CN113188566A - Airborne distributed POS data fusion method - Google Patents

Airborne distributed POS data fusion method Download PDF

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CN113188566A
CN113188566A CN202110309944.7A CN202110309944A CN113188566A CN 113188566 A CN113188566 A CN 113188566A CN 202110309944 A CN202110309944 A CN 202110309944A CN 113188566 A CN113188566 A CN 113188566A
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宫晓琳
丁孝双
孙一弘
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Beihang University
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    • G01MEASURING; TESTING
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Abstract

The invention provides an airborne distributed POS data fusion method, which specifically comprises the following steps: calculating redundant position and attitude information of the positions of the child nodes; calculating a measurement vector of the sub-node, and generating a bootstrap measurement set by using a measurement bootstrap strategy; sampling elements of the bootstrap measurement set by using a Metropolis-Hastings sampling criterion to obtain an effective measurement set; calculating the weight and the measurement noise matrix of each effective measurement vector in the effective measurement set; performing data fusion on the child nodes by using sequential filtering, and correcting the motion parameters of the child nodes by using a fusion result; and respectively repeating the steps by other child nodes which do not carry out data fusion. The method utilizes the motion information of all the sub-nodes, reduces the adverse effect of the uncertainty of the measurement noise on the transmission alignment estimation precision, and uses the data fusion result for the correction of the motion parameters, thereby improving the estimation precision of the motion parameters of each sub-node.

Description

Airborne distributed POS data fusion method
Technical Field
The invention relates to the technical field of airborne multi-task remote sensing load node information fusion, in particular to a data fusion method of an airborne distributed Position and attitude measurement System (POS), which can be used for improving the estimation precision of airborne distributed POS sub-node motion parameters.
Background
The Position and Orientation System (POS) is the main means for acquiring Position, velocity and Orientation information of a vehicle. By utilizing the information, the remote sensing data can be corrected, and the imaging quality is improved. Therefore, POS is often applied to the fields of aerial remote sensing imaging, aerial photogrammetry, and the like. For example, remote sensing loads such as a POS assisted Synthetic Aperture Radar (SAR), a laser radar, a multispectral scanner, a digital camera, a large field-of-view infrared scanner, etc. are used to meet the requirement of high precision motion imaging.
With the development of the flight platform technology, one aircraft starts to be provided with a plurality of or a plurality of remote sensing devices to realize synchronous observation of multiple observation windows, and typically, the SAR, the visible light camera, the imaging spectrometer and the laser radar work simultaneously, and the array antenna SAR with a plurality of antennas working simultaneously is provided. Such a multitask remote sensing mode integrating multiple or multiple remote sensing loads has become an important development direction of the aerial remote sensing system. Since a plurality of observation loads are installed at different positions of the carrier, the requirement for measuring the position and posture information of multiple nodes cannot be satisfied by using the conventional single POS. Therefore, in practical use, a plurality of Inertial Measurement Units (IMUs) are installed on the aircraft to form a distributed position and attitude Measurement system, i.e. a distributed POS, so as to realize Measurement of multi-node motion parameters.
The distributed POS is generally composed of one or a small number of high-precision main POS and a plurality of medium/low-precision sub IMUs, wherein the two parts are respectively arranged near remote sensing loads on two sides of a machine body or a wing to form a distributed multi-sensor system. The position of the main POS is called a main node, and the position of each sub IMU is called a sub node.
In order to realize accurate measurement of motion information at each sub-node in the distributed POS, the sub-node needs to correct the result of self strapdown calculation according to the motion information such as high-precision position, speed, attitude and the like provided by the main POS, and the result is used as the final motion parameter of the point, and the process is called transfer alignment. Due to the difference of factors such as body deformation and lever arms at each sub-node, after one-to-one transmission alignment from the main node to each sub-node is completed, the precision of motion parameters at each sub-node is different and has different heights. Particularly, the flexural deformation of the sub-nodes far away from the center of the body is the most complicated, and the transfer alignment accuracy is low. If each subnode can use the motion information of other nodes to perform data fusion, the motion parameter precision of each subnode is further improved.
