CN102551711A - Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field - Google Patents

Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field Download PDF

Info

Publication number
CN102551711A
CN102551711A CN201010580178XA CN201010580178A CN102551711A CN 102551711 A CN102551711 A CN 102551711A CN 201010580178X A CN201010580178X A CN 201010580178XA CN 201010580178 A CN201010580178 A CN 201010580178A CN 102551711 A CN102551711 A CN 102551711A
Authority
CN
China
Prior art keywords
magnetic field
field
maximum
supply source
interference device
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
CN201010580178XA
Other languages
Chinese (zh)
Other versions
CN102551711B (en
Inventor
蒋式勤
石明伟
朱俊杰
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.)
Tongji University
Original Assignee
Tongji University
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 Tongji University filed Critical Tongji University
Priority to CN 201010580178 priority Critical patent/CN102551711B/en
Publication of CN102551711A publication Critical patent/CN102551711A/en
Application granted granted Critical
Publication of CN102551711B publication Critical patent/CN102551711B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Measurement And Recording Of Electrical Phenomena And Electrical Characteristics Of The Living Body (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

The invention relates to a method for measuring a magnetic field by the aid of a superconducting quantum interference device and positioning a current source of the magnetic field. The method comprises following steps: 1) acquiring magnetic field signals on a small quantity of measuring points by the aid of the superconducting quantum interference device; 2) obtaining a magnetic field maximum value and a magnetic field minimum value at every moment according to the measured magnetic field signals; and 3) obtaining position and strength parameters of a magnetic field source after a computer processes the magnetic field maximum value and the magnetic field minimum value at every moment in the step 2). Compared with the prior art, the method has the advantages of simplicity, effectiveness, capability of greatly saving cost of hardware, and the like.

