CN114440870A - Nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering - Google Patents

Nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering Download PDF

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CN114440870A
CN114440870A CN202111637776.0A CN202111637776A CN114440870A CN 114440870 A CN114440870 A CN 114440870A CN 202111637776 A CN202111637776 A CN 202111637776A CN 114440870 A CN114440870 A CN 114440870A
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CN114440870B (en
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邓超凡
陈正想
吕冰
伍东凌
孟诚
窦柯
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Yichang Testing Technique Research Institute
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C21/00Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00
    • G01C21/10Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00 by using measurements of speed or acceleration
    • G01C21/12Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00 by using measurements of speed or acceleration executed aboard the object being navigated; Dead reckoning
    • G01C21/16Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00 by using measurements of speed or acceleration executed aboard the object being navigated; Dead reckoning by integrating acceleration or speed, i.e. inertial navigation
    • G01C21/165Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00 by using measurements of speed or acceleration executed aboard the object being navigated; Dead reckoning by integrating acceleration or speed, i.e. inertial navigation combined with non-inertial navigation instruments
    • G01C21/1654Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00 by using measurements of speed or acceleration executed aboard the object being navigated; Dead reckoning by integrating acceleration or speed, i.e. inertial navigation combined with non-inertial navigation instruments with electromagnetic compass
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C1/00Measuring angles
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C21/00Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00
    • G01C21/20Instruments for performing navigational calculations
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Abstract

The invention discloses a nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering, which is used for solving the real-time position of a magnetic interference target by establishing the position of a magnetic interference substance, the magnetic dipole moment of the magnetic interference substance and the linear function of the magnetic field of the magnetic interference substance and compensating the magnetic interference. And then, a self-adaptive particle swarm optimization algorithm is adopted to find out the magnetic dipole moment which enables the relative distance change quantity of the magnetic interference substance and the nine-axis magnetic compass carrier to measure the minimum value, the parameters of the complementary filter are solved through fuzzy control, the frequency characteristics of the triaxial accelerometer and the triaxial gyroscope are fully considered, and the problem of divergence of the calculation result is avoided. And then, solving an attitude angle by adopting a quaternion method to obtain the real-time attitude of the nine-axis magnetic compass.

Description

Nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering
Technical Field
The invention relates to the technical field of navigation, in particular to a method for acquiring the posture of a nine-axis magnetic compass based on self-adaptive complementary filtering.
Background
The nine-axis magnetic compass is composed of a three-axis gyroscope, a three-axis accelerometer, a three-axis magnetic sensor, a single chip microcomputer and corresponding peripheral circuits, and is mainly used for measuring the attitude of a carrier.
Although the attitude angle obtained by integrating the triaxial angular velocity measured by the triaxial gyroscope has high short-time accuracy, errors can be accumulated along with the increase of time due to the defects of low accuracy, large drift and the like of the MEMS gyroscope, while the attitude angle of the carrier measured by the triaxial accelerometer and the triaxial magnetic sensor can not be accumulated along with the increase of time, when the carrier moves, signals of the accelerometer cannot correctly reflect the attitude information of the carrier due to the influence of the motion acceleration.
Disclosure of Invention
In view of the above, the invention provides a nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering, which can realize data fusion of a three-axis accelerometer, a three-axis magnetic sensor and a three-axis gyroscope and obtain a high-precision attitude angle through calculation.
The invention adopts the following specific technical scheme:
a nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering comprises the following steps:
establishing a position of a magnetic interference substance, a magnetic dipole moment of the magnetic interference substance and a linear function of an interference magnetic field of the magnetic interference substance;
step two, adopting a self-adaptive particle swarm optimization algorithm, representing the position parameters of the particles by using the positions of the magnetic interference substances, and calculating according to the linear function in the step one to obtain the position parameters of each particle; finding out magnetic dipole moment which enables the relative distance change quantity of the magnetic interference substance and the nine-axis magnetic compass carrier to be the minimum value, and calculating and obtaining an interference magnetic field at the installation position of the nine-axis magnetic compass according to the magnetic dipole moment;
thirdly, compensating the magnetic field measured by the nine-axis magnetic compass by using the interference magnetic field in the second step;
after compensating the magnetic field measured by the nine-axis magnetic compass, acquiring the difference between the modulus of the acceleration vector measured by the three-axis accelerometer of the nine-axis magnetic compass and the modulus of the gravity acceleration as the input of fuzzy control to obtain the proportional parameter of the complementary filter and the integral parameter of the complementary filter;
and fifthly, calculating the real-time attitude quaternion of the nine-axis magnetic compass according to the proportional parameter and the integral parameter in the step four, and calculating the carrier attitude angle of the nine-axis magnetic compass according to the real-time attitude quaternion.
