CN114415073B - Ground quick calibration method and system for aeromagnetic vector gradiometer error model - Google Patents

Ground quick calibration method and system for aeromagnetic vector gradiometer error model Download PDF

Info

Publication number
CN114415073B
CN114415073B CN202210319138.2A CN202210319138A CN114415073B CN 114415073 B CN114415073 B CN 114415073B CN 202210319138 A CN202210319138 A CN 202210319138A CN 114415073 B CN114415073 B CN 114415073B
Authority
CN
China
Prior art keywords
sensor
axis
vector
calibration
error
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.)
Expired - Fee Related
Application number
CN202210319138.2A
Other languages
Chinese (zh)
Other versions
CN114415073A (en
Inventor
常明
徐磊
杨勇
林春生
张建强
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.)
Naval University of Engineering PLA
Original Assignee
Naval University of Engineering PLA
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 Naval University of Engineering PLA filed Critical Naval University of Engineering PLA
Priority to CN202210319138.2A priority Critical patent/CN114415073B/en
Publication of CN114415073A publication Critical patent/CN114415073A/en
Application granted granted Critical
Publication of CN114415073B publication Critical patent/CN114415073B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/0023Electronic aspects, e.g. circuits for stimulation, evaluation, control; Treating the measured signals; calibration
    • G01R33/0035Calibration of single magnetic sensors, e.g. integrated calibration
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux
    • G01R33/022Measuring gradient
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V13/00Manufacturing, calibrating, cleaning, or repairing instruments or devices covered by groups G01V1/00 – G01V11/00
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/15Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for use during transport, e.g. by a person, vehicle or boat
    • G01V3/16Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for use during transport, e.g. by a person, vehicle or boat specially adapted for use from aircraft
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/15Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for use during transport, e.g. by a person, vehicle or boat
    • G01V3/165Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for use during transport, e.g. by a person, vehicle or boat operating with magnetic or electric fields produced or modified by the object or by the detecting device

Landscapes

  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • Geophysics (AREA)
  • Environmental & Geological Engineering (AREA)
  • Geology (AREA)
  • Remote Sensing (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Aviation & Aerospace Engineering (AREA)
  • Electromagnetism (AREA)
  • Manufacturing & Machinery (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

The invention is suitable for the technical field of unmanned aerial vehicle aeromagnetic measurement calibration, and provides a ground quick calibration method of an aeromagnetic vector gradiometer error model, which comprises the following steps: establishing a vector gradiometer coordinate system according to the unmanned aerial vehicle body information; establishing a linear independent error calibration model based on the coordinate system; performing learning training according to the shaking rule of the simulated unmanned aerial vehicle; and obtaining error calibration parameters based on a solving method of multiple linear regression. The invention correspondingly provides a system for realizing the method. Therefore, the method and the device can quickly solve the error calibration parameters, can better correct the structural error of the aeromagnetic vector gradient detection system, and has stronger adaptability to the change of the field measurement place for the model calibration parameters.

