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CN109633539B - Static positioning device and static positioning method for magnetic source - Google Patents

Static positioning device and static positioning method for magnetic source Download PDF

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CN109633539B
CN109633539B CN201910061723.5A CN201910061723A CN109633539B CN 109633539 B CN109633539 B CN 109633539B CN 201910061723 A CN201910061723 A CN 201910061723A CN 109633539 B CN109633539 B CN 109633539B
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magnetic
full tensor
measurement component
magnetic source
gradient measurement
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CN109633539A (en
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伍俊
荣亮亮
张国锋
张树林
邱隆清
张朝祥
宋正威
裴易峰
谢晓明
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Shanghai Institute of Microsystem and Information Technology of CAS
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S5/00Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations
    • G01S5/02Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations using radio waves
    • G01S5/06Position of source determined by co-ordinating a plurality of position lines defined by path-difference measurements
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S5/00Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations
    • G01S5/02Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations using radio waves
    • G01S5/0257Hybrid positioning
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S5/00Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations
    • G01S5/02Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations using radio waves
    • G01S5/14Determining absolute distances from a plurality of spaced points of known location
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S5/00Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations
    • G01S5/02Position-fixing by co-ordinating two or more direction or position line determinations; Position-fixing by co-ordinating two or more distance determinations using radio waves
    • G01S5/14Determining absolute distances from a plurality of spaced points of known location
    • G01S5/145Using a supplementary range measurement, e.g. based on pseudo-range measurements

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  • Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
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  • Measuring Magnetic Variables (AREA)
  • Measurement And Recording Of Electrical Phenomena And Electrical Characteristics Of The Living Body (AREA)

Abstract

The invention provides a static positioning device and a static positioning method of a magnetic source, wherein the static positioning device comprises: a mounting bracket for providing a mounting platform; the full tensor magnetic gradient measurement assembly is arranged on the mounting bracket and is used for measuring the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement assembly; the position locator is rigidly connected with the full tensor magnetic gradient measurement assembly and is used for measuring the position coordinates of the full tensor magnetic gradient measurement assembly under a geographic coordinate system; and the measurement and control assembly is electrically connected with the full tensor magnetic gradient measurement assembly and the position positioner and is used for acquiring the magnetic field gradient value and the position coordinate and positioning the magnetic source to be positioned in a motion state in real time according to acquired data. The invention solves the problem that the moving magnetic source cannot be positioned efficiently in the prior art.

Description

一种磁源的静态定位装置及静态定位方法A static positioning device and static positioning method for a magnetic source

技术领域technical field

本发明属于磁法探测领域,特别是涉及一种磁源的静态定位装置及静态定位方法。The invention belongs to the field of magnetic detection, in particular to a static positioning device and a static positioning method for a magnetic source.

背景技术Background technique

全张量磁梯度描述的是磁场矢量在三维空间的变化率信息,即磁场矢量的三个分量在空间中三个方向上的梯度。全张量磁梯度的测量结果具有受磁化方向影响小,能够反映目标体的矢量磁矩信息,且能更好地反演场源参数(方位、磁矩等)等优点,故可以对场源进行定位和追踪,提高磁源体的分辨率。The full tensor magnetic gradient describes the change rate information of the magnetic field vector in three-dimensional space, that is, the gradient of the three components of the magnetic field vector in three directions in space. The measurement results of the full tensor magnetic gradient have the advantages of being less affected by the magnetization direction, can reflect the vector magnetic moment information of the target body, and can better invert the field source parameters (orientation, magnetic moment, etc.), so it can be used for the field source Carry out positioning and tracking, and improve the resolution of the magnetic source body.

目前已知的磁源定位方法中,通常需要磁源的总场信息才能实现对运动磁源的定位,但运动磁源的总场信息在实际测量过程中因地球磁场波动很难精确测量,从而导致现有定位方法的定位精度有限。因此,如何提供一种高精度的运动磁源定位方法是本领域技术人员迫切需要解决的技术问题。In the current known magnetic source positioning methods, the total field information of the magnetic source is usually required to locate the moving magnetic source, but it is difficult to accurately measure the total field information of the moving magnetic source due to the fluctuation of the earth’s magnetic field in the actual measurement process, thus As a result, the positioning accuracy of existing positioning methods is limited. Therefore, how to provide a high-precision moving magnetic source positioning method is an urgent technical problem to be solved by those skilled in the art.

发明内容Contents of the invention

鉴于以上所述现有技术的缺点,本发明的目的在于提供一种磁源的静态定位装置及静态定位方法,用于解决现有技术中无法对运动磁源进行高效定位的问题。In view of the above-mentioned shortcomings of the prior art, the object of the present invention is to provide a static positioning device and a static positioning method for a magnetic source, which are used to solve the problem that the moving magnetic source cannot be efficiently positioned in the prior art.

为实现上述目的及其他相关目的,本发明提供一种磁源的静态定位装置,所述静态定位装置包括:In order to achieve the above purpose and other related purposes, the present invention provides a static positioning device for a magnetic source, the static positioning device includes:

安装支架,用于提供安装平台;The mounting bracket is used to provide a mounting platform;

全张量磁梯度测量组件,设于所述安装支架上,用于测量待定位磁源在所述全张量磁梯度测量组件处产生的磁场梯度值;The full tensor magnetic gradient measurement component is arranged on the installation bracket, and is used to measure the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component;

位置定位器,刚性连接于所述全张量磁梯度测量组件,用于测量所述全张量磁梯度测量组件在地理坐标系下的位置坐标;A position locator, rigidly connected to the full tensor magnetic gradient measurement component, for measuring the position coordinates of the full tensor magnetic gradient measurement component in the geographic coordinate system;

测控组件,电连接于所述全张量磁梯度测量组件及所述位置定位器,用于采集所述磁场梯度值及所述位置坐标,并根据采集的数据对运动状态下的所述待定位磁源进行实时定位。The measurement and control component is electrically connected to the full tensor magnetic gradient measurement component and the position locator, and is used to collect the magnetic field gradient value and the position coordinates, and to locate the to-be-positioned object in a moving state according to the collected data. Magnetic source for real-time positioning.

可选地,所述全张量磁梯度测量组件包括:至少一个磁强计。Optionally, the full tensor magnetic gradient measurement component includes: at least one magnetometer.

可选地,所述安装支架包括低温容器,用于为所述全张量磁梯度测量组件提供安装平台,同时为所述全张量磁梯度测量组件提供低温环境。Optionally, the installation bracket includes a cryogenic container, which is used to provide an installation platform for the full tensor magnetic gradient measurement assembly, and provide a low temperature environment for the full tensor magnetic gradient measurement assembly.

可选地,所述全张量磁梯度测量组件包括:至少一个平面梯度计。Optionally, the full tensor magnetic gradiometer measurement component includes: at least one planar gradiometer.

可选地,所述低温容器包括低温杜瓦。Optionally, the cryogenic container includes a cryogenic Dewar.

可选地,所述位置定位器包括:差分GPS接收机或组合惯导。Optionally, the position locator includes: a differential GPS receiver or an integrated inertial navigation.

本发明还提供了一种磁源的静态定位方法,所述静态定位方法包括:The present invention also provides a static positioning method for a magnetic source, the static positioning method comprising:

搭建如上所述的静态定位装置;Build a static positioning device as described above;

在所述待定位磁源处于静止状态时,获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并获取两选定测点的所述全张量磁梯度测量组件的位置坐标,以实现根据全张量不变量获取静止状态下所述待定位磁源的初始位置坐标;When the magnetic source to be positioned is in a static state, obtain the magnetic field gradient values generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement components at two selected measuring points in the static state, and obtain two selected The position coordinates of the full tensor magnetic gradient measurement component of the measuring point, so as to obtain the initial position coordinates of the magnetic source to be positioned in a static state according to the full tensor invariant;

在所述待定位磁源处于运动状态时,获取运动状态下所述待定位磁源在任一所述选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值;When the magnetic source to be positioned is in a moving state, obtain the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component at any one of the selected measuring points in the moving state;

根据全张量不变量建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型,以实现根据同一选定测点对应的不同状态下的所述磁场梯度值、所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标获取运动状态下所述待定位磁源的实时位置坐标。Establishing a distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located according to the full tensor invariant, so as to realize the magnetic field gradient values, The initial position coordinates of the magnetic source to be located and the position coordinates corresponding to the selected measuring point obtain the real-time position coordinates of the magnetic source to be located in a moving state.

可选地,获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值的方法包括:获取静止状态下所述待定位磁源在不同测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并对不同测点对应的所述磁场梯度值进行信噪比比较以选出信噪比最优的两个所述磁场梯度值;其中,选出的两个所述磁场梯度值对应的测点作为所述选定测点。Optionally, the method for obtaining the magnetic field gradient values generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement components at two selected measuring points in a static state includes: obtaining the magnetic source to be positioned in a static state The magnetic field gradient values generated at the full tensor magnetic gradient measurement components at different measuring points, and the signal-to-noise ratio comparison is performed on the magnetic field gradient values corresponding to different measuring points to select two optimal signal-to-noise ratios. The magnetic field gradient value; wherein, the selected measuring points corresponding to the two magnetic field gradient values are used as the selected measuring points.

可选地,获取所述全张量磁梯度测量组件的位置坐标的方法包括:获取所述位置定位器的位置坐标,并获取所述全张量磁梯度测量组件与所述位置定位器之间的偏移量;基于所述偏移量对所述位置坐标进行修正,以获取所述全张量磁梯度测量组件的位置坐标。Optionally, the method for obtaining the position coordinates of the full tensor magnetic gradient measurement component includes: obtaining the position coordinates of the position locator, and obtaining the distance between the full tensor magnetic gradient measurement component and the position locator The offset amount; based on the offset amount, the position coordinates are corrected to obtain the position coordinates of the full tensor magnetic gradient measurement component.

可选地,获取所述待定位磁源的初始位置坐标的方法包括:Optionally, the method for obtaining the initial position coordinates of the magnetic source to be located includes:

根据两选定测点对应的所述磁场梯度值及全张量不变量获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;Acquire the unit of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in a static state according to the magnetic field gradient values corresponding to the two selected measuring points and the full tensor invariant vector;

根据两选定测点对应的位置坐标及静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量建立空间直线模型,以获取所述待定位磁源的初始位置坐标。According to the position coordinates corresponding to the two selected measuring points and the unit vector of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in a static state, a space linear model is established to obtain the Describe the initial position coordinates of the magnetic source to be located.

