[go: up one dir, main page]

CN112130217B - Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer - Google Patents

Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer Download PDF

Info

Publication number
CN112130217B
CN112130217B CN202010849023.5A CN202010849023A CN112130217B CN 112130217 B CN112130217 B CN 112130217B CN 202010849023 A CN202010849023 A CN 202010849023A CN 112130217 B CN112130217 B CN 112130217B
Authority
CN
China
Prior art keywords
coil
magnetic field
magnetic
axis
turntable
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.)
Active
Application number
CN202010849023.5A
Other languages
Chinese (zh)
Other versions
CN112130217A (en
Inventor
葛健
钱君立
董浩斌
王锐
郑千玮
霍治帆
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
China University of Geosciences
Original Assignee
China University of Geosciences
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by China University of Geosciences filed Critical China University of Geosciences
Priority to CN202010849023.5A priority Critical patent/CN112130217B/en
Publication of CN112130217A publication Critical patent/CN112130217A/en
Application granted granted Critical
Publication of CN112130217B publication Critical patent/CN112130217B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • 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
    • G01V3/40Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation specially adapted for measuring magnetic field characteristics of the earth

Landscapes

  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Environmental & Geological Engineering (AREA)
  • Geology (AREA)
  • Physics & Mathematics (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Geophysics (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

本发明提供了线圈矢量磁力仪几何轴与磁轴夹角电学检测系统及方法。将所述电学检测系统放置于地磁环境下,保持所述Helmholtz线圈与所述无磁转台为关闭状态,获得地磁环境磁场大小;向所述Helmholtz线圈中施加激励电流,产生线圈磁场,计算出线圈磁场大小;持续向所述Helmholtz线圈中施加激励电流,且电流大小不变,开启所述无磁转台,利用所述无磁转台带动所述Helmholtz线圈在水平面上旋转一周,通过所述总场传感器获得所述地磁环境磁场与所述线圈磁场的合成磁场值的最大值和最小值;基于所述合成磁场值的最大值和最小值,计算出所述Helmholtz线圈的几何中心轴向与磁轴向的偏离角度。本发明的有益效果是:操作简单,成本低,实现了无需借助额外检测工具的情况下对线圈矢量磁力仪几何轴向与磁轴向一致性的高精度检测。

Figure 202010849023

The invention provides an electrical detection system and method for the angle included between the geometric axis and the magnetic axis of a coil vector magnetometer. Place the electrical detection system in a geomagnetic environment, keep the Helmholtz coil and the non-magnetic turntable in a closed state, and obtain the magnetic field size of the geomagnetic environment; apply an excitation current to the Helmholtz coil to generate a coil magnetic field, and calculate the coil magnetic field. The size of the magnetic field; the excitation current is continuously applied to the Helmholtz coil, and the current size does not change, the non-magnetic turntable is turned on, and the non-magnetic turntable is used to drive the Helmholtz coil to rotate once on the horizontal plane, through the total field sensor Obtain the maximum and minimum values of the combined magnetic field value of the geomagnetic environment magnetic field and the coil magnetic field; based on the maximum and minimum values of the combined magnetic field value, calculate the geometric center axis and magnetic axis of the Helmholtz coil deviation angle. The beneficial effects of the invention are that the operation is simple, the cost is low, and the high-precision detection of the consistency between the geometric axis and the magnetic axis of the coil vector magnetometer is realized without the aid of additional detection tools.