Description

Ground quick calibration method and system for aeromagnetic vector gradiometer error model
Technical Field
The invention relates to the technical field of unmanned aerial vehicle magnetic field gradient measurement calibration, in particular to a ground quick calibration method and a ground quick calibration system for an aeromagnetic vector gradiometer error model.
Background
The vector gradient detector carried on the unmanned platform can realize high-efficiency detection and positioning of target magnetic anomaly information such as underground pipelines, buried objects, geologic bodies, submarines, mines and the like, but the data quality is influenced due to process errors and installation errors among all axial directions of the vector magnetic detector, so that the detection precision is greatly reduced, and meanwhile, the errors can also bring great interference to detection data when the platform swings, and the detection operation cannot be finished.
In the existing actual error calibration work, there are the inconveniences that the dependence on high-precision measuring equipment is strong and the requirement on a uniform magnetic environment is high, so that the improvement is needed.
Disclosure of Invention
In view of the above-mentioned shortcomings, the present invention provides a ground fast calibration method and system for an error model of an aeromagnetic vector gradiometer, which can conveniently correct the error of an aeromagnetic vector gradient detection system in the field, get rid of the harsh laboratory condition limitation, and have strong adaptability to the change of the field measurement location for the model calibration parameters.
In order to achieve the purpose, the invention provides a ground quick calibration method for an error model of an aeromagnetic vector gradiometer, which is characterized by comprising the following steps:
establishing a coordinate system of the vector gradient magnetic detector according to the unmanned aerial vehicle body information;
establishing a linear independent error calibration model based on the coordinate system;
performing learning training according to the shaking rule of the simulated unmanned aerial vehicle;
and obtaining error calibration parameters based on a solving method of multiple linear regression.
According to the calibration method of the invention, the number of the vector gradient magnetic probes is 1.
According to the calibration method, the calibration model measures the structural error and the relative null shift error between the corresponding axial directions of the two triaxial fluxgate sensors.
According to the calibration method, the step of training learning according to the shaking rule of the simulated unmanned aerial vehicle comprises the following steps:
the ground shaking measurement system composed of the three-axis nonmagnetic turntable and the vector gradient magnetic detector is used for respectively combining the measurement data of the upper hemisphere space and the lower hemisphere space to serve as a training sample for full-attitude traversing shaking.
According to the calibration method of the present invention, the step of establishing a linear independent error calibration model based on the coordinate system comprises:
establishing a projection relation between two triaxial fluxgate sensors;
and establishing a corresponding mathematical expression according to a preset calculation formula.
The invention correspondingly provides a ground rapid calibration system of an error model of an aeromagnetic vector gradiometer, which comprises
The coordinate system generating unit is used for establishing a vector gradiometer coordinate system according to the unmanned aerial vehicle body information;
the model establishing unit is used for establishing a linear independent error calibration model according to the coordinate system;
the shaking setting unit is used for learning and training according to the shaking posture of the simulated unmanned aerial vehicle;
and the calculating unit is used for obtaining the error calibration parameters based on a solving method of multiple linear regression.
According to the system of the invention, the number of the vector gradient magnetic probes is 1.
According to the system, the calibration model measures the structural error and the relative null shift error between the corresponding axial directions of the two triaxial fluxgate sensors.
According to the system, the shake setting unit is used for combining the measurement data of the upper hemisphere space and the lower hemisphere space respectively through a ground shake measurement system consisting of the three-axis nonmagnetic turntable and the vector gradient magnetic detector to serve as a training sample for full-attitude traversing shake.
According to the system of the invention, the computing unit is further configured to establish a projection relationship between the two three-axis fluxgate sensors;
and establishing a corresponding mathematical expression according to a preset calculation formula.
