrode is connected by a voltage source, the electric current that emitting electrode flows out arrives passive electrode through rock, electric current can be subject to the impact of rock resistivity and specific inductive capacity in the process through rock, thus impedance loop can be caused to change, just can be back-calculated to obtain resistivity and the specific inductive capacity of core to be measured according to the resistance value measured by setting up impedance loop and the relation between rock resistivity and specific inductive capacity.Send laboratory back to because traditional metering system needs to take out core from down-hole, this process causes measuring period long, and cost greatly, and can not the resistivity of Real-time Obtaining core sample and specific inductive capacity.
In down-hole, the real-time acquisition stratum core information of measurement while drilling energy is carried out to core sample, but subsurface environment is different from the measurement environment in laboratory, measurement can be subject to the impact of very many factors, first be that down-hole is filled with conductive drilling mud solution, now because the resistivity of rock is far away higher than mud resistivity, the conduct electricity flowed out from emitting electrode fails to be convened for lack of a quorum directly through conductive drilling mud arrival passive electrode, and seldom have electric current can penetrate mud to enter rock interior, this must cause popping one's head in and cannot measure the electrical quantity of rock.
Electric current due to the outflow of conductive drilling mud meeting blocking electrode enters the rock of high resistant, thus causes the electrical quantity change of instrument to rock insensitive.
Summary of the invention
Technical matters to be solved by this invention is, provides a kind of sensor probe configuration being applicable to subsurface environment.
The present invention for solving the problems of the technologies described above adopted technical scheme is, Rock in Well electric parameter measurement sensor probe, comprise emitting electrode, passive electrode, emitting electrode voltage source, emitting electrode voltage source is connected with passive electrode, emitting electrode respectively by wire, it is characterized in that, also comprises guarded electrode, guarded electrode voltage source, guarded electrode is ring texture, in the ring of the guarded electrode that emitting electrode is arranged on; Guarded electrode voltage source is connected with passive electrode, guarded electrode respectively by wire; Emitting electrode and passive electrode are arranged on the rock both sides of sampling down-hole in opposite directions;
Guarded electrode voltage source loads on the shield electrode, and the electric current that emitting electrode is flowed out can penetrate conductive drilling mud abreast and enter rock interior arrival passive electrode.
The present invention adopts guarded electrode form can penetrate conductive drilling mud to the electric current focusing on conduction current and make emitting electrode flow out and enters rock interior and arrive passive electrode and form loop, avoids conductive drilling mud and blocks the situation of electric current by rock.The galvanic circle of emitting electrode and passive electrode, through rock interior, provides the foundation for obtaining rock electrical quantity by impedance on the galvanic circle of measuring emitting electrode and passive electrode afterwards.
The invention has the beneficial effects as follows, be applicable to the sensor probe of subsurface environment, can measure in real time in down-hole core sample, accurate, efficient, real-time acquisition stratum core information.
Accompanying drawing explanation
Fig. 1 is the vertical view of the transverse section of sensor probe when measuring again.
Fig. 2 is the schematic diagram of emitting electrode and guarded electrode.
Fig. 3 be between emitting electrode and passive electrode loop resistance with the relation schematic diagram of guarded electrode voltage.
Embodiment
The present invention adopts specific measure to guide electric current to penetrate conductive drilling mud and enter into rock interior, thus gathers and take the electrical quantity of rock interior out of.
While powering to emitting electrode, make to be relative noble potential around internal electrode by adding suitable voltage on the shield electrode, thus the electric current that compressing is flowed out from emitting electrode cannot conduct along conductive drilling mud, select suitable voltage and electrode form that electric current can be made to penetrate conductive drilling mud, enter into rock interior, arrive ground connection pole plate by rock.
As shown in Figure 1, the rock 1 of sensor probe of the present invention to sampling is utilized to carry out electric parameter measurement.Rock 1 is wrapped up by conductive drilling mud 2.Sensor probe of the present invention comprises emitting electrode 3, passive electrode 4, emitting electrode voltage source V
2, guarded electrode 5, guarded electrode voltage source V
1, guarded electrode 5 is ring texture, as shown in Figure 2, in the ring of the guarded electrode 5 that emitting electrode 3 is arranged on; Emitting electrode voltage source V
2be connected with passive electrode 4, emitting electrode 3 respectively by wire, guarded electrode voltage source V
1be connected with passive electrode 4, guarded electrode 5 respectively by wire; Emitting electrode 3 and passive electrode 4 are arranged on rock 1 both sides of sampling down-hole in opposite directions.