Figure 202010849023

Description

System and method for electrically detecting included angle between geometric axis and magnetic axis of coil vector magnetometer
Technical Field
The invention relates to the field of magnetic field measurement, in particular to an electrical detection system and method for an included angle between a geometric axis and a magnetic axis of a coil vector magnetometer.
Background
The geomagnetic measurement is used for measuring geomagnetic elements and the change of the geomagnetic elements along with time and space, and provides basic data for research of geomagnetic fields. The geomagnetic field is a vector field and consists of seven elements, namely a total field F, a horizontal component H, a north component X, an east component Y, a vertical component Z, a magnetic dip angle I and a magnetic declination angle D. Traditional earth magnetism is measured and is mainly observed to total field of earth magnetism and three-component development, and the target information of acquireing is limited, and earth magnetism full factor is surveyed and then can be acquireed more magnetic field information, accurately reflects the characteristic of study object, has more the advantage on weak magnetism target detection. The high-precision geomagnetic element observation can be widely applied to the fields of geoscience research, disaster monitoring and early warning, military detection, resource exploration and the like, so that the research on geomagnetic total element measurement is of great significance.
The main tool for geomagnetic measurement is a high-precision magnetometer. At present, geomagnetic vector measurement mainly comprises three-component measurement, such as a fluxgate magnetometer, but the method has the problems of low precision, temperature drift and the like. A small number of instruments realize partial information measurement such as magnetic direction or geomagnetic components in a mode of combined measurement of different sensors. And coil type vector magnetometer, like FHD, ZHD etc. through the mode that total field sensor and Helmholtz coil combined together, can effectively acquire earth magnetism full factor information, and compare in other instruments have higher stability and measurement accuracy, have extensive application prospect.
For a coil type vector magnetometer, a measurement system of the coil type vector magnetometer has special requirements on the direction of a magnetic field generated by a Helmholtz coil, and a uniform magnetic field generated by the coil needs to be ensured to face a certain specific direction so as to realize geomagnetic element measurement. Ideally, the magnetic field direction of the uniform area of the Helmholtz coil is along the axial direction of the geometric center of the coil, but when the Helmholtz coil has the problems of asymmetric coil winding and the like in the processing process, the magnetic field direction of the uniform area of the coil deviates from the axial direction of the geometric center, so that the uniform magnetic field applied in the coil-type vector magnetometer deviates from the expected orientation. In the occasion with low precision requirement, the geometric axial direction of the coil is usually the direction of the magnetic field uniform area by default, but in the vector measurement, second-level observation is needed, the deviation of the magnetic field direction generated by the coil and the geometric axial direction can cause the geomagnetic vector measurement precision to be reduced, a non-negligible measurement error is generated, and the accuracy of measurement data is affected, so that the consistency of the geometric axial direction and the magnetic axial direction of the coil vector magnetometer needs to be known. Generally, this problem is determined by the directional sensitivity of the fluxgate sensor, but the fluxgate is bulky and cannot be applied to the coil vector magnetometer. Although some semiconductor sensors, such as AMR and GMR, have small size and high spatial resolution, they often have the problems of low magnetic measurement accuracy, insufficient stability, etc., and are difficult to meet the requirement of high-precision measurement.
Disclosure of Invention
In order to solve the problems, the invention provides an electrical detection system and method for an included angle between a geometric axis and a magnetic axis of a coil vector magnetometer;
coil vector magnetometer geometric axis and magnetic axis contained angle electricity detecting system includes: the magnetic field sensor comprises Helmholtz coils, a total field sensor and a non-magnetic turntable, wherein the Helmholtz coils comprise two coils which are arranged in parallel, the total field sensor is placed at the center of an area surrounded by the two coils which are arranged in parallel, the magnetic field in the area surrounded by the two coils which are arranged in parallel is uniformly distributed, the non-magnetic turntable keeps a horizontal state, one of the Helmholtz coils is placed on the non-magnetic turntable in parallel with a horizontal plane, and the axial direction of the geometric center of each Helmholtz coil and the rotating axis of the non-magnetic turntable keep coaxial;
the method for electrically detecting the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer is realized by using the system for electrically detecting the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer, and comprises the following steps of:
s1, placing the electric detection system in a geomagnetic environment, keeping the Helmholtz coil and the non-magnetic turntable in a closed state, and obtaining the magnitude of a geomagnetic environment magnetic field through the total field sensor;
s2, applying excitation current to the Helmholtz coil to generate a coil magnetic field, and calculating the size of the coil magnetic field;