The invention is suitable for the technical field of unmanned aerial vehicle aeromagnetic measurement calibration, and provides a ground quick calibration method of an aeromagnetic vector gradiometer error model, which comprises the following steps: establishing a vector gradient magnetic detector coordinate system according to the unmanned aerial vehicle body information; establishing a linear independent error calibration model based on the coordinate system; performing learning training according to the shaking rule of the simulated unmanned aerial vehicle; and obtaining error calibration parameters based on a solving method of multiple linear regression. The invention correspondingly provides a system for realizing the method. Therefore, the method can quickly solve error calibration parameters, can better correct the structural error of the aeromagnetic vector gradient detection system, and has stronger adaptability to the change of field measurement places.
Drawings
FIG. 1 is a schematic flow chart of the method of the present invention;
FIG. 2 is a schematic diagram of the vector gradient magnetic probe of the present invention;
3(a) -3 (e) are graphs of vector gradient linear independent error calibration models of the present invention;
FIGS. 4(a) -4 (f) are pre-and post-error calibration contrast plots based on multiple linear regression;
5(a) -5 (f) comparison plots of error calibration based on multiple linear regression after a site change;
fig. 6(a) -6 (f) calibrate the sloshing error contrast map for site 2 with the calibration parameters for site 1.
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more apparent, the present invention is described in further detail below with reference to the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are merely illustrative of the invention and are not intended to limit the invention.
Referring to fig. 1, the invention provides a ground fast calibration method for an error model of an aeromagnetic vector gradiometer, which comprises the following steps:
and S101, establishing a vector gradiometer coordinate system according to the unmanned aerial vehicle body information.
With reference to fig. 2, the coordinate system of the unmanned aerial vehicle body is a front-right-lower right-hand sequence, three axial directions of two three-axis fluxgate sensors (hereinafter referred to as "Sensor-1" and "Sensor-2") are converged at respective central points, and the coordinate system is also constructed according to the front-right-lower right-hand sequence
Figure 738151DEST_PATH_IMAGE001
And (c).
Figure 989004DEST_PATH_IMAGE002
And S102, establishing a linear independent error calibration model based on the coordinate system.
In this step, a projection relationship is first established. Translating the Sensor-2 to the Sensor-1 to make the centers of the two vector magnetic detectors coincide, respectively taking Axis-11, Axis-12 and Axis-13 axes of the Sensor-1 as references as shown in FIG. 3(a), and respectively projecting three axes of the Sensor-2 on each axial direction of the Sensor-1 to obtain 9 projection parameters as shown in FIG. 3(b), FIG. 3(c) and FIG. 3 (d);
the notation is simplified. The actual output values of the magnetic fields of the Sensor-1 in three non-orthogonal axial directions are
Figure 829921DEST_PATH_IMAGE003
Figure 431804DEST_PATH_IMAGE004
And
Figure 750789DEST_PATH_IMAGE005
the actual output value of the magnetic field of Sensor-2 is
Figure 856149DEST_PATH_IMAGE006
Figure 867967DEST_PATH_IMAGE007
And
Figure 425987DEST_PATH_IMAGE008
as shown in fig. 3 (e).
Write the projection expression of Sensor-2 to Axis-11 Axis of Sensor-1
Figure 548664DEST_PATH_IMAGE009
In the formula
Figure 774109DEST_PATH_IMAGE010
For the estimate of the Sensor-2 projection,
Figure 691249DEST_PATH_IMAGE011
Figure 2145DEST_PATH_IMAGE012
and
Figure 928513DEST_PATH_IMAGE013
the projection coefficients of Axis-11 of Sensor-1 in the three axial directions of Sensor-2 are shown respectively.
S102-1 writes a gradient expression in Axis-11 axial direction
Figure 742885DEST_PATH_IMAGE014
In the formula
Figure 96506DEST_PATH_IMAGE015
Showing the relative null shift of the Axis-11 up the two magnetic probes.
S102-2 deforms Axis-11 in an axial gradient expression mode
Figure 894698DEST_PATH_IMAGE016
In the formula
Figure 359177DEST_PATH_IMAGE017
Figure 28056DEST_PATH_IMAGE018
Figure 552578DEST_PATH_IMAGE019
Written in a compact form having
Figure 838066DEST_PATH_IMAGE020
S102-3 writing out gradient expressions in other two axial directions
Figure 840657DEST_PATH_IMAGE021
In the formula
Figure 895201DEST_PATH_IMAGE022
Is the relative null shift on Axis-12,
Figure 856203DEST_PATH_IMAGE023
Figure 97829DEST_PATH_IMAGE024
Figure 904111DEST_PATH_IMAGE025
Figure 78740DEST_PATH_IMAGE026
in the formula
Figure 679486DEST_PATH_IMAGE027
Is the relative null shift on Axis-13,
Figure 939566DEST_PATH_IMAGE028
Figure 278100DEST_PATH_IMAGE029
Figure 307236DEST_PATH_IMAGE030
s102-4, establishing an error model of the vector gradient with linear independence between axial directions
Figure 78883DEST_PATH_IMAGE031
S102-5 writing 9 projection parameters into a matrix form
Figure 560680DEST_PATH_IMAGE032
Then (1)
Figure 974344DEST_PATH_IMAGE011
Figure 592407DEST_PATH_IMAGE012
Figure 800534DEST_PATH_IMAGE013
Figure 504048DEST_PATH_IMAGE033
Figure 455824DEST_PATH_IMAGE034
Figure 193973DEST_PATH_IMAGE035
Figure 307422DEST_PATH_IMAGE036
Figure 763811DEST_PATH_IMAGE037
Figure 253698DEST_PATH_IMAGE038
) And (a)