The current data fusion algorithm for multi-sensor systems can be divided into two types: the first method is centralized fusion, which completes the measurement data of all sensors by one-time fusion calculation, and is proved to be the globally optimal system with the minimum information loss, but for a multi-sensor system such as an airborne distributed POS, multiplication and inversion of a high-dimensional matrix are involved at the time of fusion, and if the fusion method is adopted in the airborne distributed POS, the fusion method has the disadvantages of large calculation load, low real-time performance and low fault tolerance. The second method is distributed fusion, in which the raw data information of multiple sensors is filtered by multiple filters, and then processed by a fusion center. For example, patent No. CN201810153913.5 adopts a distributed fusion method, and the inverse of the covariance matrix obtained by transferring and aligning the sub-IMU is used as the weight matrix for data fusion, and a specific method for fusing position, velocity, and attitude information is provided. However, in the method, the weight matrix with the total number of the subnodes is required to be calculated for data fusion, the calculation of the weight matrix is complex, inversion of the matrix is involved, the problem that the matrix is singular exists, and the total calculation amount is large. Meanwhile, the method does not consider the dependence of flexural motion between the sub-nodes, which also has adverse effect on the precision of the data fusion result.
Common structures used in distributed fusion are federal filtering and sequential filtering. Both distributed fusion architectures are based on kalman filtering. The federal filtering belongs to one of decentralized filtering methods, the structure of the federal filtering comprises a plurality of sub-filters and a main filter, and information distribution between the sub-filters and the main filter is realized by applying an information distribution principle. The federal filtering has the advantages of flexible design and good fault tolerance, and is widely applied to a combined navigation system. However, the federal filtering aims at the fusion of sensor data with complementarity of a plurality of measurement functions installed at a certain point, and each subnode in the airborne distributed POS is only provided with one subimu, so that a common reference system and a plurality of subsystems required by the use of the federal filtering cannot be formed for any subnode, namely, the federal filtering structure cannot be formed, and thus the federal filtering is not suitable for the data fusion of the airborne distributed POS. And the sequential filtering is to sequentially perform Kalman filtering on multiple groups of measurement data, and take the final result as a data fusion result. For airborne distributed POS, the motion parameter information of each sub-node can be converted to any other sub-node by using the deformation data measured by the fiber bragg grating sensor, namely, any sub-node can obtain the redundant motion parameter information converted from the rest sub-nodes to the sub-node, so that a plurality of measurement vectors are formed, the possibility of filtering and estimating the plurality of measurement vectors of each sub-node by adopting sequential filtering is provided, and the sequential filtering has the advantages of smaller calculated amount and simple structure.
Disclosure of Invention
The technical problem to be solved by the invention is as follows: the defects of the prior art are overcome, the airborne distributed POS data fusion method is provided, and the estimation precision of the motion parameters of each sub-node of the airborne distributed POS is improved.
The technical solution of the invention is as follows: an airborne distributed POS data fusion method. The method comprises the following specific steps:
(1) calculating tkRedundant position and attitude information at the time child node;
(2) calculating tkMeasuring vectors of the sub-nodes at the moment, and generating a bootstrap measurement set by using a measurement bootstrap strategy;
(3) sampling elements in the bootstrap measurement set by using a Metropolis-Hastings sampling criterion to obtain an effective measurement set of the child nodes;
(4) calculating the weight and the measurement noise matrix of each effective measurement vector in the effective measurement set;
(5) using sequential filtering to perform data fusion on the child node, and applying the fusion result to the child node tkCorrecting the motion parameters at the moment;
(6) repeating the steps (1) to (5) for other child nodes which are not subjected to data fusion and motion parameter correction until all child nodes finish tkData fusion and correction of motion parameters at the moment;
(7)tk=tk+1and (5) executing the steps (1) to (6) until the data fusion and the correction of the motion parameters of all the child nodes at all the time are completed.