可选地,获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量的方法包括:Optionally, the method for obtaining the unit vector of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to two selected measuring points in a static state includes:

根据两选定测点对应的所述磁场梯度值分别获取两选定测点对应的全张量磁梯度矩阵特征值;Obtaining the full tensor magnetic gradient matrix eigenvalues corresponding to the two selected measuring points respectively according to the magnetic field gradient values corresponding to the two selected measuring points;

根据两选定测点对应的全张量磁梯度矩阵特征值分别获取两选定测点对应的全张量磁梯度矩阵最小绝对特征值,并根据两选定测点对应的全张量磁梯度矩阵最小绝对特征值获取一参考方向向量;其中,所述参考方向向量平行于静止状态下所述待定位磁源磁矩的方向向量;According to the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points, the minimum absolute eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points are respectively obtained, and according to the full tensor magnetic gradient matrix corresponding to the two selected measuring points The minimum absolute eigenvalue of the matrix obtains a reference direction vector; wherein, the reference direction vector is parallel to the direction vector of the magnetic moment of the magnetic source to be located in a static state;

根据全张量不变量

Figure BDA0001954355710000031
确定静止状态下所述待定位磁源的磁矩矢量的单位向量,从而获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;其中,MT为全张量不变量,λ1、λ2、λ3为全张量磁梯度矩阵特征值,μ0为真空磁导率,M为待定位磁源的磁矩的模,R为全张量磁梯度测量组件与待定位磁源之间的距离。According to the full tensor invariant
Figure BDA0001954355710000031
Determine the unit vector of the magnetic moment vector of the magnetic source to be positioned in the static state, thereby obtaining the unit of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in the static state vector; where, MT is the full tensor invariant, λ 1 , λ 2 , λ 3 are the eigenvalues of the full tensor magnetic gradient matrix, μ 0 is the vacuum permeability, M is the modulus of the magnetic moment of the magnetic source to be positioned, R is the distance between the full tensor magnetic gradient measurement component and the magnetic source to be located.

可选地,获取所述参考方向向量的方法包括:根据两选定测点对应的全张量磁梯度矩阵最小绝对特征值获取其对应的特征向量,并通过对两所述特征向量求取向量积以获取所述参考方向向量。Optionally, the method for obtaining the reference direction vector includes: obtaining the corresponding eigenvector according to the minimum absolute eigenvalue of the full tensor magnetic gradient matrix corresponding to the two selected measuring points, and obtaining the vector product to obtain the reference direction vector.

可选地,确定静止状态下所述待定位磁源的磁矩矢量的单位向量的方法包括:根据全张量不变量

Figure BDA0001954355710000032
及两选定测点对应的全张量磁梯度矩阵特征值判断静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的距离远近,从而确定静止状态下所述待定位磁源的磁矩矢量的单位向量。Optionally, the method for determining the unit vector of the magnetic moment vector of the magnetic source to be located in the static state includes: according to the full tensor invariant
Figure BDA0001954355710000032
and the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points to judge the distance from the magnetic source to be positioned to the full tensor magnetic gradient measuring components of the two selected measuring points in the static state, thereby determining the static state The unit vector of the magnetic moment vector of the magnetic source to be located described below.

可选地,所述空间直线模型包括:

Figure BDA0001954355710000033
Figure BDA0001954355710000034
其中,x、y、z是所述待定位磁源的初始位置坐标,Ax、Ay、Az是一选定测点的所述全张量磁梯度测量组件的位置坐标,PA、QA、HA是静止状态下所述待定位磁源到一选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量,Bx、By、Bz是另一选定测点的所述全张量磁梯度测量组件的位置坐标,PB、QB、HB是静止状态下所述待定位磁源到另一选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量。Optionally, the space linear model includes:
Figure BDA0001954355710000033
and
Figure BDA0001954355710000034
Wherein, x, y, z are the initial position coordinates of the magnetic source to be located, A x , A y , A z are the position coordinates of the full tensor magnetic gradient measurement component at a selected measuring point, PA , Q A , H A are the unit vectors of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to a selected measuring point in a static state, and B x , By y , B z are another options The position coordinates of the full tensor magnetic gradient measurement component of the fixed measuring point, P B , Q B , H B are the described full tensor magnetic gradients from the magnetic source to be positioned to another selected measuring point in a static state A unit vector that measures the component's position vector.

可选地,根据全张量不变量建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型的方法包括:根据全张量不变量

Figure BDA0001954355710000035
建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型
Figure BDA0001954355710000036
其中,MT为全张量不变量,MT1为静止状态下的待定位磁源在同一测点的全张量磁梯度测量组件处产生的全张量不变量,MT2为运动状态下的待定位磁源在同一测点的全张量磁梯度测量组件处产生的全张量不变量,λ1、λ2、λ3为全张量磁梯度矩阵的特征值,μ0为真空磁导率,M为待定位磁源的磁矩的模,R为全张量磁梯度测量组件与待定位磁源之间的距离,R1为同一测点处全张量磁梯度测量组件与静止状态下的待定位磁源之间的距离,R2为同一测点处全张量磁梯度测量组件与运动状态下的待定位磁源之间的距离。Optionally, the method for establishing the distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located according to the full tensor invariant includes: according to the full tensor invariant
Figure BDA0001954355710000035
Establishing a distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located
Figure BDA0001954355710000036
Among them, MT is the full tensor invariant, MT 1 is the full tensor invariant generated by the magnetic source to be located in the static state at the full tensor magnetic gradient measurement component at the same measuring point, and MT 2 is the undetermined magnetic source in the moving state The full tensor invariant produced by the bit magnetic source at the full tensor magnetic gradient measurement component at the same measuring point, λ 1 , λ 2 , λ 3 are the eigenvalues of the full tensor magnetic gradient matrix, and μ 0 is the vacuum permeability , M is the modulus of the magnetic moment of the magnetic source to be positioned, R is the distance between the full tensor magnetic gradient measurement component and the magnetic source to be positioned, R 1 is the distance between the full tensor magnetic gradient measurement component at the same measuring point and the static state R2 is the distance between the full tensor magnetic gradient measurement component at the same measuring point and the magnetic source to be located in the moving state.

可选地,获取运动状态下所述待定位磁源的实时位置坐标的方法包括:Optionally, the method for obtaining the real-time position coordinates of the magnetic source to be positioned in a moving state includes:

根据运动状态下所述待定位磁源在该选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值获取运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;According to the magnetic field gradient value generated at the full tensor magnetic gradient measurement component of the selected measuring point by the magnetic source to be positioned in the moving state, the distance from the magnetic source to be positioned to the selected measuring point in the moving state is obtained. The unit vector of the position vector of the full tensor magnetic gradient measurement component;

根据所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型、同一选定测点对应的不同状态下的所述磁场梯度值、所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标获取该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离;According to the distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located, the magnetic field gradient values in different states corresponding to the same selected measuring point, and the initial position of the magnetic source to be located The coordinates and the position coordinates corresponding to the selected measuring point obtain the distance between the full tensor magnetic gradient measurement component of the selected measuring point and the magnetic source to be positioned in the motion state;

根据该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离及运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量获取运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量,从而获取运动状态下所述待定位磁源的实时位置坐标。According to the distance between the full tensor magnetic gradient measurement component at the selected measuring point and the magnetic source to be positioned in the moving state and the full distance from the magnetic source to be positioned to the selected measuring point in the moving state The unit vector of the position vector of the tensor magnetic gradient measurement component obtains the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the selected measuring point in the motion state, thereby obtaining the position to be determined in the motion state The real-time position coordinates of the bit magnetic source.

如上所述,本发明的一种磁源的静态定位装置及静态定位方法,利用由安装支架或低温容器、全张量磁梯度测量组件、位置定位器及测控组件构成的静态定位装置先获取磁源在静止状态下的初始位置坐标,之后再获取磁源在运动状态下对应的磁场梯度值,以实现根据距离比值模型获取磁源在运动状态下的实时位置坐标;在获取初始位置坐标时,采集磁源到两选定测点的全张量磁梯度测量组件处的磁场梯度值,并结合与姿态无关的全张量不变量获取磁源到两选定测点的全张量磁梯度测量组件的位置矢量的单位向量,同时去除了虚解,之后再结合两选定测点的位置坐标建立空间直线模型以获取磁源在静止状态下的初始位置坐标。可见,本发明所述静态定位方法无需知道磁源的总场信息,只通过磁源在静止状态下的初始位置坐标、磁源在运动状态下的磁场梯度值及距离比值模型即可实现磁源在运动状态下的高精度实时定位;同时本发明所述静态定位装置及静态定位方法可充分发挥基于超导磁传感器构建的全张量磁梯度测量组件的灵敏度优势,实现远距离高精度实时定位;而且本发明所述静态定位装置及静态定位方法操作简单快速、便于实现,非常适合在磁法定位测量领域中应用。As mentioned above, a static positioning device and a static positioning method for a magnetic source of the present invention use a static positioning device composed of a mounting bracket or a cryogenic container, a full tensor magnetic gradient measurement component, a position locator, and a measurement and control component to first obtain the magnetic field. The initial position coordinates of the source in a static state, and then obtain the magnetic field gradient value corresponding to the magnetic source in a moving state, so as to obtain the real-time position coordinates of the magnetic source in a moving state according to the distance ratio model; when obtaining the initial position coordinates, Collect the magnetic field gradient value at the full tensor magnetic gradient measurement component from the magnetic source to the two selected measuring points, and combine the attitude-independent full tensor invariant to obtain the full tensor magnetic gradient measurement from the magnetic source to the two selected measuring points The unit vector of the position vector of the component, and remove the virtual solution, and then combine the position coordinates of the two selected measuring points to establish a space linear model to obtain the initial position coordinates of the magnetic source in the static state. It can be seen that the static positioning method of the present invention does not need to know the total field information of the magnetic source, only the initial position coordinates of the magnetic source in the static state, the magnetic field gradient value and the distance ratio model of the magnetic source in the moving state can realize the magnetic source positioning. High-precision real-time positioning in a moving state; at the same time, the static positioning device and static positioning method of the present invention can give full play to the sensitivity advantages of the full tensor magnetic gradient measurement component based on the superconducting magnetic sensor, and realize long-distance high-precision real-time positioning ; Moreover, the static positioning device and the static positioning method of the present invention are simple, quick and easy to implement, and are very suitable for application in the field of magnetic positioning measurement.

附图说明Description of drawings

图1显示为本发明实施例一所述磁源静态定位装置的结构示意图。FIG. 1 is a schematic structural diagram of a magnetic source static positioning device according to Embodiment 1 of the present invention.

图2显示为本发明实施例二所述磁源静态定位装置的结构示意图。Fig. 2 is a schematic structural diagram of the magnetic source static positioning device according to the second embodiment of the present invention.

图3显示为本发明实施例三所述磁源静态定位方法的流程图。Fig. 3 is a flow chart of the magnetic source static positioning method according to the third embodiment of the present invention.

图4显示为本发明实施例三中待定位磁源存在虚解时的分布示意图,图中A为真实磁源,A’为虚解,B1为第一测点,B2为第二测点。4 is a schematic diagram showing the distribution of the magnetic source to be located when there is a virtual solution in Embodiment 3 of the present invention. In the figure, A is the real magnetic source, A' is the virtual solution, B1 is the first measuring point, and B2 is the second measuring point.