s3, continuously applying exciting current to the Helmholtz coil, enabling the current to be unchanged, starting the nonmagnetic turntable, driving the Helmholtz coil to rotate for a circle on a horizontal plane by using the nonmagnetic turntable, and obtaining the maximum value and the minimum value of the synthesized magnetic field value of the magnetic field of the geomagnetic environment and the magnetic field of the coil through the total field sensor;
s4, calculating the deviation angle between the geometric center axial direction and the magnetic axial direction of the Helmholtz coil based on the maximum value and the minimum value of the synthesized magnetic field value; the magnetic axial direction is the magnetic field direction of the coil in the step S2;
further, in step S1, the method for keeping the Helmholtz coil turned off is as follows: current is not introduced into the Helmholtz coil, so that the coil does not generate a coil magnetic field; keeping the non-magnetic turntable in a closed state is as follows: stopping the rotation of the non-magnetic turntable;
further, in step S2, the coil magnetic field magnitude is calculated by equation (1):
A=k×i (1)
wherein k is a coil constant, i is the magnitude of an excitation current applied to the Helmholtz coil, and A is the magnitude of a coil magnetic field;
further, in step S3, a coordinate system is established with the center of the magnetic field of the coil as an origin, the geometric central axis of the Helmholtz coil as a z-axis, the horizontal direction of the vertical plane where the magnetic field of the geomagnetic environment is located as an x-axis, and the straight line perpendicular to the xoz plane as a y-axis;
in the rotation process of the non-magnetic turntable, the magnetic field of the coil
Figure BDA0002644110240000031
Expressed as formula (2):
Figure BDA0002644110240000032
wherein A represents the size of a coil magnetic field, theta represents the included angle between the non-magnetic turntable and the x axis, namely the rotation angle of the non-magnetic turntable, and alpha represents the included angle between the coil magnetic field and the z axis, namely the included angle between the geometric axial direction and the magnetic axial direction of the coil vector magnetometer;
in the rotation process of the non-magnetic turntable, according to a vector algorithm, a synthetic magnetic field of the geomagnetic environment magnetic field and the coil magnetic field is expressed as a formula (3):
Figure BDA0002644110240000033
wherein, the magnetic field of geomagnetic environment
Figure BDA0002644110240000034
F0Representing a geomagnetic environmentThe magnitude of the magnetic field, I represents the included angle between the magnetic field in the geomagnetic environment and the horizontal plane, namely the inclination angle of the magnetic field in the geomagnetic environment;
as can be seen from the formula (3), the change relationship of the synthetic magnetic field value F along with the rotation angle theta of the non-magnetic turntable is shown in the formula (4):
Figure BDA0002644110240000035
simplifying the formula (4) to obtain a formula (5):
Figure BDA0002644110240000036
calculating the maximum value and the minimum value of the synthesized magnetic field values through the formulas (6), (7) and (8):
Figure BDA0002644110240000037
Figure BDA0002644110240000038
Figure BDA0002644110240000039
wherein, FmaxRepresenting the maximum value of the resultant magnetic field value, FminRepresents the minimum value of the resultant magnetic field value.
Further, in step S4, an included angle α between the geometric axial direction and the magnetic axial direction of the coil vector magnetometer is calculated by formula (7) and formula (8), as shown in formula (9):
Figure BDA0002644110240000041
wherein, F0Representing the magnitude of the magnetic field of the geomagnetic environment, A representing the magnitude of the magnetic field of the coil, FmaxIndication boxMaximum value of magnetic field value, FminRepresents the minimum value of the resultant magnetic field value.
The technical scheme provided by the invention has the beneficial effects that: the method is simple to operate and low in cost, and high-precision detection of the consistency of the geometric axial direction and the magnetic axial direction of the coil vector magnetometer is achieved without the help of an additional detection tool.
Drawings
The invention will be further described with reference to the accompanying drawings and examples, in which:
FIG. 1 is a flow chart of an electrical detection method for an included angle between a geometric axis and a magnetic axis of a coil vector magnetometer in an embodiment of the invention;
FIG. 2 is a schematic diagram of an electrical detection system for an included angle between a geometric axis and a magnetic axis of a coil vector magnetometer in an embodiment of the invention;
FIG. 3 is a schematic diagram of a detection principle model in an embodiment of the invention;
FIG. 4 is a schematic diagram of total field sensor accuracy error relationships in an embodiment of the present invention;
FIG. 5 is a schematic illustration of the resultant magnetic field as a function of rotational angle in an embodiment of the present invention;
FIG. 6 is a schematic illustration of the maximum and minimum errors of the resultant magnetic field in an embodiment of the present invention;
FIG. 7 is a schematic diagram of a coil field fluctuation error in an embodiment of the present invention.
Detailed Description
For a more clear understanding of the technical features, objects and effects of the present invention, embodiments of the present invention will now be described in detail with reference to the accompanying drawings.
The embodiment of the invention provides an electrical detection system and method for an included angle between a geometric axis and a magnetic axis of a coil vector magnetometer.