Obtaining t in the step (1)kThe specific steps of the redundant position and attitude information at the time child node are as follows:
1) sub-node strapdown resolving
The definition of the relevant reference coordinate system includes: e is a terrestrial coordinate system; the navigation coordinate systems of the main node and the sub-nodes are northeast geographic coordinate systems, the navigation coordinate system of the main node is represented by n, and the navigation coordinate system and the calculation navigation coordinate system of the J-th sub-node are respectively represented by nJ and n′JJ is 1,2, …, N is the number of child nodes; the origin of the carrier coordinate system is the center of gravity of the carrier, the x-axis is right along the transverse axis of the carrier, the y-axis is forward along the longitudinal axis of the carrier, the z-axis is upward along the vertical axis of the carrier, and the coordinate system is fixed on the carrier and is called as a right-front upper carrier coordinate system, and b is usedm、bJAnd the carrier coordinate systems respectively represent a main node and a J-th sub-node, wherein J is 1,2, … and N.
Each child node is solved through strapdown to obtain tkThe position [ L ] of each timeJ λJ HJ]TAnd attitude [ psiJθJ γJ]TAnd velocity
Figure BDA0002989292310000041
wherein ,LJ、λJ and HJRespectively representing the latitude, longitude and altitude of the J-th sub-node; psiJ、θJ and γJRespectively representing a course angle, a pitch angle and a roll angle of the J-th sub-node;
Figure BDA0002989292310000042
and
Figure BDA0002989292310000043
respectively represent the J-th sub-node at nJEast speed, north speed, and sky speed under the tie.
2) Acquisition of redundant position and attitude information of child nodes
a) Acquisition of child node redundant location information
By mounting on a machineFiber grating sensor on wing, can obtain tkStrain information at any sub-node at any time, and further obtain the displacement of the sub-node from the initial position and relative position information Δ P between any two sub-nodes J, J '(J, J ≠ 1,2, …, N; J ≠ J')J←J′,ΔPJ←J′Representing the difference in latitude, longitude, and altitude between any two child nodes J, J'.
At tkAt the moment, the J-th child node is subjected to strapdown solution to obtain a position [ LJ λJ HJ]TJ-1, 2, …, N, and the other N-1 child nodes are designated as [ LJ′ λJ′ HJ′]T(J '═ 1,2, …, N, J' ≠ J). The redundant location information at the jth child node may be expressed as:
[LJ←J′ λJ←J′ HJ←J′]T=[LJ′ λJ′ HJ′]T+ΔPJ←J′(J,J′=1,2,…,N;J≠J′)
therefore, the J-th sub-node has N calculated values of latitude, longitude and altitude, namely [ L ] in total, in addition to the position information obtained by self strapdown calculationJ λJ HJ]T and [LJ←J′ λJ←J′ HJ←J′]T(J, J '═ 1,2, …, N, J' ≠ J). Position information [ L ] obtained by directly resolving the current child node J in a strapdown mannerJ λJ HJ]TIs newly recorded as
Figure BDA0002989292310000044
Remaining N-1 location information [ LJ←J′ λJ←J′ HJ←J′]T(J, J '═ 1,2, …, N; J ≠ J') is reiterated
Figure BDA0002989292310000045
Figure BDA0002989292310000046
b) Acquisition of child node redundant attitude information
T measured by fiber grating sensorkThe angular displacement information of each sub-node at the moment can construct a conversion matrix between any two sub-nodes J, J '(J, J ≠ 1,2, …, N; J ≠ J') carrier coordinate systems
Figure BDA0002989292310000047
Carrier coordinate system at jth child node (b)JSystem) and the point navigation coordinate system (n)JSystem) as a transformation matrix (attitude matrix) between
Figure BDA0002989292310000051
The attitude matrix at the other N-1 child nodes is represented as
Figure BDA0002989292310000052
The redundant attitude matrix at the jth child node can be represented as:
Figure BDA0002989292310000053
wherein ,
Figure BDA0002989292310000054
at tkAt time, there are N attitude matrices at the J-th child node. Using the N attitude matrices, N attitude angles can be calculated. The specific calculation method of the attitude angle is as follows:
will be provided with
Figure BDA0002989292310000055
Is recorded as:
Figure BDA0002989292310000056
wherein ,TJxyIs a matrix
Figure BDA0002989292310000057
The x-th row and y-th column of the elementElement, x ═ 1,2,3, y ═ 1,2, 3; the attitude angle of the J-th sub-node, including the heading angle psiJAngle of pitch thetaJAnd roll angle γJPrincipal value of, i.e.