When conduction current or displacement current flow through rock 1, equivalence capacitor model can be regarded as between emitting electrode and passive electrode, the resistance value at electric capacity two ends changes along with the electrical quantity of rock, by measuring the resistance value at electric capacity two ends, in conjunction with accurate numerical simulation modeling, inverting the electrical quantity of rock can be obtained.
Need to illustrate, the effect of guarded electrode is the current potential by controlling around emitting electrode, thus restriction internal polar plate flows out the flow direction of electric current.Voltage ratio a=V above guarded electrode and emitting electrode
1/ V
2design for sensor probe is extremely important.
In order to the relation in voltage and emitting electrode loop on the effect of guarded electrode and guarded electrode is better described, take frequency of operation as 1KHz, mud resistivity ρ
mud=1.0e2 Ω m, specific inductive capacity are ε
r_mud=1.0 and rock resistivity be ρ
rOCK=1.0e8 Ω m, specific inductive capacity are ε
r_ROCKthe situation of=1.0 is example, as shown in Figure 3:
Because frequency of operation is low frequency operating mode, so the current forms between the emitting electrode of probe and passive electrode is mainly conduction current, displacement current accounts for very little proportion.So only analyze the real part of impedance loop in figure 3, the active component namely in impedance.
As guarded electrode voltage and emitting electrode voltage ratio a=V
1/ V
2when=0, be equivalent to only have emitting electrode to power, the electric current of emitting electrode outflow in this case, directly flow into passive electrode along conductive drilling mud, now loop resistance value is close to Z
real=0 Ω, shows electric current not through rock interior.
As guarded electrode voltage and emitting electrode voltage ratio a=V
1/ V
2changing to about 0.8 from 0.2, in loop, resistance modulus value increases gradually, cause this is because the interior electrode of voltage compressing on guarded electrode flows out electric current inflow rock, due to the deficiency of voltage on guarded electrode, still have one part of current and flow along mud.This of voltage ratio change is interval, and we are called deficient focal region.
Work as a=V
1/ V
2change to this process of 1.0 from 0.8, in emitting electrode loop, resistance modulus value continues to increase, and in this interval the inside, along with increasing of mask voltage, the basic mountain of electric current that interior electrode flows out is all through rock.The now change of instrument to rock electrical quantity to be measured is the most responsive, and this is also the effect that our sensor probe is pursued.The electric current in this interval has reasonably been focused on inside rock, so we are called focal region this interval.
Along with mask voltage continue increase, work as a=V
1/ V
2when being greater than 1.01, due to the increase of guarded electrode voltage, the electric current of PARALLEL FLOW there will be interflow originally, is also in rock, there will be a focus exactly.Now interior electrode loop impedance is infinitely great, along with the continuation of peripheral voltage increases, interflow electric current can along interior electrode reversed flow, interior electrode loop resistive impedance value is reduced gradually by minus infinity, but because interior electrode no current flows into rock interior, so can not detect resistivity and the specific inductive capacity of rock.We called focal region this region of voltage.
Deficient focal region, focal region and the separatrix crossed between focal region are not a clear and definite point, but the interval that fuzzy, incomplete same between the focal region that different logging environment is corresponding, but it is identical for scanning for whole interval the curve tendency obtained, those skilled in the art according to different situations, different curves and can require between the focal region that definition is corresponding.
Can find out, when a>>1 time, because high voltage form can cause occurring focusing phenomenon, by current focusing in conducting mud pulp layer, can not better enter rock on the contrary; Deficient focusing phenomenon is there will be again on the contrary when a<<1 time; Only have and can realize Current Control effectively when a gets suitable value time, make electric current pass mud and enter rock, thus ensure that the electrical quantity of sensor probe to rock is the most responsive.Voltage ratio scope can change according to the situation difference measured.Those skilled in the art by controlling the voltage ratio of shielding electrode voltage source and emitting electrode voltage source flexibly, can ensure the adaptive faculty of probe to different test environments.