As shown in fig. 2, the electrical detection system for the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer comprises: helmholtz coil, total field sensor and no magnetism revolving stage, include two parallel arrangement's coil in the Helmholtz coil, total field sensor place in the center department in the region is enclosed into to two parallel arrangement's coil, just magnetic field evenly distributed in the region is enclosed into to two parallel arrangement's coil, no magnetism revolving stage keeps the horizontality, one of them coil and horizontal plane parallel placement in the Helmholtz coil are in on the no magnetism revolving stage, just the geometric centre axial of Helmholtz coil with the rotation axis of no magnetism revolving stage keeps coaxial.
The method for electrically detecting the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer is realized by using the system for electrically detecting the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer.
Referring to fig. 1, fig. 1 is a flowchart of an electrical detection method for an included angle between a geometric axis and a magnetic axis of a coil vector magnetometer in an embodiment of the present invention, which specifically includes the following steps:
s1, placing the electric detection system in a geomagnetic environment, keeping the Helmholtz coil and the non-magnetic turntable in a closed state, and obtaining the magnitude of a geomagnetic environment magnetic field through the total field sensor; keeping the Helmholtz coil in the off state is: current is not introduced into the Helmholtz coil, so that the coil does not generate a coil magnetic field; keeping the non-magnetic turntable in a closed state is as follows: stopping the rotation of the non-magnetic turntable;
s2, applying excitation current to the Helmholtz coil to generate a coil magnetic field, and calculating the size of the coil magnetic field; calculating the coil magnetic field size by the formula (1):
A=k×i (1)
wherein k is a coil constant, i is the magnitude of an excitation current applied to the Helmholtz coil, and A is the magnitude of a coil magnetic field;
s3, continuously applying exciting current to the Helmholtz coil, enabling the current to be unchanged, starting the nonmagnetic turntable, driving the Helmholtz coil to rotate for a circle on a horizontal plane by using the nonmagnetic turntable, and obtaining the maximum value and the minimum value of the synthesized magnetic field value of the magnetic field of the geomagnetic environment and the magnetic field of the coil through the total field sensor;
establishing a coordinate system by taking the center of a magnetic field of the coil as an origin, taking a geometric central axis of the Helmholtz coil as a z axis, taking the horizontal direction of a vertical plane where the magnetic field of the geomagnetic environment is located as an x axis and taking a straight line perpendicular to a plane xoz as a y axis;
in the rotation process of the non-magnetic turntable, the magnetic field of the coil
Figure BDA0002644110240000051
Expressed as formula (2):
Figure BDA0002644110240000052
wherein A represents the size of a coil magnetic field, theta represents the included angle between the non-magnetic turntable and the x axis, namely the rotation angle of the non-magnetic turntable, and alpha represents the included angle between the coil magnetic field and the z axis, namely the included angle between the geometric axial direction and the magnetic axial direction of the coil vector magnetometer;
in the rotation process of the non-magnetic turntable, according to a vector algorithm, a synthetic magnetic field of the geomagnetic environment magnetic field and the coil magnetic field is expressed as a formula (3):
Figure BDA0002644110240000061
wherein, the magnetic field of geomagnetic environment
Figure BDA0002644110240000062
F0The method comprises the steps of representing the magnitude of a magnetic field in a geomagnetic environment, wherein I represents an included angle between the magnetic field in the geomagnetic environment and a horizontal plane, namely an inclination angle of the magnetic field in the geomagnetic environment;
as can be seen from the formula (3), the change relationship of the synthetic magnetic field value F along with the rotation angle theta of the non-magnetic turntable is shown in the formula (4):
Figure BDA0002644110240000063
simplifying the formula (4) to obtain a formula (5):
Figure BDA0002644110240000064
calculating the maximum value and the minimum value of the synthesized magnetic field values through the formulas (6), (7) and (8):
Figure BDA0002644110240000065
Figure BDA0002644110240000066
Figure BDA0002644110240000067
wherein, FmaxRepresenting the maximum value of the resultant magnetic field value, FminRepresents the minimum value of the resultant magnetic field value;
s4, calculating the deviation angle between the geometric center axial direction and the magnetic axial direction of the Helmholtz coil based on the synthetic magnetic field; the magnetic axial direction is the magnetic field direction of the coil in the step S2;
the calculation process of the deviation angle between the geometric center axial direction and the magnetic axial direction of the Helmholtz coil is as follows:
calculating an included angle alpha between the geometric axial direction and the magnetic axial direction of the coil vector magnetometer according to a formula (7) and a formula (8), wherein the included angle alpha is shown as a formula (9):
Figure BDA0002644110240000068
wherein, F0Representing the magnitude of the magnetic field of the geomagnetic environment, A representing the magnitude of the magnetic field of the coil, FmaxRepresenting the maximum value of the resultant magnetic field value, FminRepresents the minimum value of the resultant magnetic field value.