Figure 111933DEST_PATH_IMAGE039
Figure 927442DEST_PATH_IMAGE040
Figure 605548DEST_PATH_IMAGE041
) Together constituting linearly independent error calibration model parameters.
And S103, performing learning training according to the shaking rule of the simulated unmanned aerial vehicle.
According to the ground shaking measuring system, the three-axis nonmagnetic turntable and the vector gradient magnetic detector are used for combining the measuring data of the upper hemisphere space and the lower hemisphere space respectively to serve as training data of full-attitude traversing shaking, so that the resolving stability and the environmental adaptability of the calibration parameters are improved.
In one test embodiment of the invention, the three-axis non-magnetic turntable shaking test system is provided. And simulating the flight attitude of the unmanned aerial vehicle to perform a shaking test. The carbon fiber pipe forming the vector gradient magnetic detector is fixed in the center of the platform of the three-axis nonmagnetic turntable, the nonmagnetic turntable does not contain a motor, and the vector gradient magnetic detector can swing freely through manual operation to realize the swinging postures of the vector gradient magnetic detector in different directions.
The test procedure was as follows:
s103-1, selecting a measuring place 1. Regarding the geomagnetic field as a uniform constant field, and keeping Axis-13 and Axis-23 of the vector gradient magnetic detector in a fixed state (called a 'lying posture' for short) which is vertical to the ground downwards;
s103-2, traversing and shaking the upper hemisphere space. According to the sequence of east → south → west → north, the three degrees of freedom of yaw, pitch and roll are synthesized under each azimuth to carry out arbitrary shaking of 8-10 periods, the amplitude of each rotation angle is controlled within +/-20 degrees, and magnetic field data are collected;
s103-3, changing the fixed orientation of the gradient rod. Continuously acquiring data without power interruption, and adjusting Axis-13 and Axis-23 axes of the vector gradient magnetic detector pointing to the earth center to point to the sky (called 'lying posture' for short);
s103-4, traversing and shaking the lower hemisphere space. After the step of S103-2 shaking is repeated, stopping Data acquisition to obtain measurement Data-1 traversed in the global surface space of the measurement site 1;
substituting the output data of each axis of the measuring site 1 into an error calibration equation set to obtain 12 error calibration coefficients, calculating the error output after the calibration based on the multiple linear regression through the formula (4), and comparing the error output with the difference value of the original output value of the vector magnetic detector. FIG. 4(a), FIG. 4(c) and FIG. 4(e) are the difference values of the raw data measured in three axial directions; fig. 4(b), 4(d) and 4(f) are graphs showing the difference values between the three axes after calibration based on the multiple linear regression method, and the unit is nT.
In fig. 4(a) to 4(f), the interference of larger amplitude caused by changing the fixed state and the azimuth conversion is eliminated, and the peak-to-peak value of the actually measured shaking curve is counted as follows:
Figure 899126DEST_PATH_IMAGE042
with reference to fig. 4(b), 4(d), 4(f) and table 1, the gradient data in the three axial directions after error calibration has a decrease in the shake error of 89% or more as compared to that before calibration.
S103-5, moving the measuring place. And (3) translating the three-axis nonmagnetic rotary table to the east by 5 meters to serve as a measurement place 2, repeating the processes from S103-1 to S103-4, recording output Data, and recording the Data as Data-2.
Comparing fig. 4(a) to fig. 4(f) and fig. 5(a) to fig. 5(f), it is found that the influence of the azimuth and attitude shake can be significantly eliminated after error calibration is performed again at different locations, and the error calibration effect of the peak-to-peak value of the shake interference before and after calibration at the location 2 can also reach more than 91%, see table 2.
Figure 346288DEST_PATH_IMAGE043
And S103-6, solving parameters and analyzing performance. And substituting the error calibration parameters calculated by the Data-1 into the Data-2 so as to verify the applicability of the error calibration model to the position change. The new calibration results are shown in fig. 6(a) -6 (f).
The error correction data in each axial direction in fig. 6(a) to 6(f) are summarized as follows:
Figure 67119DEST_PATH_IMAGE044
it can be seen from table 3 that, by using the calibration parameters of site 1 to correct the sway data of site 2, the calibration effect can still be maintained above 89%, and better calibration can be performed on the influence of changing the direction and the influence of sway attitude. The calibration effect is based on a calibration result randomly generated under a +/-20-degree large-angle shaking condition, and when the unmanned aerial vehicle carries out aeromagnetic detection, the unmanned aerial vehicle adopts flat flight (namely shaking in a small angle), which indicates that the calibration method can meet the small-angle shaking interference when the unmanned aerial vehicle carries out flat flight detection.