Figure BDA0002989292310000058
And
Figure BDA0002989292310000059
respectively as follows:
Figure BDA00029892923100000510
course angle psiJAngle of pitch thetaJAnd roll angle γJAre respectively defined as [0, 2 pi ]]、
Figure BDA00029892923100000511
Figure BDA00029892923100000512
[-π,+π](ii) a Then, ψJ、θJ and γJThe true value of (c) can be determined by:
Figure BDA00029892923100000513
according to the calculation method of the attitude angle, N-1 redundant attitude matrixes at the J-th sub-node can be calculated
Figure BDA00029892923100000514
Corresponding N-1 redundant attitude angles. The attitude matrix of the child node J itself
Figure BDA00029892923100000515
The calculated attitude angle is recorded again
Figure BDA00029892923100000516
From the rest N-1 attitude matrices
Figure BDA0002989292310000061
The attitude angle calculated is recorded as
Figure BDA0002989292310000062
Figure BDA0002989292310000063
Calculating t in the above step (2)kThe method comprises the following specific steps of measuring vectors of the sub-nodes at the moment and generating a bootstrap measurement set by using a measurement bootstrap strategy:
1) calculating a measurement vector for a child node
tkThe latitude, longitude and altitude of the time master node m after lever arm compensation are respectively recorded as Lm、λm、HmThe heading angle, pitch angle and roll angle of the master node m are respectively recorded as psim、θm、γm. T can be obtained for any sub-node J (J ═ 1,2, …, N)kN measured vector of time
Figure BDA0002989292310000064
The expression is as follows:
Figure BDA0002989292310000065
wherein ,
Figure BDA0002989292310000066
respectively represents tkThe ith latitude, longitude and altitude of the time sub-node J are different from the latitude, longitude and altitude of the master node m after lever arm compensation;
Figure BDA0002989292310000067
respectively represents tkAnd the difference value of the ith course angle, the pitch angle and the roll angle of the sub-node J at the moment and the course angle, the pitch angle and the roll angle corresponding to the main node m.
2) Generating a bootstrap measurement set using a measurement bootstrap policy
In the measurement vector
Figure BDA0002989292310000068
Based on the measurement result, the bootstrap measurement is generated by increasing the disturbance
Figure BDA0002989292310000069
The method comprises the following specific steps:
Figure BDA00029892923100000610
wherein ,
Figure BDA00029892923100000611
representing the original measurement vector
Figure BDA00029892923100000612
The c-th bootstrap measurement generated on the basis, c ═ 1,2, …, l, l denote bootstrap measurements
Figure BDA00029892923100000613
L is 5; hJIs a measurement matrix of the system, xJIs the state vector of the system, vJIs measurement noise, and vJWhite Gaussian noise satisfying zero mean with a covariance of
Figure BDA00029892923100000614
Figure BDA00029892923100000615
and vJHaving the same statistical properties, i.e.
Figure BDA00029892923100000616
White Gaussian noise satisfying zero mean, its covariance
Figure BDA00029892923100000617
By the method, NxL bootstrap measurement data can be obtained
Figure BDA00029892923100000618
Defining a bootstrap measurement set:
Figure BDA00029892923100000619
wherein
Figure BDA00029892923100000620
Representing the original measurement vector, i.e.
Figure BDA00029892923100000621
In the step (3), the Metropolis-Hastings sampling criterion is used to sample the elements in the bootstrap measurement set to obtain the effective measurement set of the child node, and the specific steps are as follows:
1) calculating confidence and acceptance probability
From N bootstrap measurements, a set was collected according to Metropolis-Hastings sampling principle
Figure BDA0002989292310000071
In the random selection of two sets
Figure BDA0002989292310000072
Then randomly extracting an element from the two sets
Figure BDA0002989292310000073
And
Figure BDA0002989292310000074
and calculating corresponding credibility
Figure BDA0002989292310000075
And
Figure BDA0002989292310000076
the calculation formula of the reliability is as follows:
Figure BDA0002989292310000077
wherein
Figure BDA00029892923100000720
Is a measure of the mean value of the prediction,
Figure BDA0002989292310000078
representative of the measurement noise vJCovariance matrix
Figure BDA0002989292310000079
Determinant (c).