Description

Measure magnetic field and locate the method in field supply source with superconducting quantum interference device
Technical field
The present invention relates to the method for field supply source location, especially relate to superconducting quantum interference device and measure magnetic field and locate the method in field supply source.
Background technology
1970-1976 D.Cohen etc. has proposed under lab to use superconducting quantum interference device (superconducting quantum interference device first; SQUID) measure the cardiac magnetic field signal, and the method for locating an electric current dipole source.Over nearly 40 years, the research of magnetic field detection and source location causes the attention of various countries' height.Range of application constantly enlarges.In order to improve the precision of source location, the port number of measuring magnetic field with SQUID constantly increases, and this also causes equipment cost to increase.36-64 the passage SQUID synchro measure field signal that general commercial cardiac magnetic field measuring system need adopt 6X 6 to arrange, not only hardware system is complicated, and the computational methods and the software for calculation of Magnetic Field Source location inverse problem also face problems.Therefore, a kind ofly can carry out the accurate localized method in field supply source through a small amount of magnetic field measuring point and belong to new invention.
Summary of the invention
The object of the invention is exactly to provide method simple, efficient for the defective that overcomes above-mentioned prior art existence; And can save the hardware cost of magnetic field measurement system; Simplify related algorithm and software, obtain the measuring magnetic field and locate the method in field supply source of source location result accurately with superconducting quantum interference device.
The object of the invention can be realized through following technical scheme: measure magnetic field and locate the method in field supply source with superconducting quantum interference device; It is characterized in that this method may further comprise the steps: 1) utilize the field signal on a small amount of measuring point of superconducting quantum interference device collection; 2) obtain each magnetic field maximum and magnetic field minimum constantly according to the field signal that measures; 3) computer is to step 2) in each magnetic field maximum and magnetic field minimum constantly of trying to achieve obtain the position and the intensive parameter in field supply source after handling.
Whether counting that field signal need be measured in the described step 1) can be fixed to confirm according to the field supply source position, for the Magnetic Field Source of fixed-site, only needs two measurement points usually; If the source position periodically changes, then need gather the field signal on several adjacent test points, obtain maximum and the minimum of measuring magnetic field through interpolation.
Described step 1), step 2) in field signal comprise X-Y coordinate that each magnetic field value constantly is corresponding with this magnetic field value.
Described step 3) is specially:
31) at first utilize formula
θ = arcsin ( 6 3 )
Obtain according to magnetic field maximum and minimizing coordinate
Figure BSA00000379078500024
Value, maximum B in magnetic field on the measurement plane Zmax(x 1, y 1) to magnetic field minimum B Zmin(x, the angle of line D y) and measurement plane X axle does
Figure BSA00000379078500025
32) then, with
Figure BSA00000379078500026
value and step 2) in the magnetic field maximum of trying to achieve and minimum and their position coordinateses on measurement plane bring following formula into:
Figure BSA00000379078500027
Obtain the depth d in field supply source;
33) utilize formula
B z max = μ 0 Q 6 π 3 d 2
Figure BSA00000379078500029
Figure BSA000003790785000210
Figure BSA000003790785000211
Obtain the coordinate (x in magnetic field intensity Q and field supply source 0, y 0), wherein, Q xAnd Q yBe the strength component of this field supply source at X and Y coordinate.
Described step 2) in, in the time can obtaining magnetic field maximum and magnetic field minima, just uses the minimum in this minima approximate substitution magnetic field, magnetic field according to field signal.
Described step 2) in, in the time can only trying to achieve maximum value of magnetic field and magnetic field minimum, just uses the maximum approximate substitution magnetic field maximum in this magnetic field according to field signal.
Because the present invention adopts above technical scheme; Promptly utilize the field signal on 2~8 measurement points of superconducting quantum interference device collection to carry out the field supply source location; So; Localization method is simple, effective, adopts 36 or 64 multichannel SQUID array detection methods to compare with prior art, can save hardware cost greatly.
Description of drawings
Fig. 1 is the sketch map that utilizes two field supply sources, field signal location on the SQUID measurement point;
Fig. 2 is the measuring point scattergram on the measurement plane.
Current dipole source of 1 expression among Fig. 1.
The specific embodiment
Below in conjunction with accompanying drawing 1 and specific embodiment the present invention is elaborated.
Embodiment
Two measurement points of A and B are arranged in the given coordinate system of Fig. 1.The position at the maximum place in A point expression magnetic field, B point expression minimizing position, magnetic field.The below of the measurement plane that the X-Y coordinate is formed, being positioned at the depth d place has a current dipole source that produces measured magnetic field.The angle of the line of measurement point A and this current dipole is θ on the measurement plane, and the angle of the line of A, B measurement point and X axle is
Figure BSA00000379078500031
on the measurement plane
When measuring the source location in magnetic field with this method, ultimate principle is as shown in Figure 1.
Under Maxwell equation quasistatic approximation condition, according to the Biot-Savart law, the magnetic induction of a current dipole generation is in the space:
B z ( x , y ) = μ 0 4 π ( Q x ( y - y 0 ) - Q y ( x - x 0 ) [ ( x - x 0 ) 2 + ( y - y 0 ) 2 + d 2 ] 3 / 2 ) - - - ( 1 )
Wherein, Q xAnd Q yBe the component of magnetic field intensity Q in X and Y direction.Generation is (x by the position coordinates in the current dipole source of measuring magnetic field 0, y 0, z 0), the depth d in current dipole source=-z 0
When the maximum of measuring magnetic field was equal with minimum, the depth d that produces the current dipole source in magnetic field can be calculated with formula
Figure BSA00000379078500041
according to Fig. 1.Wherein, D is coordinate (x on the measurement plane 1, y 1) locate magnetic field maximum B ZmaxAnd coordinate (x y) locates magnetic field minimum B ZminBetween distance.Position (the x of this current source 0, y 0) can calculate with mid-point method.But, actual measurement to magnetic field often be not symmetrically distributed about measurement plane, and be non-linear relation between the parameter of the current source in magnetic field and generation magnetic field, when finding the solution this type of inverse problem, separate not unique.For this reason, we have proposed a kind of new source location method.
Fig. 1 has provided on the detection plane magnetic field maximum and the geometrical relationship of minimum and current source position on two measurement points:
Figure BSA00000379078500042
Wherein,
θ = arcsin ( 6 3 ) - - - ( 4 )
Figure BSA00000379078500045
Figure BSA00000379078500046
Figure BSA00000379078500047
Magnetic field maximum B ZmaxWith magnetic field minimum B ZminCan obtain through measurements and calculations.On the measurement plane, measuring point (x 1, y 1) locate the magnetic field maximum of detected Z direction:
B z max = μ 0 Q 6 π 3 d 2 - - - ( 8 )
Be positioned at (x, magnetic field minimum y):
Figure BSA00000379078500051
Maximum B when known measurement magnetic field ZmaxWith minimum B ZminThe time, Q in formula (8) and (9) and d can be solved by these two equations.Thereby can obtain the current intensity component of current dipole on X and Y direction by (5), (6) and (7) formula, and calculate the plane coordinates of current source by (2) and (3) formula.When the maximum in magnetic field and minimum are not detected, can use detected maximum value of magnetic field and minima approximate substitution.
Implementation step is following:
1. two SQUID probes are aimed at respectively and can be detected magnetic field maximum B ZmaxWith minimum B ZminThe measuring position, and confirm the coordinate of these two measuring points on detection plane, i.e. (x 1, y 1) to locate be magnetic field maximum B Zmax, (x y) is the magnetic field minimum B that measures ZminThe position.
2. according to the minimizing coordinate (x in magnetic field; Y) and computing formula (5), angle
Figure BSA00000379078500052
is obtained in (6)
3. will
Figure BSA00000379078500053
Value and magnetic field maximum B ZmaxAnd coordinate (x 1, y 1), magnetic field minimum B ZminAnd coordinate (x y) brings formula (9) into and obtains the dipole depth d.
4. with formula (2), the X-Y coordinate (x of this current dipole is calculated in (3) 0, y 0).
5. calculate Q according to formula (8).
6. obtain Q according to formula (7) xAnd Q yComponent.
If there is not the time dependent situation of magnetic field peak value and valley, only need two measuring points just can accomplish the calculating of source location according to the method described above usually.Change if measure the peak value and the valley in magnetic field, can obtain the maximum and the minimum of field signal again through interpolation, carry out the current source CALCULATION OF PARAMETERS then through the signal value on the adjacent measuring point.The spacing of each measuring point can be 3.5-4cm.
When gathering field signal, as shown in Figure 2, rule of thumb confirm magnetic field maximum B earlier ZmaxThe position at place, magnetic field minimum B ZminThe right side of maximum normally, position in magnetic field, need rule of thumb search.After the peak value in magnetic field and the measuring position of valley are confirmed, the signal of synchronous detecting cardiac magnetic field on these two measuring points.