Further, in step one, the linear function is:
Figure BDA0003443005380000021
wherein,
Figure BDA0003443005380000022
indicating the location of the magnetically interfering substance,
Figure BDA0003443005380000023
represents the magnetic dipole moment of a magnetically interfering substance,
Figure BDA0003443005380000024
magnetic field, k, representing a magnetically interfering substance1、k2Is a linear parameter of a linear function.
Further, in the second step, the minimum value of the relative distance variation between the magnetic interfering substance and the nine-axis magnetic compass carrier is determined by:
Figure BDA0003443005380000025
wherein,
Figure BDA0003443005380000026
k denotes the time sequence of a nine-axis magnetic compass,
Figure BDA0003443005380000027
indicating the position of the magnetic interference target relative to the nine-axis magnetic compass vehicle at different times,
Figure BDA0003443005380000028
represents the three-axis magnetic field measured by the magnetic sensor of the nine-axis magnetic compass at different moments,
Figure BDA0003443005380000029
denotes the magnetic dipole moment, min [ of a magnetic interfering substance]Representing a minimum function.
Further, in step two, the interference magnetic field at the installation position of the nine-axis magnetic compass obtained by calculation according to the magnetic dipole moment is:
Figure BDA00034430053800000210
wherein,
Figure BDA00034430053800000211
which is indicative of a disturbing magnetic field,
Figure BDA00034430053800000212
indicating the position of the magnetic interference target relative to a nine-axis magnetic compass vehicle,
Figure BDA0003443005380000031
represents the magnetic dipole moment of a magnetically interfering substance,
Figure BDA0003443005380000032
to represent
Figure BDA0003443005380000033
The unit vector of (2).
Further, in the third step, the magnetic field measured by the nine-axis magnetic compass is compensated as follows: and the magnetic field measured by the nine-axis magnetic compass is used for subtracting the interference magnetic field, so that the compensation of the magnetic field measured by the nine-axis magnetic compass is realized.
Further, in the fifth step, the real-time attitude quaternion of the nine-axis magnetic compass calculated according to the proportional parameter and the integral parameter in the fourth step is as follows: firstly, calculating system compensation quantity of the nine-axis magnetic compass according to the proportional parameter and the integral parameter, then calculating to obtain a differential representation form of an attitude quaternion according to the system compensation quantity, and then calculating to obtain the real-time attitude quaternion according to the differential representation form of the attitude quaternion;
the real-time attitude quaternion determination method comprises the following steps:
Figure BDA0003443005380000034
wherein Q iskRepresenting real-time attitude quaternion, Qk-1Representing an attitude quaternion at the k-1 th moment, t representing a time step, and k representing a time sequence of the nine-axis magnetic compass;
Figure BDA0003443005380000035
is Qk-1Is represented in the form of a differential of (c),
Figure BDA0003443005380000036
wherein Q represents a rotational quaternion number,
Figure BDA0003443005380000037
which represents the multiplication of a quaternion by,
Figure BDA0003443005380000038
the output of the gyroscope is represented, and delta represents the system compensation quantity of the nine-axis magnetic compass;
Figure BDA0003443005380000039
wherein KpaccRepresenting the scale parameter, K, of a three-axis accelerometeriaccRepresenting integral parameters of a three-axis accelerometer, eacc(k) A cross product of the value of the acceleration measured by the triaxial accelerometer after the acceleration is normalized and the value of the acceleration obtained by coordinate transformation of the gravitational acceleration, emag(k) Representing the magnetic field value after the three-axis magnetic field normalization and the magnetic field value after the geomagnetic field is subjected to coordinate transformation under a carrier coordinate system measured by a three-axis magnetic sensorCross product, KpmagThe proportional parameter of the triaxial magnetic sensor is represented, and the proportional parameter is a fixed value after magnetic interference compensation; kimagAnd the integral parameters of the three-axis magnetic sensor are represented, and the integral parameters are fixed values after magnetic interference compensation.
Further, in the fifth step, the carrier attitude angle of the nine-axis magnetic compass calculated according to the real-time attitude quaternion is:
Figure BDA0003443005380000041
wherein [ q ]0 q1 q2 q3]k=QkRepresenting real-time attitude quaternion, q0,q1,q2,q3And alpha is a quaternion parameter, alpha represents the heading angle of the nine-axis magnetic compass, beta represents the pitch angle of the nine-axis magnetic compass, and gamma represents the roll angle of the nine-axis magnetic compass.