Sensor probe of the present invention can be operated in multifrequency pattern, and different frequency of operation is different for the susceptibility of different electrical quantitys to be measured, and adopting multifrequency pattern to combine can more accurate inverting rock electrical quantity.Under needing to set up each frequency of operation so before measuring, different resistivity and the lower corresponding impedance response of specific inductive capacity combination.For double frequency pattern:
First, two kinds of frequency f are set up by numerical evaluation
1=10KHz, f
2=1MHz is in various electricalresistivityρ=1000 ~ 1000000 Ω m and DIELECTRIC CONSTANT ε
rimpedance response Z (comprising real part and imaginary part) database under=1 ~ 80:
Z_f
1_r_s(ρ,ε
r),Z_f
1_i_s(ρ,ε
r),
Z_f
2_r_s(ρ,ε
r),Z_f
2_i_s(ρ,ε
r),
Z_f
1_ r_s (ρ, ε
r) be frequency of operation f
1certain electricalresistivityρ and DIELECTRIC CONSTANT ε
rthe real part of corresponding impedance response simulation value, Z_f
1_ i_s (ρ, ε
r) be frequency of operation f
1certain electricalresistivityρ and DIELECTRIC CONSTANT ε
rthe imaginary part of corresponding impedance response simulation value;
Z_f
2_ r_s (ρ, ε
r) be frequency of operation f
2certain electricalresistivityρ and DIELECTRIC CONSTANT ε
rthe real part of corresponding impedance response simulation value, Z_f
2_ i_s (ρ, ε
r) be frequency of operation f
2certain electricalresistivityρ and DIELECTRIC CONSTANT ε
rthe imaginary part of corresponding impedance response simulation value;
In detection process afterwards, obtain the impedance response probe value (comprising real part and imaginary part) under 2 kinds of frequencies:
Z_f
1_r_m(ρ,ε
r),Z_f
1_i_m(ρ,ε
r),
Z_f
2_r_m(ρ,ε
r),Z_f
2_i_m(ρ,ε
r)
Find optimum solution in a database, make following objective function minimum:
W
rj, W
ijbeing respectively weight coefficient, is empirical value.
By substituting in objective function to the impedance data under 2 kinds of frequencies of recording, ergodic data storehouse, finds the specific inductive capacity and resistivity that make the minimum correspondence of objective function, just can obtain the corresponding electrical quantity of oil-base mud.
Claims (1)
1. Rock in Well electric parameter measurement sensor probe, comprise emitting electrode, passive electrode, emitting electrode voltage source, emitting electrode voltage source is connected with passive electrode, emitting electrode respectively by wire, it is characterized in that, also comprise guarded electrode, guarded electrode voltage source; Guarded electrode is ring texture, in the ring of the guarded electrode that emitting electrode is arranged on; Guarded electrode voltage source is connected with passive electrode, guarded electrode respectively by wire; Emitting electrode and passive electrode are arranged on the rock both sides of sampling down-hole in opposite directions;
Guarded electrode voltage source loads on the shield electrode, and the electric current that emitting electrode is flowed out can penetrate conductive drilling mud abreast and enter rock interior arrival passive electrode.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510306766.7A CN104931821A (en) | 2015-06-05 | 2015-06-05 | Sensor probe for measuring electrical parameters of underground rock |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201510306766.7A CN104931821A (en) | 2015-06-05 | 2015-06-05 | Sensor probe for measuring electrical parameters of underground rock |
Publications (1)
Publication Number | Publication Date |
---|---|
CN104931821A true CN104931821A (en) | 2015-09-23 |
Family
ID=54119080
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201510306766.7A Pending CN104931821A (en) | 2015-06-05 | 2015-06-05 | Sensor probe for measuring electrical parameters of underground rock |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN104931821A (en) |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06342296A (en) * | 1993-06-01 | 1994-12-13 | Seikosha Co Ltd | Speaker device with electrostatic sensor |
CN2594811Y (en) * | 2002-03-12 | 2003-12-24 | 辽河石油勘探局测井公司 | Array microresistivity logging instruments with multiple laminar capacity |
CN1696473A (en) * | 2004-05-12 | 2005-11-16 | 施卢默格海外有限公司 | Formation imaging while drilling in non-conductive mud |
CN1821810A (en) * | 2006-03-24 | 2006-08-23 | 黄委会水科院高新工程技术研究开发中心 | Detecting method for bunching DC resistivity |
CN1955728A (en) * | 2005-10-28 | 2007-05-02 | 中国石油大学(北京) | Rock micro-electric scanning imaging system and imaging method |
CN101688924A (en) * | 2008-04-08 | 2010-03-31 | 哈里伯顿能源服务公司 | Method and apparatus with high resolution electrode configuration of the imaging that is used for oil-base mud |