The above processes show that the error calibration parameters have good environmental adaptability, and show that the learning process of full-space posture traversal is adopted during learning training, so that the influence on the replacement place is certain in adaptability.
And step S104, obtaining error calibration parameters based on a solving method of multiple linear regression.
S104-1 constructs a cost function. Ideally, the calibrated error should be zero, and the left side of equation (4) is zero. Take the formula (1) as an example
Figure 232522DEST_PATH_IMAGE045
The cost function is constructed such that it satisfies the minimum in the sense of a 2-norm sum of squares, i.e. it is
Figure 329791DEST_PATH_IMAGE046
Figure 897038DEST_PATH_IMAGE047
Indicating the measured second set of data,
Figure 788771DEST_PATH_IMAGE048
the total number of data obtained.
S104-2, the right side of the formula (6) is used for solving partial derivatives of the error parameters, and the partial derivatives are zero, so that
Figure 707048DEST_PATH_IMAGE049
The equation set is simplified and written into a matrix form, and then
Figure 76850DEST_PATH_IMAGE050
S104-3, obtaining an error calibration parameter solving matrix on the Axis-12 in the same way
Figure 498604DEST_PATH_IMAGE051
S104-4, obtaining an error calibration parameter solving matrix on Axis-13 in the same way
Figure 826817DEST_PATH_IMAGE052
And (S104-5) simultaneously establishing the formula (7), the formula (8), the formula (9) and the formula (5), and solving all calibration parameters of the linear independent error model between the Sensor-1 and the Sensor-2 of the magnetic field vector gradiometer.
Through the modeling and actual measurement calculation examples, the linear independent error calibration model constructed by the method has the following three advantages: on the premise of not considering the non-orthogonal calibration among three axial directions, the error calibration model is constructed with fewer parameters, is convenient to solve and is beneficial to fast learning; the learning training of random shaking can be carried out under the manual control, the mode gets rid of the limitation of higher rotation precision requirement on the instrument and equipment, and the operation threshold of carrying out precise calibration on the gradiometer in the field is reduced. Error calibration parameters after the place is changed still have good environmental adaptability, and a foundation is laid for the unmanned aerial vehicle carrying vector gradient magnetic detector to carry out ground rapid technology.
The invention also provides a system, which comprises:
and the coordinate system generating unit is used for establishing a vector gradiometer coordinate system according to the unmanned aerial vehicle body information.
And the model establishing unit is used for establishing a linear independent error calibration model according to the coordinate system.
The shaking setting unit is used for learning and training according to the shaking posture of the simulated unmanned aerial vehicle; the shaking setting unit is used for merging the measurement data of the upper hemisphere space and the lower hemisphere space respectively through a ground shaking measurement system consisting of a three-axis nonmagnetic turntable and a vector gradient magnetic detector, and the merged measurement data are used as training samples for full-attitude traversal shaking.
And the calculation unit is used for obtaining error calibration parameters based on a solving method of multiple linear regression, and can establish a projection relation between the two triaxial fluxgate sensors.
In the system, the number of the vector gradient magnetic detectors is 1, and the calibration model measures the structural error and the relative null shift error between the corresponding axial directions of the two triaxial fluxgate sensors.
In summary, the invention is applicable to the technical field of unmanned aerial vehicle aeromagnetic measurement calibration, and provides a ground rapid calibration method for an aeromagnetic vector gradiometer error model, which comprises the following steps: establishing a vector gradient magnetic detector coordinate system according to the unmanned aerial vehicle body information; establishing a linear independent error calibration model based on the coordinate system; performing learning training according to the shaking rule of the simulated unmanned aerial vehicle; and solving the error calibration parameters based on the multiple linear regression to obtain the calibration parameters. The invention correspondingly provides a system for realizing the method. Therefore, the method can quickly solve the error calibration parameters, can better correct the structural error and the relative null shift error of the aeromagnetic vector gradient detection system, and has stronger adaptability to the change of the field measurement place.
The present invention is capable of other embodiments, and various changes and modifications can be made by one skilled in the art without departing from the spirit and scope of the invention.