Claims (6)

1. measure magnetic field with superconducting quantum interference device and locate the method in field supply source, it is characterized in that this method may further comprise the steps:
1) utilizes field signal on a small amount of measuring point of superconducting quantum interference device collection;
2) obtain each magnetic field maximum and magnetic field minimum constantly according to the field signal that measures;
3) computer is to step 2) in after each magnetic field maximum constantly of trying to achieve and the processing of magnetic field minimum, obtain the position and the intensive parameter in field supply source.
2. according to claim 1ly measure magnetic field and locate the method in field supply source with superconducting quantum interference device; It is characterized in that; Whether counting that field signal need be measured in the described step 1) can come to confirm according to the fixed-site in field supply source; For the Magnetic Field Source of fixed-site, only need two measurement points usually; If the source position periodically changes, then need gather the field signal on several adjacent measurement points, obtain maximum and the minimum of measuring magnetic field through interpolation.
3. a small amount of superconducting quantum interference device measurement point of utilization according to claim 1 carries out the localized method of Magnetic Field Source, it is characterized in that described step 1) and step 2) in field signal comprise X-Y coordinate that each magnetic field value constantly is corresponding with this magnetic field value.
4. according to claim 1ly measure magnetic field and locate the method in field supply source, it is characterized in that described step 3) is specially with superconducting quantum interference device:
31) at first utilize formula
Figure FSA00000379078400011
θ = arcsin ( 6 3 )
Obtain according to magnetic field maximum and minimizing coordinate Value, maximum B in magnetic field on the measurement plane Zmax(x 1, y 1) to magnetic field minimum B Zmin(x, the angle of line D y) and measurement plane X axle does
Figure FSA00000379078400015
32) then, with
Figure FSA00000379078400016
value and step 2) in the magnetic field maximum of trying to achieve and minimum and their position coordinateses on measurement plane bring following formula into:
Figure FSA00000379078400021
Obtain the depth d in field supply source;
33) utilize formula
B z max = μ 0 Q 6 π 3 d 2
Figure FSA00000379078400023
Figure FSA00000379078400024
Figure FSA00000379078400025
Obtain the coordinate (x in magnetic field intensity Q and field supply source 0, y 0), wherein, Q xAnd Q yBe the strength component of this field supply source at X and Y coordinate.
5. according to claim 1ly measure magnetic field and locate the method in field supply source with superconducting quantum interference device; It is characterized in that; Described step 2) in, in the time can obtaining magnetic field maximum and magnetic field minima, just uses the minimum in this minima approximate substitution magnetic field, magnetic field according to field signal.
6. according to claim 1ly measure magnetic field and locate the method in field supply source with superconducting quantum interference device; It is characterized in that; Described step 2) in, in the time can only trying to achieve maximum value of magnetic field and magnetic field minimum, just uses the maximum approximate substitution magnetic field maximum in this magnetic field according to field signal.
CN 201010580178 2010-12-09 2010-12-09 Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field Expired - Fee Related CN102551711B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 201010580178 CN102551711B (en) 2010-12-09 2010-12-09 Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 201010580178 CN102551711B (en) 2010-12-09 2010-12-09 Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field

Publications (2)

Publication Number Publication Date
CN102551711A true CN102551711A (en) 2012-07-11
CN102551711B CN102551711B (en) 2013-10-16

Family

ID=46399289

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 201010580178 Expired - Fee Related CN102551711B (en) 2010-12-09 2010-12-09 Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field