In order to further determine and improve the detection precision of the electrical detection method for the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer, indexes such as the precision of a total field sensor, the stepping amount of a non-magnetic turntable, the stability of a coil magnetic field generated by a Helmholtz coil and the like in the detection method need to be provided so as to ensure the accuracy of the detection result of the detection system.
Referring to fig. 4, fig. 4 is a schematic diagram of a precision error relationship of a total field sensor in an embodiment of the present invention, and key values of a detection system are all obtained through the total field sensor, and if the total field sensor has an error, the detection system will be affected. And if the measurement precision of the total field sensor is k, the maximum detection result obtained by using the detection method is shown as the formula (10):
Figure BDA0002644110240000071
then the maximum error of the detection system is error when the sensor precision is kαAs shown in formula (11):
errorα=α′-α (11)
in Chinese Wuhan (F)0For example, 50000nT, I47.2 °), when a is 15000nT, the total field sensor accuracy error relationship diagram shown in fig. 4 can be obtained from equations (10) and (11) when the sensor accuracy k varies between 0nT and 1nT, and as can be seen from fig. 4, when the sensor accuracy k is 0.1nT, the maximum error of the detection system can be controlled to be less than 5 ".
Referring to fig. 5, fig. 5 is a schematic diagram of the variation of the synthetic magnetic field with the rotation angle according to the embodiment of the present invention, which is wuhan (F) in china0Taking 50000nT and I47.2 °), a 15000nT, the relationship between the change in the synthetic magnetic field F when the rotation angle θ of the nonmagnetic turntable rotates one revolution can be obtained from the formula (4), as shown in fig. 5. It can be seen that the synthetic magnetic field F changes periodically with one rotation of the non-magnetic turntable, but when the stepping amount of the non-magnetic turntable is too large, the total field sensor loses part of the sampling points, so that the finally needed Fmax、FminAnd errors exist between the measured value and the true maximum value and the true minimum value, and the measurement precision is finally influenced.
Referring to fig. 6, fig. 6 is a schematic diagram illustrating maximum and minimum errors of the synthesized magnetic field according to an embodiment of the present invention. When F is presentmaxAnd FminWhen an error occurs, if the error is set as e, the maximum detection result obtained by using the detection method is as shown in formula (12):
Figure BDA0002644110240000072
then the system maximum error is detectedαComprises the following steps:
errorα=α′-α (13)
in Chinese Wuhan (F)0For example, 50000nT, I47.2 °), when a 15000nT is taken, and when the extreme value error e varies between 0nT and 1nT, the maximum value and minimum value errors of the resultant magnetic field shown in fig. 6 can be obtained by equations (12) and (13).
The measurement error of the maximum value and the minimum value of the synthetic magnetic field caused by the step amount of the non-magnetic turntable can be determined from fig. 5, the detection system error caused by the measurement error of the maximum value and the minimum value of the synthetic magnetic field can be determined from fig. 6, and the combination of fig. 5 and fig. 6 can determine that when the step amount of the non-magnetic turntable is less than 0.5 degrees, the measurement error e of the maximum value and the minimum value of the synthetic magnetic field is less than 0.1nT, and the detection system error is less than 2 ".
Referring to fig. 7, fig. 7 is a schematic diagram of a coil magnetic field fluctuation error according to an embodiment of the present invention. When the excitation current is unstable, the coil magnetic field generated by the Helmholtz coil fluctuates, and the detection system result is influenced. And if the fluctuation of the magnetic field of the coil is m, the maximum detection result obtained by the detection method is shown as the formula (14):
Figure BDA0002644110240000081
then when the fluctuation of the coil magnetic field is m, the maximum error of the detection system is errorαAs in equation (15):
errorα=α′-α (15)
in Chinese Wuhan (F)0Taking 50000nT and 47.2 ° as an example, a 15000nT, when the coil magnetic field fluctuation m varies between 0 to 1nT, the schematic diagram of the coil magnetic field fluctuation as shown in fig. 7 can be obtained from equations (14) and (15).
As can be seen from fig. 7, when the coil magnetic field fluctuation is controlled to be within 0.5nT, the detection system error can be made 3 ".
In combination with the foregoing analysis, the electrical detection system and method for the included angle between the geometric axis and the magnetic axis of the coil vector magnetometer provided by the invention have the detection result shown in formula (9), and when the relevant parameters of the control detection system are as follows: the accuracy of the total field sensor is better than 0.1nT, the stepping amount of the non-magnetic rotary table is less than 0.5 degrees, and the accuracy of the detection system is 10' when the fluctuation of the magnetic field of the coil is less than 0.5 nT.
The invention has the beneficial effects that: the method is simple to operate and low in cost, and high-precision detection of the consistency of the geometric axial direction and the magnetic axial direction of the coil vector magnetometer is achieved without the help of an additional detection tool.
The above description is only for the purpose of illustrating the preferred embodiments of the present invention and is not to be construed as limiting the invention, and any modifications, equivalents, improvements and the like that fall within the spirit and principle of the present invention are intended to be included therein.