元件标号说明Component designation description

100                    磁源的静态定位装置100 static positioning device for magnetic source

101                    安装支架101 Mounting bracket

102                    全张量磁梯度测量组件102 Full tensor magnetic gradient measurement component

103                    位置定位器103 Position Locator

104                    测控组件104 Measurement and control components

200                    地面200 ground

300                    待定位磁源300 Magnetic sources to be located

400                    磁源的静态定位装置400 static positioning device for magnetic source

401                    低温容器401 Cryogenic container

402                    全张量磁梯度测量组件402 Full tensor magnetic gradient measurement component

403                    位置定位器403 Location Locator

404                    测控组件404 Measurement and Control Components

具体实施方式Detailed ways

以下通过特定的具体实例说明本发明的实施方式,本领域技术人员可由本说明书所揭露的内容轻易地了解本发明的其他优点与功效。本发明还可以通过另外不同的具体实施方式加以实施或应用,本说明书中的各项细节也可以基于不同观点与应用,在没有背离本发明的精神下进行各种修饰或改变。Embodiments of the present invention are described below through specific examples, and those skilled in the art can easily understand other advantages and effects of the present invention from the content disclosed in this specification. The present invention can also be implemented or applied through other different specific implementation modes, and various modifications or changes can be made to the details in this specification based on different viewpoints and applications without departing from the spirit of the present invention.

请参阅图1至图4。需要说明的是,本实施例中所提供的图示仅以示意方式说明本发明的基本构想,遂图示中仅显示与本发明中有关的组件而非按照实际实施时的组件数目、形状及尺寸绘制,其实际实施时各组件的形态、数量及比例可为一种随意的改变,且其组件布局形态也可能更为复杂。See Figures 1 through 4. It should be noted that the diagrams provided in this embodiment are only schematically illustrating the basic idea of the present invention, so that only the components related to the present invention are shown in the diagrams rather than the number, shape and Dimensional drawing, the shape, quantity and proportion of each component can be changed arbitrarily during actual implementation, and the layout of the components may also be more complicated.

实施例一Embodiment one

如图1所示,本实施例提供一种磁源的静态定位装置,所述静态定位装置100包括:As shown in FIG. 1 , this embodiment provides a static positioning device for a magnetic source, and the static positioning device 100 includes:

安装支架101,用于提供安装平台;The mounting bracket 101 is used to provide a mounting platform;

全张量磁梯度测量组件102,设于所述安装支架101上,用于测量待定位磁源300在所述全张量磁梯度测量组件102处产生的磁场梯度值;The full tensor magnetic gradient measurement component 102 is arranged on the mounting bracket 101, and is used to measure the magnetic field gradient value generated by the magnetic source 300 to be positioned at the full tensor magnetic gradient measurement component 102;

位置定位器103,刚性连接于所述全张量磁梯度测量组件102,用于测量所述全张量磁梯度测量组件102在地理坐标系下的位置坐标;A position locator 103, rigidly connected to the full tensor magnetic gradient measurement assembly 102, for measuring the position coordinates of the full tensor magnetic gradient measurement assembly 102 in the geographic coordinate system;

测控组件104,电连接于所述全张量磁梯度测量组件102及所述位置定位器103,用于采集所述磁场梯度值及所述位置坐标,并根据采集的数据对运动状态下的所述待定位磁源300进行实时定位。The measurement and control component 104 is electrically connected to the full tensor magnetic gradient measurement component 102 and the position locator 103, and is used to collect the magnetic field gradient value and the position coordinates, and to monitor the motion state according to the collected data. The magnetic source 300 to be positioned is used for real-time positioning.

作为示例,所述安装支架101为任一种可实现安装固定作用的结构,本实施例并不对所述安装支架101的具体结构进行限制。具体的,如图1所示,所述安装支架101包括三个层级,其中,所述全张量磁梯度测量组件102安装于所述安装支架101的第一层级(即安装支架101的底部),所述位置定位器103安装于所述安装支架101的第三层级(即安装支架101的上部),所述测控组件104安装于所述安装支架101的第二层级(即安装支架101的中部);当然,在其它实施例中,所述全张量磁梯度测量组件102、所述位置定位器103及所述测控组件104所在层级可以互换,本实施例并不对所述全张量磁梯度测量组件102、所述位置定位器103及所述测控组件104的上下位置关系进行限制,而且所述位置定位器103及所述测控组件104也可不安装于所述安装支架101上,即所述位置定位器103及所述测控组件104安装于所述安装支架101外。As an example, the mounting bracket 101 is any structure capable of mounting and fixing, and this embodiment does not limit the specific structure of the mounting bracket 101 . Specifically, as shown in FIG. 1, the installation bracket 101 includes three levels, wherein the full tensor magnetic gradient measurement assembly 102 is installed on the first level of the installation bracket 101 (ie, the bottom of the installation bracket 101) , the position locator 103 is installed on the third level of the installation bracket 101 (ie, the upper part of the installation bracket 101), and the measurement and control component 104 is installed on the second level of the installation bracket 101 (ie, the middle of the installation bracket 101 ); Of course, in other embodiments, the levels where the full tensor magnetic gradient measurement assembly 102, the position locator 103 and the measurement and control assembly 104 are located can be interchanged, and this embodiment does not apply to the full tensor magnetic Gradient measurement component 102, the position locator 103 and the measurement and control component 104 limit the vertical position relationship, and the position locator 103 and the measurement and control component 104 may not be installed on the installation bracket 101, that is, the The position locator 103 and the measurement and control component 104 are installed outside the installation bracket 101 .

作为示例,所述全张量磁梯度测量组件102包括:至少一个磁强计,即通过对至少一个磁强计按一定的物理构型进行搭建以形成所述全张量磁梯度测量组件102。需要注意的是,所述全张量磁梯度测量组件102的最终结构由所述磁强计的数量及搭建的物理构型决定,也就是说,不同数量的磁强计按不同的物理构型搭建形成的所述全张量磁梯度测量组件102的最终结构不同,但本实施例所述静态定位装置适用于任何所述全张量磁梯度测量组件102的最终结构。特别需要注意的是,由于本实施例所述全张量磁梯度测量组件102为非超导器件,故其工作于常温环境中。As an example, the full tensor magnetic gradient measurement component 102 includes: at least one magnetometer, that is, the full tensor magnetic gradient measurement component 102 is formed by building at least one magnetometer according to a certain physical configuration. It should be noted that the final structure of the full tensor magnetic gradient measurement assembly 102 is determined by the quantity of the magnetometers and the physical configuration of the building, that is to say, different numbers of magnetometers have different physical configurations. The final structure of the full tensor magnetic gradient measurement assembly 102 formed by building is different, but the static positioning device described in this embodiment is applicable to any final structure of the full tensor magnetic gradient measurement assembly 102 . It should be particularly noted that since the full tensor magnetic gradient measurement component 102 in this embodiment is a non-superconducting device, it works in a normal temperature environment.

作为示例,所述位置定位器103包括:差分GPS接收机或组合惯导。具体的,在所述全张量磁梯度测量组件102与所述位置定位器103之间不存在空间距离时,采用差分GPS接收机测量所述全张量磁梯度测量组件102的位置坐标,即差分GPS接收机的位置坐标即为所述全张量磁梯度测量组件102的位置坐标;在所述全张量磁梯度测量组件102与所述位置定位器103之间存在空间距离时,采用组合惯导测量所述全张量磁梯度测量组件102的位置坐标,即利用所述组合惯导的坐标点偏移设置功能直接测得所述全张量磁梯度测量组件102与所述位置定位器103之间的偏移量,并基于该偏移量对测得的位置坐标(即所述组合惯导的位置坐标)进行修正,从而得到所述全张量磁梯度测量组件102的位置坐标。需要注意的是,通过差分GPS接收机测量位置坐标,通过组合惯导测量位置坐标、测量偏移量、及基于偏移量对位置坐标进行修正均是本领域技术人员所公知的,故在此不再赘述。As an example, the position locator 103 includes: a differential GPS receiver or an integrated inertial navigation system. Specifically, when there is no spatial distance between the full tensor magnetic gradient measurement component 102 and the position locator 103, a differential GPS receiver is used to measure the position coordinates of the full tensor magnetic gradient measurement component 102, namely The position coordinates of the differential GPS receiver are the position coordinates of the full tensor magnetic gradient measurement assembly 102; Inertial navigation measures the position coordinates of the full tensor magnetic gradient measurement component 102, that is, the coordinate point offset setting function of the combined inertial navigation is used to directly measure the full tensor magnetic gradient measurement component 102 and the position locator 103, and based on the offset, the measured position coordinates (that is, the position coordinates of the integrated inertial navigation) are corrected, so as to obtain the position coordinates of the full tensor magnetic gradient measurement assembly 102. It should be noted that measuring the position coordinates through a differential GPS receiver, measuring the position coordinates by combining inertial navigation, measuring the offset, and correcting the position coordinates based on the offset are all known to those skilled in the art, so here No longer.

作为示例,所述测控组件104为现有任一种可实现磁场梯度值和位置坐标采集、处理的装置,本实施例并不对所述测控组件104的结构进行限制。As an example, the measurement and control component 104 is any existing device capable of collecting and processing magnetic field gradient values and position coordinates, and this embodiment does not limit the structure of the measurement and control component 104 .

实施例二Embodiment two

如图2所示,本实施例提供一种磁源的静态定位装置,所述静态定位装置400包括:As shown in FIG. 2 , this embodiment provides a static positioning device for a magnetic source, and the static positioning device 400 includes:

低温容器401,用于提供安装平台,同时提供低温环境;The cryogenic container 401 is used to provide an installation platform and provide a low temperature environment;

全张量磁梯度测量组件402,设于所述低温容器401内,用于测量待定位磁源300在所述全张量磁梯度测量组件402处产生的磁场梯度值;The full tensor magnetic gradient measurement component 402 is arranged in the cryogenic container 401, and is used to measure the magnetic field gradient value generated by the magnetic source 300 to be positioned at the full tensor magnetic gradient measurement component 402;

位置定位器403,刚性连接于所述全张量磁梯度测量组件402,用于测量所述全张量磁梯度测量组件402在地理坐标系下的位置坐标;A position locator 403, rigidly connected to the full tensor magnetic gradient measurement assembly 402, for measuring the position coordinates of the full tensor magnetic gradient measurement assembly 402 in the geographic coordinate system;

测控组件404,电连接于所述全张量磁梯度测量组件402及所述位置定位器403,用于采集所述磁场梯度值及所述位置坐标,并根据采集的数据对运动状态下的所述待定位磁源300进行实时定位。The measurement and control component 404 is electrically connected to the full tensor magnetic gradient measurement component 402 and the position locator 403, and is used to collect the magnetic field gradient value and the position coordinates, and to monitor the motion state according to the collected data. The magnetic source 300 to be positioned is used for real-time positioning.

作为示例,所述低温容器401包括低温杜瓦,而低温杜瓦是本领域技术人员所公知的,故在此不再赘述。As an example, the cryogenic container 401 includes a cryogenic Dewar, and the cryogenic Dewar is well known to those skilled in the art, so details will not be repeated here.