Further, before the interference magnetic field is compensated, calculating an initial pitch angle value and an initial roll angle value of the nine-axis magnetic compass through triaxial accelerometer data, and calculating an initial heading angle value of the nine-axis magnetic compass through triaxial magnetic sensor data;
and calculating to obtain an attitude angle quaternion under the initial state of the nine-axis magnetic compass according to the initial pitch angle value, the initial roll angle value and the initial course angle value.
Has the advantages that:
(1) a method for acquiring the attitude of a nine-axis magnetic compass based on self-adaptive complementary filtering is characterized in that the real-time position of a magnetic interference target is actually solved by establishing the position of a magnetic interference substance, the magnetic dipole moment of the magnetic interference substance and the linear function of the magnetic field of the magnetic interference substance, and the magnetic interference is compensated, so that the accuracy of the geomagnetic field measured by a three-axis magnetic sensor of the nine-axis magnetic compass is ensured. And a self-adaptive particle swarm optimization algorithm is adopted to find the magnetic dipole moment which enables the relative distance variation of the magnetic interference substance and the nine-axis magnetic compass carrier to measure the minimum value, so that the relative distance variation of the magnetic interference substance and the nine-axis magnetic compass carrier can be ensured to be minimum, and the stability of the system is ensured. The parameters of the complementary filter are solved through fuzzy control, the frequency characteristics of the three-axis accelerometer and the three-axis gyroscope are fully considered, the problem of divergence of a calculation result is avoided, and meanwhile the problems of errors and null shift in the attitude settlement process are avoided. The problem that singularities exist in the traditional method for calculating the attitude angle can be solved by adopting a quaternion method to solve the attitude angle.
(2) The position of the magnetic interference substance, the magnetic dipole moment of the magnetic interference substance and the linear function of the magnetic field of the magnetic interference substance are established, the coplanar and non-collinear property of the magnetic field and the magnetic dipole moment is fully considered, and the real-time position of the magnetic interference substance can be rapidly and efficiently solved.
(3) When the interference magnetic field at the installation position of the nine-axis magnetic compass is calculated according to the position of the magnetic interference substance, the magnetic interference substance is equivalent to a magnetic dipole model, so that the calculation speed of the interference magnetic field is improved, and the calculation amount of the attitude acquisition method of the nine-axis magnetic compass is further reduced.
Drawings
FIG. 1 is a flow chart of the attitude angle calculation of the attitude acquisition method of the nine-axis magnetic compass of the present invention.
FIG. 2 is a flow chart of the complementary filter parameter calculation in the attitude acquisition method of the nine-axis magnetic compass of the present invention.
FIG. 3 is a diagram illustrating the membership function of the difference between the modulus of the acceleration vector measured by the triaxial accelerometer of the nine-axis magnetic compass and the modulus of the gravity acceleration.
Detailed Description
The invention provides a nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering, which is used for solving the real-time position of a magnetic interference target by establishing the position of a magnetic interference substance, the magnetic dipole moment of the magnetic interference substance and the linear function of the magnetic field of the magnetic interference substance and compensating the magnetic interference. And then, a self-adaptive particle swarm optimization algorithm is adopted to find out the magnetic dipole moment which enables the relative distance change quantity of the magnetic interference substance and the nine-axis magnetic compass carrier to measure the minimum value, the parameters of the complementary filter are solved through fuzzy control, the frequency characteristics of the triaxial accelerometer and the triaxial gyroscope are fully considered, and the problem of divergence of the calculation result is avoided. And then, solving the attitude angle by adopting a quaternion method to obtain the real-time attitude of the nine-axis magnetic compass.
The invention is described in detail below by way of example with reference to the accompanying drawings.
Fig. 1 shows a flow chart of the attitude angle calculation of the attitude acquisition method of the nine-axis magnetic compass according to the present invention. A nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering comprises the following steps:
step one, establishing a position of a magnetic interference substance, a magnetic dipole moment of the magnetic interference substance and a linear function of an interference magnetic field of the magnetic interference substance.
The linear function is:
Figure BDA0003443005380000061
wherein,
Figure BDA0003443005380000062
indicating the location of the magnetically interfering substance,
Figure BDA0003443005380000063
represents the magnetic dipole moment of a magnetically interfering substance,
Figure BDA0003443005380000064
magnetic field, k, representing a magnetically interfering substance1、k2Is a linear parameter of a linear function.