Claims (5)

1.一种线圈矢量磁力仪几何轴与磁轴夹角电学检测方法,基于一种线圈矢量磁力仪几何轴与磁轴夹角电学检测系统,其特征在于:所述线圈矢量磁力仪几何轴与磁轴夹角电学检测系统包括:Helmholtz线圈、总场传感器和无磁转台,所述Helmholtz线圈中包含两个平行设置的线圈,所述总场传感器放置于所述两个平行设置的线圈所围成区域的中心处,且所述两个平行设置的线圈所围成区域内磁场均匀分布,所述无磁转台保持水平状态,所述Helmholtz线圈中其中一个线圈与水平面平行放置在所述无磁转台上,且所述Helmholtz线圈的几何中心轴向与所述无磁转台的旋转轴心保持同轴;1. a coil vector magnetometer geometric axis and the magnetic axis angle electrical detection method, based on a coil vector magnetometer geometric axis and the magnetic axis angle electrical detection system, it is characterized in that: the coil vector magnetometer geometric axis and The electrical detection system for the included angle of the magnetic axis includes: a Helmholtz coil, a total field sensor and a non-magnetic turntable, the Helmholtz coil includes two parallel coils, and the total field sensor is placed around the two parallel coils At the center of the area, and the magnetic field is evenly distributed in the area enclosed by the two parallel coils, the non-magnetic turntable is kept in a horizontal state, and one of the Helmholtz coils is placed in parallel with the horizontal plane on the non-magnetic turntable. on the turntable, and the geometric center axis of the Helmholtz coil is coaxial with the rotation axis of the non-magnetic turntable; 所述线圈矢量磁力仪几何轴与磁轴夹角电学检测方法包括以下步骤:The method for electrical detection of the angle between the geometric axis of the coil vector magnetometer and the magnetic axis includes the following steps: S1、将所述电学检测系统放置于地磁环境下,保持所述Helmholtz线圈与所述无磁转台为关闭状态,通过所述总场传感器获得地磁环境磁场大小;S1. Place the electrical detection system in a geomagnetic environment, keep the Helmholtz coil and the non-magnetic turntable in a closed state, and obtain the magnetic field size of the geomagnetic environment through the total field sensor; S2、向所述Helmholtz线圈中施加激励电流,产生线圈磁场,计算出线圈磁场大小;S2, applying excitation current to the Helmholtz coil, generating a coil magnetic field, and calculating the size of the coil magnetic field; S3、持续向所述Helmholtz线圈中施加激励电流,且电流大小不变,开启所述无磁转台,利用所述无磁转台带动所述Helmholtz线圈在水平面上旋转一周,通过所述总场传感器获得所述地磁环境磁场与所述线圈磁场的合成磁场值的最大值和最小值;S3. Continue to apply an excitation current to the Helmholtz coil, and the magnitude of the current remains unchanged, turn on the non-magnetic turntable, and use the non-magnetic turntable to drive the Helmholtz coil to rotate once on the horizontal plane, and obtain through the total field sensor the maximum value and the minimum value of the combined magnetic field value of the geomagnetic environment magnetic field and the coil magnetic field; S4、基于所述合成磁场值的最大值和最小值,计算出所述Helmholtz线圈的几何中心轴向与磁轴向的偏离角度;所述磁轴向即为步骤S2中线圈磁场方向。S4. Calculate the deviation angle between the geometric center axis of the Helmholtz coil and the magnetic axis based on the maximum and minimum values of the synthetic magnetic field; the magnetic axis is the direction of the magnetic field of the coil in step S2. 2.如权利要求1所述的线圈矢量磁力仪几何轴与磁轴夹角电学检测方法,其特征在于:步骤S1中,保持所述Helmholtz线圈为关闭状态即是:不向Helmholtz线圈通入电流,使该线圈不产生线圈磁场;保持所述无磁转台为关闭状态即是:使无磁转台停止转动。2. The method for electrical detection of the included angle between the geometric axis of the coil vector magnetometer and the magnetic axis as claimed in claim 1, wherein in step S1, keeping the Helmholtz coil in a closed state is that no current is passed to the Helmholtz coil. , so that the coil does not generate a coil magnetic field; keeping the non-magnetic turntable in a closed state means: stopping the rotation of the non-magnetic turntable. 3.如权利要求1所述的线圈矢量磁力仪几何轴与磁轴夹角电学检测方法,其特征在于:步骤S2中,通过公式(1),计算出线圈磁场大小:3. the method for electrical detection of the included angle between the geometric axis of the coil vector magnetometer and the magnetic axis as claimed in claim 1, is characterized in that: in step S2, by formula (1), the coil magnetic field size is calculated: A=k×i (1)A=k×i (1) 其中,k为线圈常数,i为向所述Helmholtz线圈中施加的激励电流的大小,A为线圈磁场大小。Wherein, k is the coil constant, i is the magnitude of the excitation current applied to the Helmholtz coil, and A is the magnitude of the coil magnetic field. 4.如权利要求1所述的线圈矢量磁力仪几何轴与磁轴夹角电学检测方法,其特征在于:步骤S3中,以线圈磁场中心为原点,以Helmholtz线圈几何中心轴为z轴,以地磁环境磁场所在竖直平面的水平方向为x轴,以垂直于xoz平面直线为y轴,建立坐标系;4. The method for electrical detection of the included angle between the geometric axis of the coil vector magnetometer and the magnetic axis as claimed in claim 1, wherein in step S3, take the coil magnetic field center as the origin, take the Helmholtz coil geometric center axis as the z-axis, and The horizontal direction of the vertical plane where the geomagnetic environmental magnetic field is located is the x-axis, and the line perpendicular to the xoz plane is the y-axis to establish a coordinate system; 无磁转台旋转过程中,线圈磁场