作为示例,所述全张量磁梯度测量组件402包括:至少一个平面梯度计,即通过对至少一个平面梯度计按一定的物理构型进行搭建以形成所述全张量磁梯度测量组件402。需要注意的是,所述全张量磁梯度测量组件402的最终结构由所述平面梯度计的数量及搭建的物理构型决定,也就是说,不同数量的平面梯度计按不同的物理构型搭建形成的所述全张量磁梯度测量组件402的最终结构不同,但本实施例所述静态定位装置适用于任何所述全张量磁梯度测量组件402的最终结构。特别需要注意的是,由于本实施例所述全张量磁梯度测量组件402为超导器件,故其工作于低温环境中。As an example, the full tensor magnetic gradient measurement component 402 includes: at least one planar gradiometer, that is, the full tensor magnetic gradient measurement component 402 is formed by building at least one planar gradiometer according to a certain physical configuration. It should be noted that the final structure of the full tensor magnetic gradiometer assembly 402 is determined by the number of the planar gradiometers and the physical configuration built, that is to say, different numbers of planar gradiometers have different physical configurations. The final structure of the full tensor magnetic gradient measurement assembly 402 formed by building is different, but the static positioning device described in this embodiment is applicable to any final structure of the full tensor magnetic gradient measurement assembly 402 . It should be particularly noted that since the full tensor magnetic gradient measurement component 402 in this embodiment is a superconducting device, it works in a low temperature environment.

作为示例,所述位置定位器403包括:差分GPS接收机或组合惯导。具体的,在所述全张量磁梯度测量组件402与所述位置定位器403之间不存在空间距离时,采用差分GPS接收机测量所述全张量磁梯度测量组件402的位置坐标,即差分GPS接收机的位置坐标即为所述全张量磁梯度测量组件402的位置坐标;在所述全张量磁梯度测量组件402与所述位置定位器403之间存在空间距离时,采用组合惯导测量所述全张量磁梯度测量组件402的位置坐标,即利用所述组合惯导的坐标点偏移设置功能直接测得所述全张量磁梯度测量组件402与所述位置定位器403之间的偏移量,并基于该偏移量对测得的位置坐标(即所述组合惯导的位置坐标)进行修正,从而得到所述全张量磁梯度测量组件402的位置坐标。需要注意的是,通过差分GPS接收机测量位置坐标,通过组合惯导测量位置坐标、测量偏移量、及基于偏移量对位置坐标进行修正均是本领域技术人员所公知的,故在此不再赘述。As an example, the position locator 403 includes: a differential GPS receiver or an integrated inertial navigation system. Specifically, when there is no spatial distance between the full tensor magnetic gradient measurement component 402 and the position locator 403, a differential GPS receiver is used to measure the position coordinates of the full tensor magnetic gradient measurement component 402, namely The position coordinates of the differential GPS receiver are the position coordinates of the full tensor magnetic gradient measurement assembly 402; when there is a spatial distance between the full tensor magnetic gradient measurement assembly 402 and the position locator 403, the combined Inertial navigation measures the position coordinates of the full tensor magnetic gradient measurement component 402, that is, the coordinate point offset setting function of the combined inertial navigation is used to directly measure the full tensor magnetic gradient measurement component 402 and the position locator 403, and based on the offset, correct the measured position coordinates (that is, the position coordinates of the integrated inertial navigation), so as to obtain the position coordinates of the full tensor magnetic gradient measurement component 402. It should be noted that measuring the position coordinates through a differential GPS receiver, measuring the position coordinates by combining inertial navigation, measuring the offset, and correcting the position coordinates based on the offset are all known to those skilled in the art, so here No longer.

作为示例,所述测控组件404为现有任一种可实现磁场梯度值和位置坐标采集、处理的装置,本实施例并不对所述测控组件404的结构进行限制。As an example, the measurement and control component 404 is any existing device capable of collecting and processing magnetic field gradient values and position coordinates, and this embodiment does not limit the structure of the measurement and control component 404 .

实施例三Embodiment three

如图3所示,本实施例提供一种磁源的静态定位方法,所述静态定位方法包括:As shown in FIG. 3 , this embodiment provides a static positioning method for a magnetic source, and the static positioning method includes:

搭建如实施例一或实施例二所述的静态定位装置;Build the static positioning device as described in Embodiment 1 or Embodiment 2;

在所述待定位磁源处于静止状态时,获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并获取两选定测点的所述全张量磁梯度测量组件的位置坐标,以实现根据全张量不变量获取静止状态下所述待定位磁源的初始位置坐标;When the magnetic source to be positioned is in a static state, obtain the magnetic field gradient values generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement components at two selected measuring points in the static state, and obtain two selected The position coordinates of the full tensor magnetic gradient measurement component of the measuring point, so as to obtain the initial position coordinates of the magnetic source to be positioned in a static state according to the full tensor invariant;

在所述待定位磁源处于运动状态时,获取运动状态下所述待定位磁源在任一所述选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值;When the magnetic source to be positioned is in a moving state, obtain the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component at any one of the selected measuring points in the moving state;

根据全张量不变量建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型,以实现根据同一选定测点对应的不同状态下的所述磁场梯度值、所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标获取运动状态下所述待定位磁源的实时位置坐标。Establishing a distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located according to the full tensor invariant, so as to realize the magnetic field gradient values, The initial position coordinates of the magnetic source to be located and the position coordinates corresponding to the selected measuring point obtain the real-time position coordinates of the magnetic source to be located in a moving state.

需要注意的是,本实施例所述静态定位装置的组成、搭建具体请参阅实施例一或实施例二,本实施例不再对所述静态定位装置的组成及搭建进行说明。It should be noted that for the composition and construction of the static positioning device described in this embodiment, please refer to Embodiment 1 or Embodiment 2 for details, and this embodiment will not describe the composition and construction of the static positioning device.

作为示例,在所述待定位磁源处于静止状态时,通过搬运所述静态定位装置以实现获取不同测点对应的所述磁场梯度值及位置坐标。具体的,可通过仅搬运一次所述静态定位装置获得两测点对应的所述磁场梯度值及位置坐标;也可通过搬运多次所述静态定位装置以获得多个不同测点对应的所述磁场梯度值及位置坐标,并从中选出两个测点作为所述选定测点,从而获得该两选定测点对应的所述磁场梯度值及位置坐标;甚至可通过搬运多次所述静态定位装置来获取多个测点,并对多个测点两两组合以获取多组初始位置坐标,最后通过求取平均值以得到最终的初始位置坐标。需要注意的是,本实施例可通过判断定点测量的全张量磁梯度是否变化来确定所述待定位磁源是处于静止状态还是运动状态,当然,确定所述待定位磁源是处于静止状态还是运动状态并不仅限于上述方法,但由于这些方法均是本领域技术人员所公知的,故在此不再赘述。As an example, when the magnetic source to be positioned is in a static state, the static positioning device is transported to obtain the magnetic field gradient values and position coordinates corresponding to different measuring points. Specifically, the magnetic field gradient values and position coordinates corresponding to the two measuring points can be obtained by only carrying the static positioning device once; it is also possible to obtain the corresponding values of multiple different measuring points by carrying the static positioning device multiple times. magnetic field gradient value and position coordinates, and select two measuring points as the selected measuring points, thereby obtaining the magnetic field gradient value and position coordinates corresponding to the two selected measuring points; The static positioning device is used to obtain multiple measuring points, and the multiple measuring points are combined in pairs to obtain multiple sets of initial position coordinates, and finally the final initial position coordinates are obtained by calculating the average value. It should be noted that this embodiment can determine whether the magnetic source to be positioned is in a static state or a moving state by judging whether the full tensor magnetic gradient measured at a fixed point changes. Of course, it is determined whether the magnetic source to be positioned is in a static state Also, the motion state is not limited to the above methods, but since these methods are well known to those skilled in the art, they will not be repeated here.

其中,获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值的方法包括:获取静止状态下所述待定位磁源在不同测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并对不同测点对应的所述磁场梯度值进行信噪比比较以选出信噪比最优的两个所述磁场梯度值;其中,选出的两个所述磁场梯度值对应的测点作为所述选定测点。需要注意的是,通过所述全张量磁梯度测量组件测量所述待定位磁源在所述全张量磁梯度测量组件处产生的磁场梯度值及对输出信号进行信噪比计算均是本领域技术人员所公知的,故在此不再赘述。Wherein, the method for obtaining the magnetic field gradient values generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement components at two selected measuring points in the static state includes: obtaining the magnetic source to be positioned in the static state at different The magnetic field gradient value generated at the full tensor magnetic gradient measurement component of the measuring point, and compare the signal-to-noise ratio of the magnetic field gradient values corresponding to different measuring points to select the two magnetic fields with the best signal-to-noise ratio Gradient value; wherein, the selected measuring points corresponding to the two magnetic field gradient values are used as the selected measuring points. It should be noted that the measurement of the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component through the full tensor magnetic gradient measurement component and the calculation of the signal-to-noise ratio of the output signal are both basic It is well known to those skilled in the art, so it will not be repeated here.

其中,在所述全张量磁梯度测量组件与所述位置定位器之间不存在空间距离时,可通过所述位置定位器(如差分GPS接收机)直接获取所述全张量磁梯度测量组件的位置坐标,即所述位置定位器的位置坐标即为所述全张量磁梯度测量组件的位置坐标。在所述全张量磁梯度测量组件与所述位置定位器之间存在空间距离时,获取所述全张量磁梯度测量组件位置坐标的方法包括:获取所述位置定位器的位置坐标,并获取所述全张量磁梯度测量组件与所述位置定位器之间的偏移量;基于所述偏移量对所述位置坐标进行修正,以获取所述全张量磁梯度测量组件的位置坐标。如利用所述组合惯导的坐标点偏移设置功能直接测量所述全张量磁梯度测量组件与所述位置定位器之间的偏移量,并通过所述组合惯导测量其自身的位置坐标,之后再基于所述偏移量对所述位置坐标进行修正以获取所述全张量磁梯度测量组件的位置坐标。需要注意的是,通过差分GPS接收机或组合惯导测量位置坐标、利用组合惯导的坐标点偏移设置功能测量偏移量、及根据偏移量对位置坐标进行修正均是本领域技术人员所公知的,故在此不再赘述。Wherein, when there is no spatial distance between the full tensor magnetic gradient measurement component and the position locator, the full tensor magnetic gradient measurement can be directly obtained by the position locator (such as a differential GPS receiver) The position coordinates of the component, that is, the position coordinates of the position locator are the position coordinates of the full tensor magnetic gradient measurement component. When there is a spatial distance between the full tensor magnetic gradient measurement component and the position locator, the method for obtaining the position coordinates of the full tensor magnetic gradient measurement component includes: acquiring the position coordinates of the position locator, and Obtain an offset between the full tensor magnetic gradient measurement component and the position locator; correct the position coordinates based on the offset to obtain the position of the full tensor magnetic gradient measurement component coordinate. For example, using the coordinate point offset setting function of the combined inertial navigation to directly measure the offset between the full tensor magnetic gradient measurement component and the position locator, and measure its own position through the combined inertial navigation coordinates, and then correct the position coordinates based on the offset to obtain the position coordinates of the full tensor magnetic gradient measurement component. It should be noted that measuring the position coordinates through a differential GPS receiver or integrated inertial navigation, using the coordinate point offset setting function of the integrated inertial navigation to measure the offset, and correcting the position coordinates according to the offset are all those skilled in the art. known, so it will not be repeated here.