Before the interference magnetic field is compensated, the initial pitch angle value and the initial roll angle value of the nine-axis magnetic compass are calculated through the data of the triaxial accelerometer, and the initial heading angle value of the nine-axis magnetic compass is calculated through the data of the triaxial magnetic sensor.
And calculating according to the coordinate transformation relation of the gravity acceleration at the initial moment under the carrier coordinate system and the geographic coordinate system to obtain a pitch angle and a roll angle, calculating by using the pitch angle, the roll angle and the measured triaxial magnetic field data to obtain the horizontal component of the geomagnetic field, and calculating by using an inverse trigonometric function to obtain an azimuth angle. And finally, calculating to obtain the attitude angle quaternion in the initial state through the conversion relation between the attitude angle and the quaternion.
The nine-axis magnetic compass is mainly composed of a three-axis gyroscope, a three-axis magnetic sensor, a three-axis accelerometer and a corresponding data acquisition and processing system, wherein the three-axis gyroscope is used for measuring three-axis direction angular velocity data, the three-axis magnetic sensor is used for measuring three-axis direction magnetic field data, and the three-axis accelerometer is used for measuring three-axis direction acceleration data.
Under the quasi-static condition, the gravity acceleration has no projection component in the horizontal direction in the geographic coordinate system, the accelerometer only has measurement value output in the Z-axis direction, and the measurement value is the earth gravity acceleration g. Then there are:
Figure BDA0003443005380000065
in the formula (1), the first and second groups,
Figure BDA0003443005380000066
for three components of three axes of the gravity acceleration measured by the triaxial accelerometer under a carrier coordinate system, the pitch angle beta and the roll angle gamma can be calculated by unfolding the formula (1):
Figure BDA0003443005380000067
Figure BDA0003443005380000071
the carrier coordinate system is not coincident with the geographic coordinate system. At this time, components of the earth magnetic field in each axis are superposed, and the heading angle α can be solved only by solving the projections of the components of the earth magnetic field measured by the three-axis magnetic sensor in the three axes of the carrier coordinate system.
Figure BDA0003443005380000072
[mx my mz]For three-axis magnetic sensor measurementsThe three-component of the three axes, m, of the geomagnetic field in the carrier coordinate systemx' and myIn the practical application process, the nine-axis magnetic compass is inevitably interfered by various external ferromagnetic substances, and the long-term accuracy of the azimuth angle of the nine-axis magnetic compass is guaranteed by depending on the accurate measurement of the geomagnetic field by the magnetic sensor.
And step two, adopting a self-adaptive particle swarm optimization algorithm to find out the magnetic dipole moment which enables the relative distance change quantity of the magnetic interference substance and the nine-axis magnetic compass carrier to measure the minimum value, and calculating the position of the magnetic interference substance according to the linear function in the step one.
When the nine-axis magnetic compass is arranged on the carrier, the carrier and the magnetic target can be regarded as making relative uniform linear motion in a short time, namely the variation of the relative distance in the same time
Figure BDA0003443005380000073
The same is true.
In the nine-axis magnetic compass, three-axis magnetic fields measured by the magnetic sensors at equal time intervals are sequentially
Figure BDA0003443005380000074
The positions of the interference targets relative to the carrier are respectively obtained according to the measured three-axis magnetic field inversion
Figure BDA0003443005380000075
Solving the target position and magnetic moment can ultimately be translated into a nonlinear optimization problem.
The minimum value of the relative distance variation of the magnetic interference substance and the nine-axis magnetic compass carrier is expressed by the following formula:
Figure BDA0003443005380000076
wherein,
Figure BDA0003443005380000077
k denotes the time sequence of a nine-axis magnetic compass,
Figure BDA0003443005380000081
indicating the position of the magnetic interference target relative to the nine-axis magnetic compass vehicle at different times,
Figure BDA0003443005380000082
represents the three-axis magnetic field measured by the magnetic sensor of the nine-axis magnetic compass at different moments,
Figure BDA0003443005380000083
denotes the magnetic dipole moment, min [ of a magnetic interference substance]Representing a minimum function.