Claims (8)

1. A ground quick calibration method for an error model of an aeromagnetic vector gradiometer is characterized by comprising the following steps:
establishing a vector gradient magnetic detector coordinate system according to unmanned aerial vehicle body information: three axial directions of two three-axis fluxgate sensors Sensor-1 and Sensor-2 are preset to be intersected at respective central points,constructing a coordinate system according to a front-right-bottom right-hand order
Figure 509224DEST_PATH_IMAGE001
And
Figure 143467DEST_PATH_IMAGE002
establishing a linear independent error calibration model based on the coordinate system;
performing learning training according to the shaking rule of the simulated unmanned aerial vehicle;
obtaining error calibration parameters based on a solving method of multiple linear regression;
the step of establishing a linear independent error calibration model based on the coordinate system comprises the following steps:
firstly, establishing a projection relation, translating the Sensor-2 to the Sensor-1, enabling the centers of the two vector magnetic detectors to coincide, and respectively taking Axis-11, Axis-12 and Axis-13 axes of the Sensor-1 as references and respectively projecting three axes of the Sensor-2 in each axial direction of the Sensor-1 to obtain 9 projection parameters;
setting the actual output values of the magnetic fields in the three non-orthogonal axial directions of the Sensor-1 as
Figure 443999DEST_PATH_IMAGE003
Figure 480088DEST_PATH_IMAGE004
And
Figure 309504DEST_PATH_IMAGE005
the actual output value of the magnetic field of Sensor-2 is
Figure 431043DEST_PATH_IMAGE006
Figure 535266DEST_PATH_IMAGE007
And
Figure 894703DEST_PATH_IMAGE008
write the projection expression of Sensor-2 to Axis-11 Axis of Sensor-1
Figure 426178DEST_PATH_IMAGE009
In the formula
Figure 267970DEST_PATH_IMAGE010
For the estimate of the Sensor-2 projection,
Figure 175883DEST_PATH_IMAGE011
Figure 655406DEST_PATH_IMAGE012
and
Figure 357783DEST_PATH_IMAGE013
the projection coefficients of the three axial directions of the Sensor-2 on the Axis-11 of the Sensor-1 are respectively;
writing an Axis-11 axial gradient expression
Figure 922756DEST_PATH_IMAGE014
In the formula
Figure 368781DEST_PATH_IMAGE015
Represents the relative zero drift of the Axis-11 two magnetic detectors upwards;
deforming the gradient expression of Axis-11 in the axial direction
Figure 968390DEST_PATH_IMAGE016
In the formula
Figure 576089DEST_PATH_IMAGE017
Figure 893938DEST_PATH_IMAGE018
Figure 878074DEST_PATH_IMAGE019
Written in a compact form, having
Figure 597768DEST_PATH_IMAGE020
Writing out gradient expressions in two other axial directions
Figure 376369DEST_PATH_IMAGE021
In the formula
Figure DEST_PATH_IMAGE022
Is the relative null shift on Axis-12,
Figure 414470DEST_PATH_IMAGE023
Figure 936718DEST_PATH_IMAGE024
Figure 510919DEST_PATH_IMAGE025
Figure 725999DEST_PATH_IMAGE026
in the formula
Figure 752861DEST_PATH_IMAGE027
Is the relative null shift on Axis-13,
Figure 78800DEST_PATH_IMAGE028
Figure 507508DEST_PATH_IMAGE029
Figure 893489DEST_PATH_IMAGE030
establishing an error model of vector gradients that is linearly independent between axial directions
Figure 407647DEST_PATH_IMAGE031
Writing 9 projection parameters in matrix form
Figure 537277DEST_PATH_IMAGE032
Then (a)
Figure 820491DEST_PATH_IMAGE011
Figure 642954DEST_PATH_IMAGE012
Figure 877364DEST_PATH_IMAGE013
Figure DEST_PATH_IMAGE033
Figure 545105DEST_PATH_IMAGE034
Figure 682826DEST_PATH_IMAGE035
Figure 410610DEST_PATH_IMAGE036
Figure 899360DEST_PATH_IMAGE037
Figure 370793DEST_PATH_IMAGE038
) And (a)
Figure 628599DEST_PATH_IMAGE039
Figure 527285DEST_PATH_IMAGE040
Figure 237752DEST_PATH_IMAGE041
) Together, constitute the linearly independent error calibration model parameters.
2. The calibration method according to claim 1, wherein the number of the vector gradient magnetic probes is 1.
3. The calibration method according to claim 1, wherein the calibration model measures structural errors and relative null shift errors between corresponding axial directions of the two tri-axial fluxgate sensors.
4. The calibration method according to claim 1, wherein the step of training learning according to the law of shaking imitating the unmanned aerial vehicle comprises:
the ground shaking measurement system composed of the three-axis nonmagnetic turntable and the vector gradient magnetic detector is used for respectively combining the measurement data of the upper hemisphere space and the lower hemisphere space to serve as a training sample for full-attitude traversing shaking.
5. A ground rapid calibration system for an error model of an aeromagnetic vector gradiometer is characterized by comprising