Figure FDA0003057259680000021
表示为如公式(2):
During the rotation of the non-magnetic turntable, the magnetic field of the coil
Figure FDA0003057259680000021
It is expressed as formula (2):
Figure FDA0003057259680000022
Figure FDA0003057259680000022
其中,A表示线圈磁场大小,θ表示无磁转台与x轴的夹角,即无磁转台旋转角度,α表示线圈磁场与z轴的夹角,即线圈矢量磁力仪几何轴向与磁轴向的夹角;Among them, A represents the size of the coil magnetic field, θ represents the angle between the non-magnetic turntable and the x-axis, that is, the rotation angle of the non-magnetic turntable, α represents the angle between the coil magnetic field and the z-axis, that is, the geometric axis and the magnetic axis of the coil vector magnetometer. the included angle; 无磁转台旋转过程中,根据矢量运算法则,所述地磁环境磁场与所述线圈磁场的合成磁场
Figure FDA0003057259680000023
表示为如公式(3):
During the rotation of the non-magnetic turntable, according to the vector algorithm, the combined magnetic field of the geomagnetic environment magnetic field and the coil magnetic field is
Figure FDA0003057259680000023
It is expressed as formula (3):
Figure FDA0003057259680000024
Figure FDA0003057259680000024
其中,地磁环境磁场
Figure FDA0003057259680000025
F0表示地磁环境磁场大小,I表示地磁环境磁场与水平面的夹角,即地磁环境磁场的倾角;
Among them, the geomagnetic environment magnetic field
Figure FDA0003057259680000025
F 0 represents the size of the geomagnetic environment magnetic field, I represents the angle between the geomagnetic environment magnetic field and the horizontal plane, that is, the inclination angle of the geomagnetic environment magnetic field;
由公式(3)可知,合成磁场值F随着无磁转台旋转角度θ的变化关系如公式(4)所示:It can be known from formula (3) that the variation relationship of the synthetic magnetic field value F with the rotation angle θ of the non-magnetic turntable is shown in formula (4):
Figure FDA0003057259680000026
Figure FDA0003057259680000026
将公式(4)进行简化得到公式(5):Simplify formula (4) to obtain formula (5):
Figure FDA0003057259680000027
Figure FDA0003057259680000027
通过公式(6)、(7)、(8),计算得到合成磁场值的最大值和最小值:Through formulas (6), (7), (8), the maximum and minimum values of the synthetic magnetic field are calculated:
Figure FDA0003057259680000028
Figure FDA0003057259680000028
Figure FDA0003057259680000029
Figure FDA0003057259680000029
Figure FDA00030572596800000210
Figure FDA00030572596800000210
其中,Fmax表示合成磁场值的最大值,Fmin表示合成磁场值的最小值。Among them, F max represents the maximum value of the combined magnetic field value, and F min represents the minimum value of the combined magnetic field value.
5.如权利要求4所述的线圈矢量磁力仪几何轴与磁轴夹角电学检测方法,其特征在于:在步骤S4中,通过公式(7)和公式(8),计算得出线圈矢量磁力仪几何轴向与磁轴向的夹角α,如公式(9):5. The method for electrical detection of the angle between the geometric axis of the coil vector magnetometer and the magnetic axis as claimed in claim 4, wherein in step S4, by formula (7) and formula (8), the coil vector magnetic force is calculated The angle α between the geometric axis of the instrument and the magnetic axis, as in formula (9):
Figure FDA0003057259680000031
Figure FDA0003057259680000031
其中,F0表示地磁环境磁场大小,A表示线圈磁场大小,Fmax表示合成磁场值的最大值,Fmin表示合成磁场值的最小值。Among them, F 0 represents the size of the geomagnetic environment magnetic field, A represents the size of the coil magnetic field, F max represents the maximum value of the combined magnetic field value, and F min represents the minimum value of the combined magnetic field value.
CN202010849023.5A 2020-08-21 2020-08-21 Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer Active CN112130217B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202010849023.5A CN112130217B (en) 2020-08-21 2020-08-21 Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202010849023.5A CN112130217B (en) 2020-08-21 2020-08-21 Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer

Publications (2)

Publication Number Publication Date
CN112130217A CN112130217A (en) 2020-12-25
CN112130217B true CN112130217B (en) 2021-08-06

Family

ID=73850497

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202010849023.5A Active CN112130217B (en) 2020-08-21 2020-08-21 Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer

Country Status (1)

Country Link
CN (1) CN112130217B (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113074616B (en) * 2021-03-25 2023-10-20 中国电子科技集团公司第十六研究所 Concentricity testing device and method for coaxial superconducting magnet
CN113608273B (en) * 2021-08-12 2022-08-30 中国地质大学(武汉) Geomagnetic daily variation error correction method for coil type vector magnetometer
CN113820751B (en) * 2021-08-20 2022-08-30 中国地质大学(武汉) Mechanical drift correction method and device for dIdD magnetometer platform and storage device
CN114689637B (en) * 2022-05-31 2022-09-30 中国科学技术大学 Molecular information detection method and system based on nano-diamond probe paramagnetic resonance
CN117031373B (en) * 2023-06-14 2024-07-02 中勘地球物理有限责任公司 Multi-magnetic-axis consistency calibration method for fluxgate magnetometer

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101833074A (en) * 2010-04-29 2010-09-15 苏州同心医疗器械有限公司 Device and method thereof for measuring magnetization vector direction deflection angle of permanent magnet
CN204613380U (en) * 2015-04-21 2015-09-02 骏材(深圳)科技工程有限公司 A kind of magnetic moment measurement device
CN106950516A (en) * 2017-03-24 2017-07-14 中国科学院上海微系统与信息技术研究所 A kind of weak swirl magnetic field measuring device and method
WO2018023033A1 (en) * 2016-07-29 2018-02-01 Western Michigan University Research Foundation Magnetic nanoparticle-based gyroscopic sensor
CN109407159A (en) * 2018-11-13 2019-03-01 中国地质大学(武汉) A kind of earth magnetism total factor sensor attitude error calibration method
CN110568384A (en) * 2019-08-27 2019-12-13 中国科学院武汉物理与数学研究所 An active magnetic compensation method for an ultrasensitive atomic magnetometer
CN110596625A (en) * 2019-07-22 2019-12-20 哈尔滨工程大学 A Calibration Method for the Optimal Arrangement and Calibration of Magnetic Fields of Three-dimensional Helmholtz Coils

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101833074A (en) * 2010-04-29 2010-09-15 苏州同心医疗器械有限公司 Device and method thereof for measuring magnetization vector direction deflection angle of permanent magnet
CN204613380U (en) * 2015-04-21 2015-09-02 骏材(深圳)科技工程有限公司 A kind of magnetic moment measurement device
WO2018023033A1 (en) * 2016-07-29 2018-02-01 Western Michigan University Research Foundation Magnetic nanoparticle-based gyroscopic sensor
CN106950516A (en) * 2017-03-24 2017-07-14 中国科学院上海微系统与信息技术研究所 A kind of weak swirl magnetic field measuring device and method
CN109407159A (en) * 2018-11-13 2019-03-01 中国地质大学(武汉) A kind of earth magnetism total factor sensor attitude error calibration method
CN110596625A (en) * 2019-07-22 2019-12-20 哈尔滨工程大学 A Calibration Method for the Optimal Arrangement and Calibration of Magnetic Fields of Three-dimensional Helmholtz Coils
CN110568384A (en) * 2019-08-27 2019-12-13 中国科学院武汉物理与数学研究所 An active magnetic compensation method for an ultrasensitive atomic magnetometer

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
亥姆霍兹线圈测量系统的测量原理及程序设计;彭全岭 等;《高能物理与核物理》;20010930;第25卷(第9期);第920-925页 *

Also Published As

Publication number Publication date
CN112130217A (en) 2020-12-25

Similar Documents

Publication Publication Date Title
CN112130217B (en) Electrical detection system and method for angle between geometric axis and magnetic axis of coil vector magnetometer
JP4093861B2 (en) Compensation of large magnetic errors for electronic compass and all orientation operations
CN102313543B (en) Magnetic azimuth measuring system based on giant magneto-resistance sensor, measurement method and perpendicular compensation method
CN104345348B (en) Aviation superconduction full tensor magnetic gradient measurements system relevant parameter acquisition device and method
CN107544042B (en) A magnetometer array calibration method
CN111077595B (en) A correction method and storage medium for angle error of superconducting magnetic measuring system
JP2007500350A (en) System using 2-axis magnetic sensor for 3-axis compass solution
CN109459712A (en) Vector closed loop compensation formula triaxial magnetic field sensor probe based on Helmholtz coil
CN107121655B (en) Non-orthogonal angle measuring device and method for magnetic field cancellation coil of non-shielding SERF atomic magnetometer
CN113325353A (en) Magnetometer spatial attitude calibration method and system
Včelák et al. Precise magnetic sensors for navigation and prospection
CN114089243A (en) A vector atomic magnetometer device and method based on magnetic field rotation modulation method
CN102354000A (en) Orthogonal field calibration device for three-component magnetic probe and calibration method thereof
CN112130229B (en) Coil vector magnetometer out-of-levelness error electrical detection system and method
DOELL et al. Analysis of spinner magnetometer operation
CN108469593A (en) A kind of comprehensive magnetic field gradient sensor of high-resolution orthogonal fluxgate based on amorphous wire orthogonal array
RU138023U1 (en) DEVICE FOR CALIBRATING A THREE-COMPONENT MAGNETOMETER
CN114779144B (en) Method, chip and device for measuring mounting matrix of three-axis magnetometer
CN111624531B (en) A Component Solution Method for TMR Three-axis Integrated Magnetic Sensor
CN110568387B (en) A Spacecraft Magnetic Moment Test Method Based on Magnetic Gradient Tensor
CN115097370A (en) Steering difference calibration method for self-balancing vector magnetometer in large-plane magnetic measurement system
CN110702102B (en) Magnetic navigation system for navigation aircraft and navigation method thereof
CN113820751A (en) Method, device and storage device for mechanical drift correction of dIdD magnetometer platform
JPH06265611A (en) Magnetic field measuring device
Ge et al. Modeling and reduction of the initial orientation error of a coil vector magnetometer

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