Based on the classical electromagnetic theory, when the position of the detection point and the target is larger than 2.5 times of the maximum size of the target, the magnetic interference substance at one point in the space can be equivalent to a magnetic dipole model, and the magnetic dipole moment is
Figure BDA0003443005380000084
Then at a distance from the magnetically interfering substance
Figure BDA0003443005380000085
The magnetic potential and the magnetic field are respectively as follows:
Figure BDA0003443005380000086
Figure BDA0003443005380000087
as can be seen from the formula, the three vectors are located in the same plane when viewed as three vectors, that is:
Figure BDA0003443005380000088
wherein k is1And k is2The solution method of (2) is as follows:
putting equation (8) into equation (7):
Figure BDA0003443005380000089
due to the fact that
Figure BDA00034430053800000810
And
Figure BDA00034430053800000811
non-collinear, geometric principles can be derived:
Figure BDA00034430053800000812
solving the system of linear equations in equation (10) yields k1And k is2
The method comprises the steps of firstly deducing a calculation method of a target magnetic moment and a target position when the magnetic moment and the magnetic field of a known target are known according to a target magnetic dipole model, assuming that a magnetic target and a carrier do relative linear motion in a short time, so that the variation of relative distance in the same time is equal, converting a target inversion problem into a nonlinear optimization problem, solving the nonlinear optimization problem through a particle swarm optimization algorithm to obtain the target magnetic moment, calculating the relative position of the target, and finally calculating an interference magnetic field generated by the target at the position of the carrier according to the target parameters obtained through calculation to realize magnetic interference compensation.
And step three, calculating an interference magnetic field at the installation position of the nine-axis magnetic compass according to the position of the magnetic interference substance in the step two, and compensating the interference magnetic field.
Calculating the interference magnetic field at the installation position of the nine-axis magnetic compass according to the position of the magnetic interference substance in the step two as follows:
Figure BDA0003443005380000091
wherein,
Figure BDA0003443005380000092
which is indicative of a disturbing magnetic field,
Figure BDA0003443005380000093
indicating the position of the magnetic interference target relative to a nine-axis magnetic compass vehicle,
Figure BDA0003443005380000094
representing the magnetic dipole moment of the magnetically interfering species,
Figure BDA0003443005380000095
to represent
Figure BDA0003443005380000096
The unit vector of (2).
The disturbing magnetic field is compensated as follows: the magnetic field measured by the nine-axis magnetic compass is used for subtracting the interference magnetic field, so that the compensation of the interference magnetic field is realized.
And step four, taking the difference between the modulus of the acceleration vector measured by the triaxial accelerometer of the nine-axis magnetic compass and the modulus of the gravity acceleration as the input of fuzzy control to obtain the proportional parameter of the complementary filter and the integral parameter of the complementary filter.
Firstly, defining a parameter capable of reflecting the motion state of the system, taking the parameter as the input of fuzzy control, then constructing a fuzzy control rule and an input-output membership function, and adjusting the PI parameter of system complementary filtering in real time according to the output of the fuzzy control.
When the attitude quaternion at the initial moment of the known system is output, the attitude quaternion of the system can be solved in real time according to the output of the gyroscope.
The dynamic response of the gyroscope for solving the attitude angle is fast, but accumulated errors, zero drift and the like can be generated in the process of solving the attitude. The magnetic sensor and the accelerometer have no accumulated error, but have poor instantaneous characteristics, and cannot meet the requirement of real-time attitude calculation when the attitude of the carrier is changed violently. Therefore, the advantages of the two can be combined, the high-pass filtering is carried out on the attitude angle measured by the gyroscope by utilizing the complementary filtering principle, the low-pass filtering is carried out on the attitude angle measured by the magnetic sensor and the accelerometer, and finally, a signal which is good in both high-frequency band and low-frequency band is obtained.
According to the definition of the coordinate transformation matrix, the gravity acceleration of the gravity vector of the geographic coordinate system rotating to the carrier coordinate system is as follows:
Figure BDA0003443005380000101
Figure BDA0003443005380000102
the gravity vector of the geographic coordinate system is rotated to a coordinate transformation matrix of the carrier coordinate system.
The acceleration measured by the triaxial accelerometer under the carrier coordinate system is normalized and then recorded as abAcceleration g in a carrier coordinate system obtained by coordinate transformation of the acceleration and the gravitational accelerationbThe error vector in between can be represented by the cross product of these two vectors as:
eacc(k)=gb×ab (12)
this cross product vector is still located in the carrier coordinate system. The gyro integral error is also on the body coordinate system, and the cross product is in direct proportion to the gyro integral error and is just used for correcting the gyro error.
The error vector can likewise be calculated from the magnetic field measurements in the magnetic field carrier coordinate system:
emag(k)=mb×Hb (13)
wherein m isbRepresenting the magnetic field value H under the carrier coordinate system obtained by the coordinate change of the normalized geomagnetic fieldbAnd the value of the normalized triaxial magnetic field measured by the triaxial magnetic sensor in the carrier coordinate system is represented.