In obtaining confidence level
Figure BDA00029892923100000710
And
Figure BDA00029892923100000711
on the basis of (1), calculating the acceptance probability according to the following formula:
Figure BDA00029892923100000712
i.e. probability of acceptance
Figure BDA00029892923100000713
Is taken as
Figure BDA00029892923100000714
And a minimum value between 1.
2) Constructing valid metrology collections
Firstly, a random number χ satisfying uniform distribution U (0,1) is generated, and an effective measurement set ΩJThe determination method of (2) is as follows:
Figure BDA00029892923100000715
in the formula, if the elements are randomly extracted
Figure BDA00029892923100000716
And
Figure BDA00029892923100000717
if the corresponding acceptance probability is greater than or equal to the generated random number χ, then it will be
Figure BDA00029892923100000718
As an effective measurement set omegaJThe elements of (1); otherwise, will
Figure BDA00029892923100000719
As an effective measurement set omegaJOf (1). The above process is a sampling process for determining the effective measurement vector.
Repeating the sampling for L times, wherein L is 2N, and L effective measurement vectors in the effective measurement set are respectively defined as zJ(1),zJ(2),…zJ(L) these effective measurement vectors constitute an effective measurement set omegaJ
The specific steps of calculating the weight of each effective measurement vector in the effective measurement set and measuring the noise matrix in the step (4) are as follows:
1) computing a coherence distance and a coherence matrix
Defining an effective metrology set omegaJAny two of the measurement vectors zJ(ξ) and zJThe confidence distance between (ζ) is
Figure BDA0002989292310000081
The calculation method is as follows:
Figure BDA0002989292310000082
calculating a consistency distance based thereon
Figure BDA0002989292310000083
And the consistency matrix ΨJThe calculation method is as follows:
Figure BDA0002989292310000084
wherein ,
Figure BDA0002989292310000085
represents omegaJThe maximum value of the confidence distance between any two measurement vectors.
2) Calculating weights of effective measurement vectors and measurement noise matrix
Obtain the consistency matrix ΨJThen, the maximum module eigenvalue lambda and the corresponding eigenvector beta of the matrix are calculated, and the beta is unitized to obtain
Figure BDA0002989292310000086
Order weight vector
Figure BDA0002989292310000087
At this time, the process of the present invention,
Figure BDA0002989292310000088
can be used to represent the corresponding valid measurement vector is valid measurement set omegaJThe overall degree of support of all elements in.
According to the basic principle of calculating the variance in the mathematical statistics, the measurement noise matrix corresponding to each element in the effective measurement set is calculated
Figure BDA0002989292310000089
The calculation method is as follows:
Figure BDA00029892923100000810
in the step (5), the sequential filtering is used for carrying out data fusion on the child nodes, and the fusion result is used for the child nodes tkThe correction of the moment motion parameters comprises the following specific steps:
1) establishing airborne distributed POS transfer alignment model
The transfer alignment model adopts a matching mode of 'position + attitude', and the system state vector is a 15-dimensional state vector and comprises a platform misalignment angle of a child node J
Figure BDA00029892923100000811
Error in velocity
Figure BDA00029892923100000812
Position error (δ L)J、δλJ、δHJ) Gyro constant drift
Figure BDA00029892923100000813
And adding a constant offset
Figure BDA00029892923100000814
And N is the number of subsystems. Wherein,
Figure BDA00029892923100000815
Figure BDA00029892923100000816
east, north and sky misalignment angles of the J-th child node respectively;
Figure BDA00029892923100000817
respectively, J-th sub-node is at nJEast, north and sky speed errors under the system; delta LJ、δλJ、δHJRespectively a latitude error, a longitude error and an altitude error of the J-th child node;
Figure BDA00029892923100000818
and