作为示例,获取所述待定位磁源的初始位置坐标的方法包括:As an example, the method for obtaining the initial position coordinates of the magnetic source to be located includes:

根据两选定测点对应的所述磁场梯度值及全张量不变量获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;Acquire the unit of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in a static state according to the magnetic field gradient values corresponding to the two selected measuring points and the full tensor invariant vector;

根据两选定测点对应的位置坐标及静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量建立空间直线模型,以获取所述待定位磁源的初始位置坐标。According to the position coordinates corresponding to the two selected measuring points and the unit vector of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in a static state, a space linear model is established to obtain the Describe the initial position coordinates of the magnetic source to be located.

具体的,获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量的方法包括:Specifically, the method for obtaining the unit vector of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in the static state includes:

根据两选定测点对应的所述磁场梯度值分别获取两选定测点对应的全张量磁梯度矩阵特征值;Obtaining the full tensor magnetic gradient matrix eigenvalues corresponding to the two selected measuring points respectively according to the magnetic field gradient values corresponding to the two selected measuring points;

根据两选定测点对应的全张量磁梯度矩阵特征值分别获取两选定测点对应的全张量磁梯度矩阵最小绝对特征值,并根据两选定测点对应的全张量磁梯度矩阵最小绝对特征值获取一参考方向向量;其中,所述参考方向向量平行于静止状态下所述待定位磁源磁矩的方向向量;According to the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points, the minimum absolute eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points are respectively obtained, and according to the full tensor magnetic gradient matrix corresponding to the two selected measuring points The minimum absolute eigenvalue of the matrix obtains a reference direction vector; wherein, the reference direction vector is parallel to the direction vector of the magnetic moment of the magnetic source to be located in a static state;

根据全张量不变量

Figure BDA0001954355710000101
确定静止状态下所述待定位磁源的磁矩矢量的单位向量,从而获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;其中,MT为全张量不变量,λ1、λ2、λ3为全张量磁梯度矩阵特征值,μ0为真空磁导率,M为待定位磁源的磁矩的模,R为全张量磁梯度测量组件与待定位磁源之间的距离。According to the full tensor invariant
Figure BDA0001954355710000101
Determine the unit vector of the magnetic moment vector of the magnetic source to be positioned in the static state, thereby obtaining the unit of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in the static state vector; where, MT is the full tensor invariant, λ 1 , λ 2 , λ 3 are the eigenvalues of the full tensor magnetic gradient matrix, μ 0 is the vacuum permeability, M is the modulus of the magnetic moment of the magnetic source to be positioned, R is the distance between the full tensor magnetic gradient measurement component and the magnetic source to be located.

其中,根据两选定测点对应的所述磁场梯度值分别获取两选定测点对应的全张量磁梯度矩阵特征值的方法包括:根据两选定测点对应的所述磁场梯度值分别获取该两选定测点对应的全张量磁梯度矩阵,之后再根据所述全张量磁梯度矩阵分别获取该两选定测点对应的全张量磁梯度矩阵特征值λ1、λ2、λ3;其中,λ2≥λ3≥λ1,|λ1|≥|λ3|,|λ2|≥|λ3|。需要注意的是,根据磁场梯度值得到全张量磁梯度矩阵及根据全张量磁梯度矩阵得到全张量磁梯度矩阵特征值λ1、λ2、λ3均是本领域技术人员所公知的,故在此不再赘述。Wherein, the method for obtaining the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points according to the magnetic field gradient values corresponding to the two selected measuring points respectively includes: according to the magnetic field gradient values corresponding to the two selected measuring points, respectively Obtain the full tensor magnetic gradient matrix corresponding to the two selected measuring points, and then respectively obtain the eigenvalues λ 1 and λ 2 of the full tensor magnetic gradient matrix corresponding to the two selected measuring points according to the full tensor magnetic gradient matrix , λ 3 ; where, λ 2 ≥λ 3 ≥λ 1 , |λ 1 |≥|λ 3 |, |λ 2 |≥|λ 3 |. It should be noted that obtaining the full tensor magnetic gradient matrix according to the magnetic field gradient value and obtaining the eigenvalues λ 1 , λ 2 , and λ 3 of the full tensor magnetic gradient matrix according to the full tensor magnetic gradient matrix are well known to those skilled in the art , so it will not be repeated here.

其中,获取所述参考方向向量的方法包括:根据两选定测点对应的全张量磁梯度矩阵最小绝对特征值获取其对应的特征向量,并通过对两所述特征向量求取向量积以获取所述参考方向向量。本实施例利用全张量磁梯度矩阵最小绝对特征值对应的特征向量垂直于待定位磁源的磁矩矢量和待定位磁源到选定测点的全张量磁梯度测量组件的位置矢量(即V3*m=0,其中V3是全张量磁梯度矩阵最小绝对特征值λ3对应的特征向量,m是待定位磁源的磁矩矢量),通过对两选定测点对应的特征向量求取向量积,从而得到与静止状态下所述待定位磁源磁矩的方向向量平行的参考方向向量(即求取的向量积即为所述参考方向向量);其中参考方向向量

Figure BDA0001954355710000102
ms是参考方向向量,i、j、k分别是x、y、z轴方向的单位向量,V3iA、V3jA、V3kA是一选定测点对应的全张量磁梯度矩阵最小绝对特征值的特征向量在x、y、z坐标系中的坐标,V3iB、V3jB、V3kB是另一选定测点对应的全张量磁梯度矩阵最小绝对特征值的特征向量在x、y、z坐标系中的坐标。需要注意的是,本实施例所述全张量磁梯度矩阵最小绝对特征值是指全张量磁梯度矩阵特征值中绝对值最小的一个,即λ3。Wherein, the method for obtaining the reference direction vector includes: obtaining the corresponding eigenvector according to the minimum absolute eigenvalue of the full tensor magnetic gradient matrix corresponding to the two selected measuring points, and obtaining the vector product of the two eigenvectors to obtain Get the reference direction vector. This embodiment utilizes the eigenvector corresponding to the minimum absolute eigenvalue of the full tensor magnetic gradient matrix to be perpendicular to the magnetic moment vector of the magnetic source to be located and the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be located to the selected measuring point ( That is V 3 *m=0, wherein V 3 is the eigenvector corresponding to the minimum absolute eigenvalue λ 3 of the full tensor magnetic gradient matrix, and m is the magnetic moment vector of the magnetic source to be located), by corresponding to the two selected measuring points Eigenvector obtains the vector product, thereby obtains the reference direction vector parallel to the direction vector of the magnetic moment of the magnetic source to be positioned in the static state (that is, the vector product obtained is the reference direction vector); wherein the reference direction vector
Figure BDA0001954355710000102
m s is the reference direction vector, i, j, k are unit vectors in the directions of x, y, and z axes respectively, V 3iA , V 3jA , V 3kA are the minimum absolute features of the full tensor magnetic gradient matrix corresponding to a selected measuring point The coordinates of the eigenvector of the value in the x, y, z coordinate system, V 3iB , V 3jB , V 3kB are the eigenvectors of the minimum absolute eigenvalues of the full tensor magnetic gradient matrix corresponding to another selected measuring point in x, y , coordinates in the z coordinate system. It should be noted that the smallest absolute eigenvalue of the full tensor magnetic gradient matrix in this embodiment refers to the one with the smallest absolute value among the eigenvalues of the full tensor magnetic gradient matrix, that is, λ 3 .

由于所述待定位磁源的磁矩矢量的单位向量

Figure BDA0001954355710000111
和所述待定位磁源到选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量
Figure BDA0001954355710000112
均可由全张量磁梯度矩阵特征值λ1、λ2、λ3和绝对值较大的两个特征值λ1、λ2对应的特征向量V1、V2表示,即
Figure BDA0001954355710000113
Figure BDA0001954355710000114
其中
Figure BDA0001954355710000115
Figure BDA0001954355710000116
Figure BDA0001954355710000117
可见磁矩矢量的单位向量
Figure BDA0001954355710000118
和位置矢量的单位向量~r均存在虚解,但鉴于磁矩矢量和位置矢量的夹角是确定的,故磁矩矢量的单位向量
Figure BDA0001954355710000119
和位置矢量的单位向量
Figure BDA00019543557100001110
只有如下四种组合,也即存在3个虚解;而在已知所述参考方向向量平行于静止状态下所述待定位磁源的磁矩的方向向量时,可根据所述参考方向向量去除两个虚解;如图4所示,在已知所述参考方向向量时,可将位于第二象限和第四象限中的虚解去除。Due to the unit vector of the magnetic moment vector of the magnetic source to be positioned
Figure BDA0001954355710000111
and the unit vector of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the selected measuring point
Figure BDA0001954355710000112
Both can be expressed by the eigenvalues λ 1 , λ 2 , λ 3 of the full tensor magnetic gradient matrix and the eigenvectors V 1 and V 2 corresponding to the two eigenvalues λ 1 and λ 2 with relatively large absolute values, namely
Figure BDA0001954355710000113
and
Figure BDA0001954355710000114
in
Figure BDA0001954355710000115
Figure BDA0001954355710000116
Figure BDA0001954355710000117
The unit vector of the visible magnetic moment vector
Figure BDA0001954355710000118
and the unit vector ~r of the position vector have virtual solutions, but since the angle between the magnetic moment vector and the position vector is determined, the unit vector of the magnetic moment vector
Figure BDA0001954355710000119
and the unit vector of the position vector
Figure BDA00019543557100001110
There are only the following four combinations, that is, there are 3 virtual solutions; and when the reference direction vector is known to be parallel to the direction vector of the magnetic moment of the magnetic source to be located in the static state, it can be removed according to the reference direction vector Two virtual solutions; as shown in FIG. 4 , when the reference direction vector is known, the virtual solutions located in the second quadrant and the fourth quadrant can be removed.