Country Status (1)

Country Link
CN (1) CN102551711B (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107092033A (en) * 2017-04-19 2017-08-25 中南大学 It is a kind of to be used to regulate and control the method for measurement signal intensity
CN109375368A (en) * 2018-10-24 2019-02-22 泉州师范学院 A kind of production method of the multifocal spot array of three-dimensional based on space Dipole Arrays
CN110850483A (en) * 2019-11-12 2020-02-28 中国船舶重工集团公司第七一九研究所 Underwater target detection and positioning method based on electric field electrode array arrangement

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000325323A (en) * 1999-05-20 2000-11-28 Shimadzu Corp Organism action current source estimating device
CN1552285A (en) * 2003-05-26 2004-12-08 中国科学院物理研究所 Magnetocardiogram and its analyzing method
US7521708B1 (en) * 2004-12-29 2009-04-21 The United States Of America As Represented By The Secretary Of The Navy High sensitivity ring-SQUID magnetic sensor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000325323A (en) * 1999-05-20 2000-11-28 Shimadzu Corp Organism action current source estimating device
CN1552285A (en) * 2003-05-26 2004-12-08 中国科学院物理研究所 Magnetocardiogram and its analyzing method
US7521708B1 (en) * 2004-12-29 2009-04-21 The United States Of America As Represented By The Secretary Of The Navy High sensitivity ring-SQUID magnetic sensor

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
张磊等: "基于单电流偶极子的心脏磁场反演计算", 《现代医学仪器》 *
石明伟等: "浅谈心脏磁场的检测及心脏源模型建模", 《硅谷》 *

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107092033A (en) * 2017-04-19 2017-08-25 中南大学 It is a kind of to be used to regulate and control the method for measurement signal intensity
CN107092033B (en) * 2017-04-19 2019-06-11 中南大学 A method of for regulating and controlling measuring signal intensity
CN109375368A (en) * 2018-10-24 2019-02-22 泉州师范学院 A kind of production method of the multifocal spot array of three-dimensional based on space Dipole Arrays
CN110850483A (en) * 2019-11-12 2020-02-28 中国船舶重工集团公司第七一九研究所 Underwater target detection and positioning method based on electric field electrode array arrangement
CN110850483B (en) * 2019-11-12 2021-09-14 中国船舶重工集团公司第七一九研究所 Underwater target detection and positioning method based on electric field electrode array arrangement

Also Published As

Publication number Publication date
CN102551711B (en) 2013-10-16

Similar Documents

Publication Publication Date Title
CN106772639B (en) Underground irony pipeline buried depth magnetic dipole structured approach Optimization inversion
CN108152687B (en) Power transformer partial discharge positioning method utilizing ultrasonic inversion
CN102151149A (en) Method and system for automatically measuring ultrasound image of fetus
CN107328849A (en) Thinning detecting system and thinning detection method
CN105043381A (en) Magnetic nail-based positioning method
CN112525201B (en) Underwater target tracking method based on electromagnetic field characteristic multi-information fusion
CN207440306U (en) A kind of buried abandoned well detection device
CN108151766A (en) Localization method, magnetic nail positioning navigation error correcting method and the positioning device of magnetic nail
CN102621582A (en) Method for detecting positions of underground metal pipelines by aid of space vector method and device
CN102809687B (en) Digital measurement method for alternating-current frequency
CN109799279A (en) A kind of ferromagnetic conduit stress mornitoring and monitoring method
CN110161572A (en) A kind of horizontal topological structure quick nondestructive detection system of grounded screen and method
CN102551711B (en) Method for measuring magnetic field by aid of superconducting quantum interference device and positioning current source of magnetic field
CN103292773A (en) Symmetry error evaluation method based on minimum zone
CN106483583B (en) Positioning system, method and the electronic tag survey meter of electronic tag
CN102573055B (en) Method for locating nodes in wireless sensor network
CN103673912A (en) Image correcting system for deformation measurement of speckle correlation methods
CN110471118A (en) A kind of detection method of ultra-deep underground utilities sectional elevation
CN112503399B (en) Method and device for determining underground pipeline position and storage medium thereof
CN109683203A (en) A kind of earthquake ground dipole interference source localization method and system in electricity observation
CN105572671A (en) Spatial positioning device based on local coordinate system and system and method thereof
CN102928666B (en) Digital measurement method for phase difference of alternating current
CN114236620A (en) Metal pipeline positioning method and device
CN208704763U (en) A kind of magnetic field induction positioning device
CN110687609B (en) Method for eliminating interference of parallel pipelines in detection of alternating current and direct current stray currents of buried pipelines

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
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20131016

Termination date: 20161209