CN101819282A (en) * | 2010-04-28 | 2010-09-01 | 中国石油天然气集团公司 | Electrode for measuring formation resistivity |
CN202645540U (en) * | 2012-07-18 | 2013-01-02 | 中国石油天然气集团公司 | Diameter-variable three-detection-depth high-resolution three-lateral logger |
CN104453880A (en) * | 2014-12-09 | 2015-03-25 | 重庆地质仪器厂 | Seven-electrode resistivity measurement probe |
-
2015
- 2015-06-05 CN CN201510306766.7A patent/CN104931821A/en active Pending
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06342296A (en) * | 1993-06-01 | 1994-12-13 | Seikosha Co Ltd | Speaker device with electrostatic sensor |
CN2594811Y (en) * | 2002-03-12 | 2003-12-24 | 辽河石油勘探局测井公司 | Array microresistivity logging instruments with multiple laminar capacity |
CN1696473A (en) * | 2004-05-12 | 2005-11-16 | 施卢默格海外有限公司 | Formation imaging while drilling in non-conductive mud |
CN1955728A (en) * | 2005-10-28 | 2007-05-02 | 中国石油大学(北京) | Rock micro-electric scanning imaging system and imaging method |
CN1821810A (en) * | 2006-03-24 | 2006-08-23 | 黄委会水科院高新工程技术研究开发中心 | Detecting method for bunching DC resistivity |
CN101688924A (en) * | 2008-04-08 | 2010-03-31 | 哈里伯顿能源服务公司 | Method and apparatus with high resolution electrode configuration of the imaging that is used for oil-base mud |
CN101819282A (en) * | 2010-04-28 | 2010-09-01 | 中国石油天然气集团公司 | Electrode for measuring formation resistivity |
CN202645540U (en) * | 2012-07-18 | 2013-01-02 | 中国石油天然气集团公司 | Diameter-variable three-detection-depth high-resolution three-lateral logger |
CN104453880A (en) * | 2014-12-09 | 2015-03-25 | 重庆地质仪器厂 | Seven-electrode resistivity measurement probe |
Non-Patent Citations (1)
Title |
---|
李婷兰: "高分辨感应测井仪数字球形聚焦系统研究", 《中国优秀硕士学位论文全文数据库 基础科学辑》 * |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN101216523B (en) | Substation grounding net defect diagnostic method and apparatus | |
CN102735992B (en) | Surface potential pilot frequency comparison-based ground grid defect identification method and system | |
CN102767364B (en) | High-resolution dual-side-direction logging instrument and resistivity measurement method | |
CN102767367B (en) | High-resolution lateral logger and resistivity-measuring method | |
Yu et al. | Break-point diagnosis of grounding grids using transient electromagnetic apparent resistivity imaging | |
CN107725045B (en) | Multi-polar polarizability combined logging instrument and logging method thereof | |
CN102495291A (en) | Impedance frequency response method for measuring corrosion state of grounding network of transformer substation | |
CN110082393A (en) | Dykes and dams real-time monitoring system and method based on mobile communication and high-density electric | |
CN104897995B (en) | Grounding net of transformer substation corrosion detection system and method based on surface potential | |
CN106291722A (en) | A kind of ground well induced-polarization measurement method and relevant device | |
CN106547030A (en) | Dam leakage electric field 3-D scanning automatic detection device and method | |
CN206378448U (en) | Polluted Soil detection arrangement of measuring-line structure based on comprehensive geophysical prospecting methods | |
CN104360402B (en) | Well-to-ground joint electrical-method testing method and system | |
CN205809177U (en) | A kind of rock complex resistivity measurement apparatus under the conditions of oil-water displacement | |
CN103869206A (en) | Grounding network state detection system for high-frequency pulse inverse scattering imaging | |
CN105510982B (en) | To three-dimensional multi-electrode on-line water flushing system before TBM construction tunnel focus type based on induced polarization method | |
CN104989387A (en) | Sensor probe for measuring downhole rock electrical parameters | |
CN209264613U (en) | A kind of refuse landfill pollutant diffusion monitoring device based on resistivity CT imaging | |
Parashar et al. | Designing efficient soil resistivity measurement technique for agricultural wireless sensor network | |
CN206331127U (en) | The node type seismic prospecting instrument of wave detector state is monitored in real time | |
CN207964994U (en) | Grounding net of transformer substation health status detection device | |
CN104931821A (en) | Sensor probe for measuring electrical parameters of underground rock | |
CN103643946A (en) | Dual-electrical-parameter logging instrument while drilling | |
CN103292680A (en) | Novel electric nondestructive anchor rod length measuring method and device | |
CN110967767A (en) | Method for detecting karst cave by cross-hole induced polarization |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
RJ01 | Rejection of invention patent application after publication |
Application publication date: 20150923 |
|
RJ01 | Rejection of invention patent application after publication |