组合一:

Figure BDA00019543557100001111
Combination one:
Figure BDA00019543557100001111

组合二:

Figure BDA00019543557100001112
Combination two:
Figure BDA00019543557100001112

组合三:

Figure BDA00019543557100001113
Combination three:
Figure BDA00019543557100001113

组合四:

Figure BDA00019543557100001114
Combination four:
Figure BDA00019543557100001114

其中,确定静止状态下所述待定位磁源的磁矩矢量的单位向量的方法包括:根据全张量不变量

Figure BDA00019543557100001115
及两选定测点对应的全张量磁梯度矩阵特征值判断静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的距离远近,从而确定静止状态下所述待定位磁源的磁矩矢量的单位向量。本实施例通过全张量不变量
Figure BDA0001954355710000121
及两选定测点对应的全张量磁梯度矩阵特征值得到两选定测点对应的MT值,并根据MT值越大,所述待定位磁源距离该选定测点的所述全张量磁梯度测量组件的距离越近,以去除另一虚解,从而确定静止状态下所述待定位磁源的磁矩矢量的单位向量。如图4所示,根据全张量不变量
Figure BDA0001954355710000122
及两选定测点对应的全张量磁梯度矩阵特征值可知待定位磁源到选定测点B1的距离小于待定位磁源到选定测点B2的距离,即待定位磁源距离选定测点B1更近,从而将所述待定位磁源锁定在第三象限(即确定所述待定位磁源的磁矩矢量的单位向量)。Wherein, the method for determining the unit vector of the magnetic moment vector of the magnetic source to be positioned in the static state includes: according to the full tensor invariant
Figure BDA00019543557100001115
and the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points to judge the distance from the magnetic source to be positioned to the full tensor magnetic gradient measuring components of the two selected measuring points in the static state, thereby determining the static state The unit vector of the magnetic moment vector of the magnetic source to be located described below. This embodiment adopts the full tensor invariant
Figure BDA0001954355710000121
and the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points to obtain the MT values corresponding to the two selected measuring points, and according to the larger the MT value, the distance between the magnetic source to be positioned and the full tensor of the selected measuring point The closer the distance of the tensor magnetic gradient measurement component is, the other dummy solution is removed, so as to determine the unit vector of the magnetic moment vector of the magnetic source to be positioned in the static state. As shown in Figure 4, according to the full tensor invariant
Figure BDA0001954355710000122
and the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points, it can be seen that the distance from the magnetic source to be located to the selected measuring point B1 is smaller than the distance from the magnetic source to be located to the selected measuring point B2, that is, the distance to the magnetic source to be located is selected The measurement point B1 is closer, so that the magnetic source to be located is locked in the third quadrant (that is, the unit vector of the magnetic moment vector of the magnetic source to be located is determined).

其中,根据所述待定位磁源的磁矩矢量的单位向量获取所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量方法包括:根据所述待定位磁源的磁矩矢量的单位向量,从四个组合中选出唯一一组组合,从而得到所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量。Wherein, according to the unit vector of the magnetic moment vector of the magnetic source to be located, the method of obtaining the unit vector of the position vector of the full tensor magnetic gradient measurement assembly from the magnetic source to be located to two selected measuring points includes: according to the Describe the unit vector of the magnetic moment vector of the magnetic source to be positioned, and select a unique group of combinations from the four combinations, thereby obtaining the full tensor magnetic gradient measurement assembly from the magnetic source to be positioned to two selected measuring points The unit vector of the position vector.

具体的,所述空间直线模型包括:

Figure BDA0001954355710000123
Figure BDA0001954355710000124
其中,x、y、z是所述待定位磁源的初始位置坐标,Ax、Ay、Az是一选定测点的所述全张量磁梯度测量组件的位置坐标,PA、QA、HA是静止状态下所述待定位磁源到一选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量,Bx、By、Bz是另一选定测点的所述全张量磁梯度测量组件的位置坐标,PB、QB、HB是静止状态下所述待定位磁源到另一选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;即通过求取两条空间直线的交点得到所述待定位磁源的初始位置坐标。当然,也可将多组测点的相应数据代入上述空间直线模型以获取多组空间直线,再通过最小二乘等数值求解方法获得待定位磁源初始位置坐标的最优解。Specifically, the space linear model includes:
Figure BDA0001954355710000123
and
Figure BDA0001954355710000124
Wherein, x, y, z are the initial position coordinates of the magnetic source to be located, A x , A y , A z are the position coordinates of the full tensor magnetic gradient measurement component at a selected measuring point, PA , Q A , H A are the unit vectors of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to a selected measuring point in a static state, and B x , By y , B z are another options The position coordinates of the full tensor magnetic gradient measurement component of the fixed measuring point, P B , Q B , H B are the described full tensor magnetic gradients from the magnetic source to be positioned to another selected measuring point in a static state The unit vector of the position vector of the measurement component; that is, the initial position coordinates of the magnetic source to be positioned are obtained by calculating the intersection of two space straight lines. Of course, the corresponding data of multiple sets of measuring points can also be substituted into the above-mentioned spatial straight line model to obtain multiple sets of spatial straight lines, and then the optimal solution of the initial position coordinates of the magnetic source to be located can be obtained by numerical solution methods such as least squares.

作为示例,根据全张量不变量建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型的方法包括:根据全张量不变量

Figure BDA0001954355710000125
建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型
Figure BDA0001954355710000126
其中,MT为全张量不变量,MT1为静止状态下的待定位磁源在同一测点的全张量磁梯度测量组件处产生的全张量不变量,MT2为运动状态下的待定位磁源在同一测点的全张量磁梯度测量组件处产生的全张量不变量,λ1、λ2、λ3为全张量磁梯度矩阵的特征值,μ0为真空磁导率,M为待定位磁源的磁矩的模,R为全张量磁梯度测量组件与待定位磁源之间的距离,R1为同一测点处全张量磁梯度测量组件与静止状态下的待定位磁源之间的距离,R2为同一测点处全张量磁梯度测量组件与运动状态下的待定位磁源之间的距离。As an example, the method for establishing the distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located according to the full tensor invariant includes: according to the full tensor invariant
Figure BDA0001954355710000125
Establishing a distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located
Figure BDA0001954355710000126
Among them, MT is the full tensor invariant, MT 1 is the full tensor invariant generated by the magnetic source to be located in the static state at the full tensor magnetic gradient measurement component at the same measuring point, and MT 2 is the undetermined magnetic source in the moving state The full tensor invariant produced by the bit magnetic source at the full tensor magnetic gradient measurement component at the same measuring point, λ 1 , λ 2 , λ 3 are the eigenvalues of the full tensor magnetic gradient matrix, and μ 0 is the vacuum permeability , M is the modulus of the magnetic moment of the magnetic source to be positioned, R is the distance between the full tensor magnetic gradient measurement component and the magnetic source to be positioned, R 1 is the distance between the full tensor magnetic gradient measurement component at the same measuring point and the static state R2 is the distance between the full tensor magnetic gradient measurement component at the same measuring point and the magnetic source to be located in the moving state.

作为示例,获取运动状态下所述待定位磁源的实时位置坐标的方法包括:As an example, the method for obtaining the real-time position coordinates of the magnetic source to be positioned in a moving state includes:

根据运动状态下所述待定位磁源在该选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值获取运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量(即根据待定位磁源的运动连续性,也就是根据静止状态下所述待定位磁源的初始位置坐标可直接确定运动状态下所述待定位磁源所在象限,从而得到运动状态下所述待定位磁源对应的磁矩矢量的单位向量,进而得到运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量);According to the magnetic field gradient value generated at the full tensor magnetic gradient measurement component of the selected measuring point by the magnetic source to be positioned in the moving state, the distance from the magnetic source to be positioned to the selected measuring point in the moving state is obtained. The unit vector of the position vector of the full tensor magnetic gradient measurement assembly (that is, according to the motion continuity of the magnetic source to be positioned, that is, according to the initial position coordinates of the magnetic source to be positioned in the static state can directly determine the motion state. The quadrant where the magnetic source to be positioned is located, thereby obtaining the unit vector of the magnetic moment vector corresponding to the magnetic source to be positioned in the motion state, and then obtaining the full tensor from the magnetic source to be positioned to the selected measuring point in the motion state unit vector of the position vector of the magnetic gradiometric component);

根据所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型、同一选定测点对应的不同状态下的所述磁场梯度值、所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标获取该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离(即根据同一选定测点对应的不同状态下的所述磁场梯度值分别得到静止状态下所述待定位磁源在该选定测点的全张量磁梯度测量组件处产生的全张量不变量MT1及运动状态下所述待定位磁源在该选定测点的全张量磁梯度测量组件处产生的全张量不变量MT2;并根据所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标得到该选定测点的所述全张量磁梯度测量组件与静止状态下所述待定位磁源之间的距离R1;之后将上述数据代入

Figure BDA0001954355710000131
得到该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离R2);According to the distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located, the magnetic field gradient values in different states corresponding to the same selected measuring point, and the initial position of the magnetic source to be located Coordinates and the position coordinates corresponding to the selected measuring point obtain the distance between the full tensor magnetic gradient measurement component of the selected measuring point and the magnetic source to be positioned under the motion state (that is, according to the same selected measuring point corresponding The magnetic field gradient values in different states of different states are respectively obtained from the full tensor invariant MT 1 generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component of the selected measuring point in the static state and the MT in the moving state. The full tensor invariant MT 2 produced by the magnetic source to be positioned at the full tensor magnetic gradient measurement component of the selected measuring point; and according to the initial position coordinates of the magnetic source to be positioned and the corresponding to the selected measuring point The position coordinates obtain the distance R1 between the full tensor magnetic gradient measurement component of the selected measuring point and the magnetic source to be positioned in the static state; then substitute the above data into
Figure BDA0001954355710000131
Obtain the distance R 2 between the full tensor magnetic gradient measurement component of the selected measuring point and the magnetic source to be positioned in the moving state;

根据该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离及运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量获取运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量,从而获取运动状态下所述待定位磁源的实时位置坐标(即将该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离R2乘以运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量即可得到运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量,之后将其在坐标系进行投影即可得到运动状态下所述待定位磁源的实时位置坐标)。According to the distance between the full tensor magnetic gradient measurement component at the selected measuring point and the magnetic source to be positioned in the moving state and the full distance from the magnetic source to be positioned to the selected measuring point in the moving state The unit vector of the position vector of the tensor magnetic gradient measurement component obtains the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the selected measuring point in the motion state, thereby obtaining the position to be determined in the motion state The real-time position coordinates of the bit magnetic source (that is, the distance R between the full tensor magnetic gradient measurement assembly of the selected measuring point and the magnetic source to be positioned under the motion state is multiplied by the magnetic field to be positioned under the motion state. The unit vector of the position vector of the full tensor magnetic gradient measurement component from the source to the selected measuring point can obtain the full tensor magnetic gradient measurement from the magnetic source to be positioned to the selected measuring point in a moving state The position vector of the component, and then project it on the coordinate system to obtain the real-time position coordinates of the magnetic source to be positioned in the motion state).

需要注意的是,基于上述方法,本实施例还可将本次测得的待定位磁源的实时位置坐标作为下次的初始位置坐标,以实现对运动中的待定位磁源进行实时定位,从而得到待定位磁源的运动轨迹。It should be noted that, based on the above method, this embodiment can also use the real-time position coordinates of the magnetic source to be positioned measured this time as the initial position coordinates of the next time, so as to realize real-time positioning of the magnetic source to be positioned in motion, Thus, the trajectory of the magnetic source to be positioned is obtained.