A coordinate system generating unit for establishing a vector gradient magnetic detector coordinate system according to the unmanned aerial vehicle body information, and presetting three axial intersections of two triaxial fluxgate sensors Sensor-1 and Sensor-2 in eachA central point, constructing a coordinate system according to a front-right-lower right-hand order
Figure 512876DEST_PATH_IMAGE042
And
Figure 890767DEST_PATH_IMAGE043
the model establishing unit is used for establishing a linear independent error calibration model according to the coordinate system;
the shaking setting unit is used for learning and training according to the shaking rule of the simulated unmanned aerial vehicle;
the calculation unit is used for obtaining error calibration parameters based on a solving method of multiple linear regression;
the model building unit is specifically configured to:
firstly, establishing a projection relation, translating the Sensor-2 to the Sensor-1, enabling the centers of the two vector magnetic detectors to coincide, and respectively taking Axis-11, Axis-12 and Axis-13 axes of the Sensor-1 as references and respectively projecting three axes of the Sensor-2 in each axial direction of the Sensor-1 to obtain 9 projection parameters;
setting the actual output values of the magnetic fields in the three non-orthogonal axial directions of the Sensor-1 as
Figure 960354DEST_PATH_IMAGE003
Figure 992590DEST_PATH_IMAGE004
And
Figure 805825DEST_PATH_IMAGE005
the actual output value of the magnetic field of Sensor-2 is
Figure 38224DEST_PATH_IMAGE006
Figure 13133DEST_PATH_IMAGE007
And
Figure 963771DEST_PATH_IMAGE008
write the projection expression of Sensor-2 to Axis-11 Axis of Sensor-1
Figure 580698DEST_PATH_IMAGE044
In the formula
Figure 667602DEST_PATH_IMAGE045
For the estimate of the Sensor-2 projection,
Figure 344571DEST_PATH_IMAGE011
Figure 251347DEST_PATH_IMAGE012
and
Figure 406385DEST_PATH_IMAGE013
the projection coefficients of the three axial directions of the Sensor-2 on the Axis-11 of the Sensor-1 are respectively;
writing an Axis-11 axial gradient expression
Figure 613376DEST_PATH_IMAGE046
In the formula
Figure 930087DEST_PATH_IMAGE047
Represents the relative zero drift of the Axis-11 two magnetic detectors upwards;
deforming the gradient expression of Axis-11 in the axial direction
Figure 88274DEST_PATH_IMAGE016
In the formula
Figure 47003DEST_PATH_IMAGE017
Figure 108500DEST_PATH_IMAGE018
Figure 861692DEST_PATH_IMAGE019
Written in a compact form, having
Figure 8640DEST_PATH_IMAGE020
Writing out gradient expressions in two other axial directions
Figure 505480DEST_PATH_IMAGE021
In the formula
Figure 155904DEST_PATH_IMAGE048
Is the relative null shift on Axis-12,
Figure 345577DEST_PATH_IMAGE023
Figure 979821DEST_PATH_IMAGE024
Figure 280352DEST_PATH_IMAGE025
Figure 785283DEST_PATH_IMAGE026
in the formula
Figure 145857DEST_PATH_IMAGE049
Is the relative null shift on Axis-13,
Figure 267397DEST_PATH_IMAGE028
Figure 338996DEST_PATH_IMAGE029
Figure 229591DEST_PATH_IMAGE030
establishing an error model of vector gradients that is linearly independent between axial directions
Figure 761067DEST_PATH_IMAGE050
Writing 9 projection parameters in matrix form
Figure 104323DEST_PATH_IMAGE051
Then (1)
Figure 746657DEST_PATH_IMAGE011
Figure 491759DEST_PATH_IMAGE012
Figure 194136DEST_PATH_IMAGE013
Figure 24689DEST_PATH_IMAGE033
Figure 939555DEST_PATH_IMAGE034
Figure 804743DEST_PATH_IMAGE035
Figure 678021DEST_PATH_IMAGE036
Figure 995870DEST_PATH_IMAGE037
Figure 212963DEST_PATH_IMAGE038
) And (a)
Figure 932657DEST_PATH_IMAGE039
Figure 976836DEST_PATH_IMAGE040
Figure 781981DEST_PATH_IMAGE041
) Together, constitute the linearly independent error calibration model parameters.
6. The system of claim 5, wherein the number of vector gradient magnetometers is 1.
7. The system of claim 5, wherein the calibration model measures structural and relative null shift errors between corresponding axes of the two tri-axis fluxgate sensors.
8. The system according to claim 5, wherein the shake setting unit is configured to combine the measurement data of the upper hemispherical space and the lower hemispherical space, respectively, as a training sample for full-attitude traverse shake, by a ground shake measurement system composed of a three-axis nonmagnetic turntable and a vector gradient magnetic probe.
CN202210319138.2A 2022-03-29 2022-03-29 Ground quick calibration method and system for aeromagnetic vector gradiometer error model Expired - Fee Related CN114415073B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202210319138.2A CN114415073B (en) 2022-03-29 2022-03-29 Ground quick calibration method and system for aeromagnetic vector gradiometer error model