Figure BDA0002989292310000091
the sub-IMU at the J-th sub-node is under its carrier coordinate system (b)JSystem) gyro constant drift and add a constant bias;
Figure BDA0002989292310000092
at the J-th child node, respectively, the child IMU is at bJThe gyroscope on the x axis, the y axis and the z axis is subjected to random constant drift;
Figure BDA0002989292310000093
at the J-th child node, respectively, the child IMU is at bJThe accelerometer is constantly biased in the x, y and z axes. The system state vector thus has the form:
Figure BDA0002989292310000094
Figure BDA0002989292310000095
a) establishment of equation of state
The system state equation has the form:
Figure BDA00029892923100000911
wherein the system noise
Figure BDA0002989292310000096
Is zero mean white Gaussian noise, its variance matrix
Figure BDA0002989292310000097
Determined by the noise levels of the gyroscopes and accelerometers in the IMU. FJThe state transition matrix is expressed in the following specific form:
Figure BDA0002989292310000098
wherein ,
Figure BDA0002989292310000099
Figure BDA00029892923100000910
Figure BDA0002989292310000101
Figure BDA0002989292310000102
Figure BDA0002989292310000103
Figure BDA0002989292310000104
wherein ,ωieRepresenting the rotational angular velocity of the earth;
Figure BDA0002989292310000105
and
Figure BDA0002989292310000106
respectively, the sub IMU at the sub-node J in the navigation coordinate system (n)JSystem), northbound, and skyward specific force components;
Figure BDA0002989292310000107
and
Figure BDA0002989292310000108
respectively, the child nodes J in the navigation coordinate system (n)JSystem) east-wise, north-wise and sky-wise speeds;
Figure BDA0002989292310000109
and
Figure BDA00029892923100001010
the main curvature radius of the child node J along the meridian circle and the prime circle is respectively; t is a filtering period; gJThe system noise matrix of the child node J is expressed in the following specific form:
Figure BDA0002989292310000111
b) establishment of measurement equation
L valid measurement vectors z of child node JJA specific expression of (τ) (τ ═ 1,2, …, L) is:
Figure BDA0002989292310000112
wherein ,
Figure BDA0002989292310000113
respectively representing the difference values of the tau-th latitude, longitude and altitude calculation value of the child node J and the latitude, longitude and altitude of the master node m after lever arm compensation;
Figure BDA0002989292310000114
and
Figure BDA0002989292310000115
respectively representing differences of the tau-th course angle, the pitch angle and the roll angle calculated value of the child node J and the course angle, the pitch angle and the roll angle corresponding to the master node m;
the expression of the measurement equation:
Figure BDA0002989292310000116
zJ(τ) corresponding measurement matrix
Figure BDA0002989292310000117
wherein ,
Figure BDA0002989292310000118
Figure BDA0002989292310000119
Taas a master node's attitude matrix, i.e.
Figure BDA00029892923100001110
And order
Figure BDA00029892923100001111
Representation matrix TaThe elements in the s-th row and T-th column, i.e. TaCan be expressed as:
Figure BDA00029892923100001112
2) data fusion using sequential filtering
Firstly, time updating is carried out, and for the J-th child node, the time is updated according to the last time tk-1Filtered estimate of
Figure BDA0002989292310000121
And transferring the alignment model to obtain the current tkOne-step predictive estimate of time of day
Figure BDA0002989292310000122
The calculation formula is as follows:
Figure BDA0002989292310000123
wherein ,ΓJIs to transfer the state of the continuous system to the matrix FJAnd discretizing to obtain a transfer matrix of the discrete system.
In the same way, according to the estimated mean square error array P of the last momentJ(k-1| k-1) and the transfer alignment model may be derived for the current tkThe mean square error matrix is predicted by one step at a moment, and the calculation formula is as follows:
Figure BDA0002989292310000124
wherein ,ΞJIs to drive the noise of the continuous system to the array GJAnd discretizing to obtain a noise driving array of the discrete system.