综上所述,本发明的一种磁源的静态定位装置及静态定位方法,利用由安装支架或低温容器、全张量磁梯度测量组件、位置定位器及测控组件构成的静态定位装置先获取磁源在静止状态下的初始位置坐标,之后再获取磁源在运动状态下对应的磁场梯度值,以实现根据距离比值模型获取磁源在运动状态下的实时位置坐标;在获取初始位置坐标时,采集磁源到两选定测点的全张量磁梯度测量组件处的磁场梯度值,并结合与姿态无关的全张量不变量获取磁源到两选定测点的全张量磁梯度测量组件的位置矢量的单位向量,同时去除了虚解,之后再结合两选定测点的位置坐标建立空间直线模型以获取磁源在静止状态下的初始位置坐标。可见,本发明所述静态定位方法无需知道磁源的总场信息,只通过磁源在静止状态下的初始位置坐标、磁源在运动状态下的磁场梯度值及距离比值模型即可实现磁源在运动状态下的高精度实时定位;同时本发明所述静态定位装置及静态定位方法可充分发挥基于超导磁传感器构建的全张量磁梯度测量组件的灵敏度优势,实现远距离高精度实时定位;而且本发明所述静态定位装置及静态定位方法操作简单快速、便于实现,非常适合在磁法定位测量领域中应用。所以,本发明有效克服了现有技术中的种种缺点而具高度产业利用价值。In summary, a static positioning device and a static positioning method for a magnetic source of the present invention use a static positioning device composed of a mounting bracket or a cryogenic container, a full tensor magnetic gradient measurement component, a position locator, and a measurement and control component to first obtain The initial position coordinates of the magnetic source in a stationary state, and then obtain the corresponding magnetic field gradient value of the magnetic source in a moving state, so as to obtain the real-time position coordinates of the magnetic source in a moving state according to the distance ratio model; when obtaining the initial position coordinates , collect the magnetic field gradient value at the full tensor magnetic gradient measurement component from the magnetic source to the two selected measuring points, and combine the attitude-independent full tensor invariant to obtain the full tensor magnetic gradient from the magnetic source to the two selected measuring points Measure the unit vector of the position vector of the component, remove the virtual solution, and then combine the position coordinates of the two selected measuring points to establish a space linear model to obtain the initial position coordinates of the magnetic source in a static state. It can be seen that the static positioning method of the present invention does not need to know the total field information of the magnetic source, only the initial position coordinates of the magnetic source in the static state, the magnetic field gradient value and the distance ratio model of the magnetic source in the moving state can realize the magnetic source positioning. High-precision real-time positioning in a moving state; at the same time, the static positioning device and static positioning method of the present invention can give full play to the sensitivity advantages of the full tensor magnetic gradient measurement component based on the superconducting magnetic sensor, and realize long-distance high-precision real-time positioning ; Moreover, the static positioning device and the static positioning method of the present invention are simple, quick and easy to implement, and are very suitable for application in the field of magnetic positioning measurement. Therefore, the present invention effectively overcomes various shortcomings in the prior art and has high industrial application value.

上述实施例仅例示性说明本发明的原理及其功效,而非用于限制本发明。任何熟悉此技术的人士皆可在不违背本发明的精神及范畴下,对上述实施例进行修饰或改变。因此,举凡所属技术领域中具有通常知识者在未脱离本发明所揭示的精神与技术思想下所完成的一切等效修饰或改变,仍应由本发明的权利要求所涵盖。The above-mentioned embodiments only illustrate the principles and effects of the present invention, but are not intended to limit the present invention. Anyone skilled in the art can modify or change the above-mentioned embodiments without departing from the spirit and scope of the present invention. Therefore, all equivalent modifications or changes made by those skilled in the art without departing from the spirit and technical ideas disclosed in the present invention should still be covered by the claims of the present invention.

Claims (14)