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202210319138.2A CN114415073B (en) 2022-03-29 2022-03-29 Ground quick calibration method and system for aeromagnetic vector gradiometer error model

Publications (2)

Publication Number Publication Date
CN114415073A CN114415073A (en) 2022-04-29
CN114415073B true CN114415073B (en) 2022-08-09

Family

ID=81263451

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202210319138.2A Expired - Fee Related CN114415073B (en) 2022-03-29 2022-03-29 Ground quick calibration method and system for aeromagnetic vector gradiometer error model

Country Status (1)

Country Link
CN (1) CN114415073B (en)

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AU2002366366A1 (en) * 2001-12-18 2003-06-30 Bhp Billiton Innovation Pty Ltd Method of processing marine magnetic gradient data and exploration methods using that data
CN101923152A (en) * 2010-06-25 2010-12-22 中国科学院上海微系统与信息技术研究所 Room temperature calibration method for equivalent error area of gradiometer
CN104345348A (en) * 2014-11-07 2015-02-11 吉林大学 Device and method for obtaining relevant parameters of aviation superconductive full-tensor magnetic gradient measuring system
CN105891755A (en) * 2016-02-25 2016-08-24 吉林大学 Aircraft hanging-type fluxgate magnetic gradient tensor instrument correction method
CN106940454A (en) * 2017-04-27 2017-07-11 吉林大学 The ground simulation method and system of Caliberation Flight in the detection of magnetic air gradient tensor
CN109633494A (en) * 2019-01-14 2019-04-16 北京卫星环境工程研究所 Spacecraft Distribution of Magnetic Field information imaging method
CN113281824A (en) * 2021-05-19 2021-08-20 北京大学 Aviation magnetic compensation method considering airplane non-rigidity and polarized current factors

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9671226B2 (en) * 2014-12-17 2017-06-06 Honeywell International Inc. Magnetic sensor calibration for aircraft

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AU2002366366A1 (en) * 2001-12-18 2003-06-30 Bhp Billiton Innovation Pty Ltd Method of processing marine magnetic gradient data and exploration methods using that data
CN101923152A (en) * 2010-06-25 2010-12-22 中国科学院上海微系统与信息技术研究所 Room temperature calibration method for equivalent error area of gradiometer
CN104345348A (en) * 2014-11-07 2015-02-11 吉林大学 Device and method for obtaining relevant parameters of aviation superconductive full-tensor magnetic gradient measuring system
CN105891755A (en) * 2016-02-25 2016-08-24 吉林大学 Aircraft hanging-type fluxgate magnetic gradient tensor instrument correction method
CN106940454A (en) * 2017-04-27 2017-07-11 吉林大学 The ground simulation method and system of Caliberation Flight in the detection of magnetic air gradient tensor
CN109633494A (en) * 2019-01-14 2019-04-16 北京卫星环境工程研究所 Spacecraft Distribution of Magnetic Field information imaging method
CN113281824A (en) * 2021-05-19 2021-08-20 北京大学 Aviation magnetic compensation method considering airplane non-rigidity and polarized current factors

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
Factor Analysis on Integrated Error Model of Magnetic Gradient Tensor;Lei Xu等;《IEEE SENSORS JOURNAL》;20210701;全文 *
航磁矢量测量的误差分析和补偿算法研究;缪林良等;《电子测量与仪器学报》;20211231;全文 *

Also Published As

Publication number Publication date
CN114415073A (en) 2022-04-29

Similar Documents

Publication Publication Date Title
CN107272069B (en) Magnetic target method for tracing based on magnetic anomaly gradient
JP4093861B2 (en) Compensation of large magnetic errors for electronic compass and all orientation operations
CN107544042B (en) Magnetometer array correction method
CN110146839A (en) A kind of mobile platform magnetic gradient tensor system compensation method
CN113008227B (en) Geomagnetic binary measurement method for measuring attitude based on three-axis accelerometer
CN105804722A (en) Correction method for mining borehole clinometer probe tube
CN102252689A (en) Electronic compass calibration method based on magnetic sensor
CN106767671B (en) Geologic structure face occurrence calculation method based on three-dimensional electronic compass
CN112347625B (en) Magnetic interference compensation method for aircraft carrier
CN103353612B (en) A kind of measurement and positioning equipment of underground target object and measurement and positioning method
Zongwei et al. A low-cost calibration strategy for measurement-while-drilling system
CN110440746A (en) A kind of no-dig technique subterranean drill bit posture fusion method based on the decline of quaternary number gradient
CN105892498A (en) Target staring and scanning control system based on triaxial holder
CN105388533B (en) It is installed on the land bearing calibration of magnetometer magnetic disturbance in latent device
CN110736484B (en) Background magnetic field calibration method based on fusion of gyroscope and magnetic sensor
CN106842080A (en) A kind of magnetic field measuring device attitude swings interference minimizing technology
CN113866688B (en) Error calibration method for three-axis magnetic sensor under condition of small attitude angle
CN113447993B (en) Magnetic force vector measurement compensating flight method and system and magnetic compensation method and system
Gao et al. A calibration method for the misalignment error between inertial navigation system and tri-axial magnetometer in three-component magnetic measurement system
CN114415073B (en) Ground quick calibration method and system for aeromagnetic vector gradiometer error model
CN109633541A (en) A kind of magnetic source positioning device and source localization method
Pang et al. A new misalignment calibration method of portable geomagnetic field vector measurement system
CN114111841B (en) Data calibration method and data calibration device
CN110568387B (en) Magnetic gradient tensor-based spacecraft magnetic moment testing method
CN113624253A (en) Rotator error compensation and experiment method for three-axis magnetic sensor

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
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20220809

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