Then, the effective measurement vector obtained in the step (3) is used for measurement updating, and the J-th sub-node is located at the current tkThe L measured direction at that time are respectively recorded as
Figure BDA0002989292310000125
The data fusion formula of the J-th child node is as follows:
when in use
Figure BDA0002989292310000126
When the measurement is updated, the following steps are carried out:
Figure BDA0002989292310000127
Figure BDA0002989292310000128
Figure BDA0002989292310000129
wherein ,
Figure BDA00029892923100001210
and
Figure BDA00029892923100001211
are respectively as
Figure BDA00029892923100001212
The corresponding measurement matrix and the measurement noise matrix;
Figure BDA00029892923100001213
to use
Figure BDA00029892923100001214
Calculating a filter gain matrix during measurement updating;
Figure BDA00029892923100001215
indicating use of
Figure BDA00029892923100001216
Calculating to obtain a state estimation value during measurement updating;
Figure BDA00029892923100001217
is composed of
Figure BDA00029892923100001218
A corresponding estimated mean square error matrix; i is and
Figure BDA00029892923100001219
unit arrays with the same dimension.
When in use
Figure BDA00029892923100001220
When carrying out measurement update in proper order, have:
Figure BDA00029892923100001221
Figure BDA00029892923100001222
Figure BDA00029892923100001223
wherein ,
Figure BDA0002989292310000131
and
Figure BDA0002989292310000132
are respectively as
Figure BDA0002989292310000133
A corresponding measurement matrix and a measurement noise matrix;
Figure BDA0002989292310000134
to use
Figure BDA0002989292310000135
Calculating a filter gain matrix during measurement updating;
Figure BDA0002989292310000136
indicating use of
Figure BDA0002989292310000137
Calculating to obtain a state estimation value during measurement updating;
Figure BDA0002989292310000138
is composed of
Figure BDA0002989292310000139
And (4) corresponding estimation mean square error matrix.
Executing the data fusion formula, and when the flow runs to the condition that tau is equal to L, obtaining the result
Figure BDA00029892923100001310
As the current tkThe final data fusion result at the J-th child node at time instant, i.e.
Figure BDA00029892923100001311
wherein ,
Figure BDA00029892923100001312
containing tkLatitude error delta L after data fusion of J-th sub-node at momentJ(k) Longitude error δ λJ(k) And height error deltaHJ(k) And also includes n after data fusionJEast-down velocity error under tie
Figure BDA00029892923100001313
Error in north direction velocity
Figure BDA00029892923100001314
And speed error in the sky
Figure BDA00029892923100001315
And east misalignment angle after data fusion
Figure BDA00029892923100001316
Angle of north misalignment
Figure BDA00029892923100001317
And angle of vertical misalignment
Figure BDA00029892923100001318
3) Motion parameter correction
Using the above fusion result to tkAnd correcting the result of the J-th sub-node strapdown calculation at the moment. The calibration procedure is as follows:
a) position correction
LJ(k)|new=LJ(k)-δLJ(k),λJ(k)|new=λJ(k)-δλJ(k),HJ(k)|new=HJ(k)-δHJ(k)
wherein ,LJ(k)、λJ(k)、HJ(k) Respectively represents tkAt the moment, the J-th child node is subjected to strapdown resolving to obtain latitude, longitude and altitude; l isJ(k)|new、λJ(k)|new、HJ(k)|newRespectively represents tkThe corrected latitude, longitude, and altitude of the jth child at time instant.
b) Velocity correction
Figure BDA00029892923100001319
wherein ,
Figure BDA00029892923100001320
respectively represents tkAt the moment, the J-th child node is subjected to strapdown calculation to obtain an east-direction speed, a north-direction speed and a sky-direction speed;
Figure BDA00029892923100001321
respectively represents tkAnd the east-direction speed, the north-direction speed and the sky-direction speed corrected by the J-th sub-node at the moment.