1.一种磁源的静态定位装置,其特征在于,所述静态定位装置包括:1. A kind of static positioning device of magnetic source, it is characterized in that, described static positioning device comprises: 安装支架,用于提供安装平台;The mounting bracket is used to provide a mounting platform; 全张量磁梯度测量组件,设于所述安装支架上,用于测量待定位磁源在所述全张量磁梯度测量组件处产生的磁场梯度值;The full tensor magnetic gradient measurement component is arranged on the installation bracket, and is used to measure the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component; 位置定位器,刚性连接于所述全张量磁梯度测量组件,用于测量所述全张量磁梯度测量组件在地理坐标系下的位置坐标;A position locator, rigidly connected to the full tensor magnetic gradient measurement component, for measuring the position coordinates of the full tensor magnetic gradient measurement component in the geographic coordinate system; 测控组件,电连接于所述全张量磁梯度测量组件及所述位置定位器,用于采集所述磁场梯度值及所述位置坐标,并根据采集的数据对运动状态下的所述待定位磁源进行实时定位;所述磁场梯度值包括静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值,所述位置坐标包括两选定测点的所述全张量磁梯度测量组件的位置坐标;其中,The measurement and control component is electrically connected to the full tensor magnetic gradient measurement component and the position locator, and is used to collect the magnetic field gradient value and the position coordinates, and to locate the to-be-positioned object in a moving state according to the collected data. The magnetic source performs real-time positioning; the magnetic field gradient value includes the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component at two selected measuring points in a static state, and the position coordinates include two The position coordinates of the described full tensor magnetic gradient measurement component of the selected measuring point; Wherein, 获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值的方法包括:直接获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值;或者,获取静止状态下所述待定位磁源在不同测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并对不同测点对应的所述磁场梯度值进行信噪比比较以选出信噪比最优的两个所述磁场梯度值,其中选出的两个所述磁场梯度值对应的测点作为所述选定测点;The method for obtaining the magnetic field gradient values generated by the full tensor magnetic gradient measurement components at the two selected measuring points of the magnetic source to be positioned in the static state includes: directly obtaining the magnetic field gradient values of the magnetic source to be positioned in the static state at the two selected points The magnetic field gradient value generated at the full tensor magnetic gradient measurement component at the fixed measurement point; or, obtain the magnetic field generated at the full tensor magnetic gradient measurement component at different measurement points by the magnetic source to be positioned in a static state Gradient value, and compare the signal-to-noise ratio of the magnetic field gradient values corresponding to different measuring points to select the two magnetic field gradient values with the best signal-to-noise ratio, wherein the selected two magnetic field gradient values correspond to The measuring point is used as the selected measuring point; 在所述全张量磁梯度测量组件与所述位置定位器之间不存在空间距离时,获取所述全张量磁梯度测量组件的位置坐标的方法包括:通过所述位置定位器直接获取所述全张量磁梯度测量组件的位置坐标;When there is no spatial distance between the full tensor magnetic gradient measurement component and the position locator, the method for obtaining the position coordinates of the full tensor magnetic gradient measurement component includes: directly acquiring the position coordinates of the full tensor magnetic gradient measurement component through the position locator Describe the positional coordinates of the full tensor magnetic gradient measurement component; 在所述全张量磁梯度测量组件与所述位置定位器之间存在空间距离时,获取所述全张量磁梯度测量组件的位置坐标的方法包括:获取所述位置定位器的位置坐标,并获取所述全张量磁梯度测量组件与所述位置定位器之间的偏移量;基于所述偏移量对所述位置坐标进行修正,以获取所述全张量磁梯度测量组件的位置坐标。When there is a spatial distance between the full tensor magnetic gradient measurement component and the position locator, the method for acquiring the position coordinates of the full tensor magnetic gradient measurement component includes: acquiring the position coordinates of the position locator, And obtain the offset between the full tensor magnetic gradient measurement component and the position locator; modify the position coordinates based on the offset to obtain the full tensor magnetic gradient measurement component Position coordinates. 2.根据权利要求1所述的磁源的静态定位装置,其特征在于,所述全张量磁梯度测量组件包括:至少一个磁强计。2 . The static positioning device for a magnetic source according to claim 1 , wherein the full tensor magnetic gradient measurement component comprises: at least one magnetometer. 3 . 3.根据权利要求1所述的磁源的静态定位装置,其特征在于,所述安装支架包括低温容器,用于为所述全张量磁梯度测量组件提供安装平台,同时为所述全张量磁梯度测量组件提供低温环境。3. The static positioning device of the magnetic source according to claim 1, wherein the installation bracket comprises a cryogenic container for providing an installation platform for the full tensor magnetic gradient measurement assembly, and at the same time for the full tensor magnetic gradient measurement assembly The magnetic gradient measurement component provides a low temperature environment. 4.根据权利要求3所述的磁源的静态定位装置,其特征在于,所述全张量磁梯度测量组件包括:至少一个平面梯度计。4 . The static positioning device for a magnetic source according to claim 3 , wherein the full tensor magnetic gradient measurement component comprises: at least one planar gradiometer. 5.根据权利要求3所述的磁源的静态定位装置,其特征在于,所述低温容器包括低温杜瓦。5. The static positioning device for a magnetic source according to claim 3, wherein the cryogenic container comprises a cryogenic Dewar. 6.根据权利要求1所述的磁源的静态定位装置,其特征在于,所述位置定位器包括:差分GPS接收机或组合惯导。6. The static positioning device for magnetic sources according to claim 1, wherein the position locator comprises: a differential GPS receiver or an integrated inertial navigation system. 7.一种磁源的静态定位方法,其特征在于,所述静态定位方法包括:7. A static positioning method for a magnetic source, characterized in that the static positioning method comprises: 搭建如权利要求1至6任一项所述的静态定位装置;Build the static positioning device as described in any one of claims 1 to 6; 在所述待定位磁源处于静止状态时,获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并获取两选定测点的所述全张量磁梯度测量组件的位置坐标,以实现根据全张量不变量获取静止状态下所述待定位磁源的初始位置坐标;When the magnetic source to be positioned is in a static state, obtain the magnetic field gradient values generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement components at two selected measuring points in the static state, and obtain two selected The position coordinates of the full tensor magnetic gradient measurement component of the measuring point, so as to obtain the initial position coordinates of the magnetic source to be positioned in a static state according to the full tensor invariant; 在所述待定位磁源处于运动状态时,获取运动状态下所述待定位磁源在任一所述选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值;When the magnetic source to be positioned is in a moving state, obtain the magnetic field gradient value generated by the magnetic source to be positioned at the full tensor magnetic gradient measurement component at any one of the selected measuring points in the moving state; 根据全张量不变量建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型,以实现根据同一选定测点对应的不同状态下的所述磁场梯度值、所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标获取运动状态下所述待定位磁源的实时位置坐标;Establishing a distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located according to the full tensor invariant, so as to realize the magnetic field gradient values, The initial position coordinates of the magnetic source to be located and the position coordinates corresponding to the selected measuring point acquire the real-time position coordinates of the magnetic source to be located in a moving state; 其中,获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值的方法包括:直接获取静止状态下所述待定位磁源在两选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值;或者,获取静止状态下所述待定位磁源在不同测点的所述全张量磁梯度测量组件处产生的磁场梯度值,并对不同测点对应的所述磁场梯度值进行信噪比比较以选出信噪比最优的两个所述磁场梯度值,其中选出的两个所述磁场梯度值对应的测点作为所述选定测点;Wherein, the method for acquiring the magnetic field gradient values generated by the full tensor magnetic gradient measurement components at two selected measuring points of the magnetic source to be positioned in the static state includes: directly obtaining the magnetic field gradient value of the magnetic source to be positioned in the static state The magnetic field gradient values generated at the full tensor magnetic gradient measurement components of the two selected measuring points; or, obtaining the magnetic source to be positioned in a static state generated at the full tensor magnetic gradient measurement components of different measuring points The magnetic field gradient value, and compare the signal-to-noise ratio of the magnetic field gradient values corresponding to different measuring points to select the two magnetic field gradient values with the best signal-to-noise ratio, wherein the selected two magnetic field gradient values The corresponding measuring point is used as the selected measuring point; 在所述全张量磁梯度测量组件与所述位置定位器之间不存在空间距离时,获取所述全张量磁梯度测量组件的位置坐标的方法包括:通过所述位置定位器直接获取所述全张量磁梯度测量组件的位置坐标;When there is no spatial distance between the full tensor magnetic gradient measurement component and the position locator, the method for obtaining the position coordinates of the full tensor magnetic gradient measurement component includes: directly acquiring the position coordinates of the full tensor magnetic gradient measurement component through the position locator Describe the positional coordinates of the full tensor magnetic gradient measurement component; 在所述全张量磁梯度测量组件与所述位置定位器之间存在空间距离时,获取所述全张量磁梯度测量组件的位置坐标的方法包括:获取所述位置定位器的位置坐标,并获取所述全张量磁梯度测量组件与所述位置定位器之间的偏移量;基于所述偏移量对所述位置坐标进行修正,以获取所述全张量磁梯度测量组件的位置坐标。When there is a spatial distance between the full tensor magnetic gradient measurement component and the position locator, the method for acquiring the position coordinates of the full tensor magnetic gradient measurement component includes: acquiring the position coordinates of the position locator, And obtain the offset between the full tensor magnetic gradient measurement component and the position locator; modify the position coordinates based on the offset to obtain the full tensor magnetic gradient measurement component Position coordinates. 8.根据权利要求7所述的磁源的静态定位方法,其特征在于,获取所述待定位磁源的初始位置坐标的方法包括:8. The static positioning method of the magnetic source according to claim 7, wherein the method for obtaining the initial position coordinates of the magnetic source to be positioned comprises: 根据两选定测点对应的所述磁场梯度值及全张量不变量获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;Acquire the unit of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in a static state according to the magnetic field gradient values corresponding to the two selected measuring points and the full tensor invariant vector; 根据两选定测点对应的位置坐标及静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量建立空间直线模型,以获取所述待定位磁源的初始位置坐标。According to the position coordinates corresponding to the two selected measuring points and the unit vector of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in a static state, a space linear model is established to obtain the Describe the initial position coordinates of the magnetic source to be located. 9.根据权利要求8所述的磁源的静态定位方法,其特征在于,获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量的方法包括:9. The static location method of magnetic source according to claim 8, is characterized in that, obtains the position vector of the described full tensor magnetic gradient measuring assembly of described magnetic source to be positioned under static state to two selected measuring points Methods for unit vectors include: 根据两选定测点对应的所述磁场梯度值分别获取两选定测点对应的全张量磁梯度矩阵特征值;Obtaining the full tensor magnetic gradient matrix eigenvalues corresponding to the two selected measuring points respectively according to the magnetic field gradient values corresponding to the two selected measuring points; 根据两选定测点对应的全张量磁梯度矩阵特征值分别获取两选定测点对应的全张量磁梯度矩阵最小绝对特征值,并根据两选定测点对应的全张量磁梯度矩阵最小绝对特征值获取一参考方向向量;其中,所述参考方向向量平行于静止状态下所述待定位磁源磁矩的方向向量;According to the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points, the minimum absolute eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points are respectively obtained, and according to the full tensor magnetic gradient matrix corresponding to the two selected measuring points The minimum absolute eigenvalue of the matrix obtains a reference direction vector; wherein, the reference direction vector is parallel to the direction vector of the magnetic moment of the magnetic source to be located in a static state; 根据全张量不变量
Figure FDA0004036231870000031
确定静止状态下所述待定位磁源的磁矩矢量的单位向量,从而获取静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;其中,MT为全张量不变量,λ1、λ2、λ3为全张量磁梯度矩阵特征值,μ0为真空磁导率,M为待定位磁源的磁矩的模,R为全张量磁梯度测量组件与待定位磁源之间的距离。
According to the full tensor invariant
Figure FDA0004036231870000031
Determine the unit vector of the magnetic moment vector of the magnetic source to be positioned in the static state, thereby obtaining the unit of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the two selected measuring points in the static state vector; where, MT is the full tensor invariant, λ 1 , λ 2 , λ 3 are the eigenvalues of the full tensor magnetic gradient matrix, μ 0 is the vacuum permeability, M is the modulus of the magnetic moment of the magnetic source to be positioned, R is the distance between the full tensor magnetic gradient measurement component and the magnetic source to be located.
10.根据权利要求9所述的磁源的静态定位方法,其特征在于,获取所述参考方向向量的方法包括:根据两选定测点对应的全张量磁梯度矩阵最小绝对特征值获取其对应的特征向量,并通过对两所述特征向量求取向量积以获取所述参考方向向量。10. The static location method of the magnetic source according to claim 9, wherein the method for obtaining the reference direction vector comprises: obtaining the minimum absolute eigenvalue of the full tensor magnetic gradient matrix corresponding to the two selected measuring points. corresponding eigenvectors, and obtain the reference direction vector by calculating the vector product of the two eigenvectors. 11.根据权利要求9所述的磁源的静态定位方法,其特征在于,确定静止状态下所述待定位磁源的磁矩矢量的单位向量的方法包括:根据全张量不变量
Figure FDA0004036231870000041
及两选定测点对应的全张量磁梯度矩阵特征值判断静止状态下所述待定位磁源到两选定测点的所述全张量磁梯度测量组件的距离远近,从而确定静止状态下所述待定位磁源的磁矩矢量的单位向量。
11. The static location method of magnetic source according to claim 9, it is characterized in that, the method for determining the unit vector of the magnetic moment vector of the magnetic source to be positioned under the static state comprises: according to the full tensor invariant
Figure FDA0004036231870000041
and the eigenvalues of the full tensor magnetic gradient matrix corresponding to the two selected measuring points to judge the distance from the magnetic source to be positioned to the full tensor magnetic gradient measuring components of the two selected measuring points in the static state, thereby determining the static state The unit vector of the magnetic moment vector of the magnetic source to be located described below.
12.根据权利要求8所述的磁源的静态定位方法,其特征在于,所述空间直线模型包括:
Figure FDA0004036231870000042
其中,x、y、z是所述待定位磁源的初始位置坐标,Ax、Ay、Az是一选定测点的所述全张量磁梯度测量组件的位置坐标,PA、QA、HA是静止状态下所述待定位磁源到一选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量,Bx、By、Bz是另一选定测点的所述全张量磁梯度测量组件的位置坐标,PB、QB、HB是静止状态下所述待定位磁源到另一选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量。
12. The static positioning method of the magnetic source according to claim 8, wherein the space linear model comprises:
Figure FDA0004036231870000042
Wherein, x, y, z are the initial position coordinates of the magnetic source to be located, A x , A y , A z are the position coordinates of the full tensor magnetic gradient measurement component at a selected measuring point, PA , Q A , H A are the unit vectors of the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to a selected measuring point in a static state, and B x , By y , B z are another options The position coordinates of the full tensor magnetic gradient measurement component of the fixed measuring point, P B , Q B , H B are the described full tensor magnetic gradients from the magnetic source to be positioned to another selected measuring point in a static state A unit vector that measures the component's position vector.
13.根据权利要求7至12任一项所述的磁源的静态定位方法,其特征在于,根据全张量不变量建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型的方法包括:根据全张量不变量
Figure FDA0004036231870000043
建立所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型
Figure FDA0004036231870000044
其中,MT为全张量不变量,MT1为静止状态下的待定位磁源在同一测点的全张量磁梯度测量组件处产生的全张量不变量,MT2为运动状态下的待定位磁源在同一测点的全张量磁梯度测量组件处产生的全张量不变量,λ1、λ2、λ3为全张量磁梯度矩阵的特征值,μ0为真空磁导率,M为待定位磁源的磁矩的模,R为全张量磁梯度测量组件与待定位磁源之间的距离,R1为同一测点处全张量磁梯度测量组件与静止状态下的待定位磁源之间的距离,R2为同一测点处全张量磁梯度测量组件与运动状态下的待定位磁源之间的距离。
13. The static location method of the magnetic source according to any one of claims 7 to 12, characterized in that, according to the full tensor invariant, the distance between the full tensor magnetic gradient measurement component and the magnetic source to be positioned is established. The method of the distance ratio model consists of: according to the full tensor invariant
Figure FDA0004036231870000043
Establishing a distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located
Figure FDA0004036231870000044
Among them, MT is the full tensor invariant, MT 1 is the full tensor invariant generated by the magnetic source to be located in the static state at the full tensor magnetic gradient measurement component at the same measuring point, and MT 2 is the undetermined magnetic source in the moving state The full tensor invariant produced by the bit magnetic source at the full tensor magnetic gradient measurement component at the same measuring point, λ 1 , λ 2 , λ 3 are the eigenvalues of the full tensor magnetic gradient matrix, and μ 0 is the vacuum permeability , M is the modulus of the magnetic moment of the magnetic source to be positioned, R is the distance between the full tensor magnetic gradient measurement component and the magnetic source to be positioned, R 1 is the distance between the full tensor magnetic gradient measurement component at the same measuring point and the static state R2 is the distance between the full tensor magnetic gradient measurement component at the same measuring point and the magnetic source to be located in the moving state.
14.根据权利要求13所述的磁源的静态定位方法,其特征在于,获取运动状态下所述待定位磁源的实时位置坐标的方法包括:14. The static positioning method of the magnetic source according to claim 13, wherein the method for obtaining the real-time position coordinates of the magnetic source to be positioned in a moving state comprises: 根据运动状态下所述待定位磁源在该选定测点的所述全张量磁梯度测量组件处产生的磁场梯度值获取运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量;According to the magnetic field gradient value generated at the full tensor magnetic gradient measurement component of the selected measuring point by the magnetic source to be positioned in the moving state, the distance from the magnetic source to be positioned to the selected measuring point in the moving state is obtained. The unit vector of the position vector of the full tensor magnetic gradient measurement component; 根据所述全张量磁梯度测量组件与所述待定位磁源之间的距离比值模型、同一选定测点对应的不同状态下的所述磁场梯度值、所述待定位磁源的初始位置坐标及该选定测点对应的位置坐标获取该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离;According to the distance ratio model between the full tensor magnetic gradient measurement component and the magnetic source to be located, the magnetic field gradient values in different states corresponding to the same selected measuring point, and the initial position of the magnetic source to be located The coordinates and the position coordinates corresponding to the selected measuring point obtain the distance between the full tensor magnetic gradient measurement component of the selected measuring point and the magnetic source to be positioned in the motion state; 根据该选定测点的所述全张量磁梯度测量组件与运动状态下所述待定位磁源之间的距离及运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量的单位向量获取运动状态下所述待定位磁源到该选定测点的所述全张量磁梯度测量组件的位置矢量,从而获取运动状态下所述待定位磁源的实时位置坐标。According to the distance between the full tensor magnetic gradient measurement component at the selected measuring point and the magnetic source to be positioned in the moving state and the full distance from the magnetic source to be positioned to the selected measuring point in the moving state The unit vector of the position vector of the tensor magnetic gradient measurement component obtains the position vector of the full tensor magnetic gradient measurement component from the magnetic source to be positioned to the selected measuring point in the motion state, thereby obtaining the position to be determined in the motion state The real-time position coordinates of the bit magnetic source.
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