The differential equation in equation (13) is solved using the first order Runge-Kutta method:
Figure BDA0003443005380000103
wherein
Figure BDA0003443005380000104
Figure BDA0003443005380000105
It can be seen that the error vector calculated by the accelerometer is subjected to PI operation, and then is subjected to complementary filtering fusion with the output of the gyroscope to obtain the final attitude angle output.
Effect of complementary filter with Kp、KiThe selection of the accelerometer and the gyroscope has a great relationship, if the selection is not proper, the error of attitude estimation is large, and even the problem of divergence of a calculation result occurs, the selection needs to be carried out according to the output frequency characteristics of the accelerometer and the gyroscope. Based on the frequency characteristics of the accelerometer and gyroscopepAnd KiCan be designed according to classical control theory.
The input and output relations of the system in the s domain are as follows:
Figure BDA0003443005380000111
wherein,
Figure BDA0003443005380000112
respectively representing low-pass filter and high-pass filter coefficients, and F1(s)+F2(s) ═ 1 satisfies the complementary filter equation, R1(s) represents the output of the accelerometer and magnetic sensor in the s-domain, R2(s) represents the output of the gyroscope in the s domain,
Figure BDA0003443005380000113
representing the output of the complementary filtering system in the s-domain. It can be seen that the system is a second order system, where Kp=2ξωn
Figure BDA0003443005380000114
Xi is the system damping coefficient, omeganIs the natural vibration angular frequency.
Measured from acceleration when the system is in a state of rest or low-acceleration motionHigh precision of attitude angle, KpaccCan be taken to be larger, whereas K is the case when the system is in a state of high acceleration motionpaccA smaller value is required.
Defining:
Figure BDA0003443005380000115
the difference between the module value representing the acceleration vector and the module value of the gravity acceleration is that err is close to zero when the carrier is static, and the err is larger when the carrier is in a maneuvering state such as acceleration, so that the dynamic condition of the carrier can be reflected.
Using err as input of fuzzy control to detect the maneuvering state of carrier, and output K of self-adaptive modulepaccThe switching frequencies of the low-pass filter and the high-pass filter. It can be seen that err is close to zero when the carrier is at rest, when K is presentpaccTaking the larger value, when the carrier is in low dynamic state, the value of err is smaller, and K is in this casepaccTaking a moderate value, when the carrier is in a high dynamic state, the value of err is larger, and K is in the momentpaccTaking the smaller value. Let the fuzzy set of the fuzzy variable err be { zero, small, large }, the domain of discourse after quantization be { zero, small, big }, the fuzzy set of err be { large, medium, small }, and the domain of discourse after quantization be { big, medium, small }. Adjustment coefficient KpaccThe fuzzy control rule of (1) is as follows:
Figure BDA0003443005380000121
membership functions of err are respectively shown in fig. 3, and a central method is selected as the defuzzification method.
Output coefficient K of fuzzy control modulepaccK can be calculated by combining the damping coefficient xi of the systemiaccThe three-axis magnetic field after magnetic interference compensation is not influenced by external magnetic interference, KpmagAnd KimagThe fixed value can be kept constant.
As can be seen from the above, the parameters of the complementary filter include the scaling parameter KpAnd integral parameter KiIn the present invention, the ratio parameter KpProportional parameter K including a three-axis accelerometerpaccAnd the proportional parameter K of the three-axis magnetic sensorpmag(ii) a Integral parameter KiIntegral parameter K comprising a three-axis accelerometeriaccAnd integral parameter K of three-axis magnetic sensorimag
And step five, calculating the real-time attitude quaternion of the nine-axis magnetic compass according to the proportional parameter and the integral parameter in the step four, and calculating the carrier attitude angle of the nine-axis magnetic compass according to the real-time attitude quaternion.
And calculating the real-time attitude quaternion of the nine-axis magnetic compass according to the proportional parameter and the integral parameter in the step four as follows: calculating system compensation quantity of the nine-axis magnetic compass according to the proportional parameter and the integral parameter, then calculating to obtain a differential representation form of the attitude quaternion according to the system compensation quantity, and then calculating to obtain a real-time attitude quaternion according to the differential representation form of the attitude quaternion;
the real-time attitude quaternion is formulated as:
Figure BDA0003443005380000122
wherein Q iskRepresenting real-time attitude quaternion, Qk-1Representing an attitude quaternion at the k-1 th moment, t representing a time step, and k representing a time sequence of the nine-axis magnetic compass;
Figure BDA0003443005380000123
is Qk-1Is represented in the form of a differential of (c),
Figure BDA0003443005380000124
wherein Q represents a rotational quaternion number,
Figure BDA0003443005380000125
which represents the multiplication of a quaternion,
Figure BDA0003443005380000126
the output of the gyroscope is represented, and delta represents the system compensation quantity of the nine-axis magnetic compass;
Figure BDA0003443005380000131
wherein KpaccRepresenting the scale parameter, K, of a three-axis accelerometeriaccIntegral parameters representing a three-axis accelerometer, eacc(k) A cross product of the value of the acceleration measured by the triaxial accelerometer after the acceleration normalization and the value of the acceleration obtained by the coordinate transformation of the gravitational acceleration, emag(k) Represents the cross product, K, of the magnetic field value measured by the three-axis magnetic sensor and normalized by the three-axis magnetic field in the carrier coordinate system and the magnetic field value after coordinate transformation of the geomagnetic fieldpmagThe proportional parameter of the triaxial magnetic sensor is represented, and the proportional parameter is a fixed value after magnetic interference compensation; kimagAnd the integral parameters of the three-axis magnetic sensor are represented, and the integral parameters are fixed values after magnetic interference compensation.
And calculating the carrier attitude angle of the nine-axis magnetic compass according to the real-time attitude quaternion as follows:
Figure BDA0003443005380000132
wherein [ q ]0 q1 q2 q3]k=QkRepresenting real-time attitude quaternion, q0,q1,q2,q3And alpha is a quaternion parameter, alpha represents the heading angle of the nine-axis magnetic compass, beta represents the pitch angle of the nine-axis magnetic compass, and gamma represents the roll angle of the nine-axis magnetic compass.
Therefore, the attitude angle data of the installed carrier can be obtained by utilizing the three-axis acceleration data, the three-axis angular velocity data and the three-axis magnetic field data of the nine-axis magnetic compass through self-adaptive complementary filtering data fusion.
The above embodiments are merely illustrative of the design principles of the present invention, and the shapes of the components in the description may be different and the names are not limited. Therefore, a person skilled in the art of the present invention can modify or substitute the technical solutions described in the foregoing embodiments; such modifications and substitutions do not depart from the spirit and scope of the present invention.

Claims (8)

1. A nine-axis magnetic compass attitude acquisition method based on adaptive complementary filtering is characterized by comprising the following steps:
establishing a position of a magnetic interference substance, a magnetic dipole moment of the magnetic interference substance and a linear function of an interference magnetic field of the magnetic interference substance;
step two, adopting a self-adaptive particle swarm optimization algorithm, representing the position parameters of the particles by using the positions of the magnetic interference substances, and calculating according to the linear function in the step one to obtain the position parameters of each particle; finding out magnetic dipole moment which enables the relative distance change quantity of the magnetic interference substance and the nine-axis magnetic compass carrier to be the minimum value, and calculating and obtaining an interference magnetic field at the installation position of the nine-axis magnetic compass according to the magnetic dipole moment;
thirdly, compensating the magnetic field measured by the nine-axis magnetic compass by using the interference magnetic field in the second step;
after compensating the magnetic field measured by the nine-axis magnetic compass, acquiring the difference between the modulus of the acceleration vector measured by the three-axis accelerometer of the nine-axis magnetic compass and the modulus of the gravity acceleration as the input of fuzzy control to obtain the proportional parameter of the complementary filter and the integral parameter of the complementary filter;
and fifthly, calculating the real-time attitude quaternion of the nine-axis magnetic compass according to the proportional parameter and the integral parameter in the step four, and calculating the carrier attitude angle of the nine-axis magnetic compass according to the real-time attitude quaternion.
2. The method for obtaining the attitude of a nine-axis magnetic compass according to claim 1, wherein in step one, the linear function is:
Figure RE-FDA0003550525840000011
wherein,
Figure RE-FDA0003550525840000012
indicating the location of the magnetically interfering substance,
Figure RE-FDA0003550525840000013
representing the magnetic dipole moment of the magnetically interfering species,
Figure RE-FDA0003550525840000014
magnetic field, k, representing a magnetically interfering substance1、k2Is a linear parameter of a linear function.
3. The method for obtaining the attitude of a nine-axis magnetic compass according to claim 1, wherein in the second step, the minimum value of the variation of the relative distance between the magnetic interference substance and the nine-axis magnetic compass carrier is determined by:
Figure RE-FDA0003550525840000015
wherein,
Figure RE-FDA0003550525840000016
k denotes the time sequence of a nine-axis magnetic compass,
Figure RE-FDA0003550525840000021
indicating the position of the magnetic interference target relative to the nine-axis magnetic compass vehicle at different times,
Figure RE-FDA0003550525840000022
represents the three-axis magnetic field measured by the magnetic sensor of the nine-axis magnetic compass at different moments,
Figure RE-FDA0003550525840000023
denotes the magnetic dipole moment, min [ of a magnetic interfering substance]Representing a minimum function.
4. The attitude obtaining method of a nine-axis magnetic compass according to claim 1, wherein in step two, the magnetic interference field at the installation position of the nine-axis magnetic compass obtained by the calculation of the magnetic dipole moment is:
Figure RE-FDA0003550525840000024
wherein,
Figure RE-FDA0003550525840000025
which is indicative of a disturbing magnetic field,
Figure RE-FDA0003550525840000026
indicating the position of the magnetic interference target relative to a nine-axis magnetic compass vehicle,
Figure RE-FDA0003550525840000027
represents the magnetic dipole moment of a magnetically interfering substance,
Figure RE-FDA0003550525840000028
to represent
Figure RE-FDA0003550525840000029
The unit vector of (2).
5. The attitude obtaining method of the nine-axis magnetic compass according to claim 1, wherein in step three, the magnetic field measured by the nine-axis magnetic compass is compensated as follows: and the magnetic field measured by the nine-axis magnetic compass is used for subtracting the interference magnetic field, so that the compensation of the magnetic field measured by the nine-axis magnetic compass is realized.
6. The attitude obtaining method of a nine-axis magnetic compass according to claim 1, wherein in the fifth step, the real-time attitude quaternion of the nine-axis magnetic compass calculated according to the proportional parameter and the integral parameter in the fourth step is: firstly, calculating system compensation quantity of the nine-axis magnetic compass according to the proportional parameter and the integral parameter, then calculating to obtain a differential representation form of an attitude quaternion according to the system compensation quantity, and then calculating to obtain the real-time attitude quaternion according to the differential representation form of the attitude quaternion;
the real-time attitude quaternion determination method comprises the following steps:
Figure RE-FDA00035505258400000210
wherein Q iskRepresenting real-time attitude quaternion, Qk-1Representing an attitude quaternion at the k-1 th moment, t representing a time step, and k representing a time sequence of the nine-axis magnetic compass;
Figure RE-FDA00035505258400000211
is Qk-1Is represented in the form of a differential of (c),
Figure RE-FDA00035505258400000212
wherein Q represents a rotational quaternion number,
Figure RE-FDA00035505258400000213
which represents the multiplication of a quaternion by,
Figure RE-FDA00035505258400000214
the output of the gyroscope is represented, and delta represents the system compensation quantity of the nine-axis magnetic compass;
Figure RE-FDA0003550525840000031
wherein KpaccRepresenting the scale parameter, K, of a three-axis accelerometeriaccRepresenting integral parameters of a three-axis accelerometer, eacc(k) A cross product of the value of the acceleration measured by the triaxial accelerometer after the acceleration is normalized and the value of the acceleration obtained by coordinate transformation of the gravitational acceleration, emag(k) Representing the magnetic field value measured by the triaxial magnetic sensor after the triaxial magnetic field normalization and the magnetic field value of the geomagnetic field after coordinate transformation under the carrier coordinate systemCross product of (K)pmagThe proportional parameter of the triaxial magnetic sensor is represented, and the proportional parameter is a fixed value after magnetic interference compensation; kimagAnd the integral parameters of the three-axis magnetic sensor are represented, and the integral parameters are fixed values after magnetic interference compensation.
7. The attitude obtaining method of a nine-axis magnetic compass according to claim 1, wherein in step five, the carrier attitude angle of the nine-axis magnetic compass calculated according to the real-time attitude quaternion is:
Figure RE-FDA0003550525840000032
wherein [ q ]0 q1 q2 q3]k=QkRepresenting real-time attitude quaternion, q0,q1,q2,q3And alpha is a quaternion parameter, alpha represents the heading angle of the nine-axis magnetic compass, beta represents the pitch angle of the nine-axis magnetic compass, and gamma represents the roll angle of the nine-axis magnetic compass.
8. The attitude obtaining method of a nine-axis magnetic compass according to claim 1, wherein the initial pitch angle value and the initial roll angle value of the nine-axis magnetic compass are calculated by three-axis accelerometer data and the initial heading angle value of the nine-axis magnetic compass is calculated by three-axis magnetic sensor data before the compensation of the disturbing magnetic field;
and calculating to obtain an attitude angle quaternion under the initial state of the nine-axis magnetic compass according to the initial pitch angle value, the initial roll angle value and the initial course angle value.
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