c) Attitude correction
Calculating tkNavigation coordinate system n of J-th sub-node at momentJAnd calculating a navigation coordinate system nJ' conversion matrix between
Figure BDA0002989292310000141
Figure BDA0002989292310000142
Modified transformation matrix
Figure BDA0002989292310000143
Comprises the following steps:
Figure BDA0002989292310000144
wherein ,
Figure BDA0002989292310000145
is tkObtaining an attitude matrix after performing strapdown calculation on J sub-nodes at the moment;
using modified transformation matrices
Figure BDA0002989292310000146
Calculating tkCourse angle psi of sub-node J at timeJ(k)|newAngle of pitch thetaJ(k)|newAnd roll angle γJ(k)|new
Repeating the steps (1) to (5) for other child nodes which are not subjected to data fusion and motion parameter correction in the step (6) until all child nodes finish tkThe method comprises the following specific steps of time data fusion and motion parameter correction:
1) let tkThe child node number of which is k at the moment when the steps (1) to (5) are completedN,kNThe initial value is 1;
2) if k isNN is the number of the child nodes, which indicates that the child nodes still do not finish data fusion and correction of motion parameters, kN=kN+1, pair number kNThe child node repeats steps (1) to (5);
3) if k isNIf N, stop step (6), meaning all child nodes have completed tkAnd (4) data fusion of time and correction of motion parameters.
Compared with the prior art, the invention has the advantages that:
the measurement bootstrap strategy and the sequential filtering are combined around the goal of improving the overall accuracy of airborne distributed POS multi-node motion parameter measurement. In the former method, the motion parameter information of all the child nodes is obtained by obtaining the measurement vector of each child node which is closer to the true value, then the measurement vectors are used for carrying out sequential filtering, and the obtained data fusion result is used for correcting the motion parameters of the child nodes. The method fully utilizes the motion parameter information of all the child nodes, overcomes the adverse effect of the uncertainty of the measurement noise on the transmission alignment estimation precision, and finally improves the estimation precision of the motion parameters of the child nodes.
Drawings
FIG. 1 is a flow chart of the present invention;
fig. 2 is a structural diagram of a data fusion method based on measurement bootstrapping and sequential filtering according to the present invention.
Detailed Description
As shown in FIG. 1, the specific method of the present invention is implemented as follows:
1. calculating tkThe method comprises the following specific steps of calculating redundant position and attitude information at a time sub-node:
(1) sub-node strapdown resolving
The definition of the relevant reference coordinate system includes: e is a terrestrial coordinate system; the navigation coordinate systems of the main node and the sub-nodes are northeast geographic coordinate systems, the navigation coordinate system of the main node is represented by n, and the navigation coordinate system and the calculation navigation coordinate system of the J-th sub-node are respectively represented by nJ and n′JIs represented by the formula J ═1,2, …, N, N is the number of child nodes; the origin of the carrier coordinate system is the center of gravity of the carrier, the x-axis is right along the transverse axis of the carrier, the y-axis is forward along the longitudinal axis of the carrier, the z-axis is upward along the vertical axis of the carrier, and the coordinate system is fixed on the carrier and is called as a right-front upper carrier coordinate system, and b is usedm、bJAnd the carrier coordinate systems respectively represent a main node and a J-th sub-node, wherein J is 1,2, … and N.
Each child node is solved through strapdown to obtain tkThe position [ L ] of each timeJ λJ HJ]TAnd attitude [ psiJθJ γJ]TAnd velocity
Figure BDA0002989292310000151
wherein ,LJ、λJ and HJRespectively representing the latitude, longitude and altitude of the J-th sub-node; psiJ、θJ and γJRespectively representing a course angle, a pitch angle and a roll angle of the J-th sub-node;
Figure BDA0002989292310000152
and
Figure BDA0002989292310000153
respectively represent the J-th sub-node at nJEast speed, north speed, and sky speed under the tie.
(2) Acquisition of redundant position and attitude information of child nodes
a) Acquisition of child node redundant location information
T can be obtained by a fiber grating sensor arranged on the wingkStrain information at any sub-node at any time, and further obtain the displacement of the sub-node from the initial position and relative position information Δ P between any two sub-nodes J, J '(J, J ≠ 1,2, …, N; J ≠ J')J←J′,ΔPJ←J′Representing the difference in latitude, longitude, and altitude between any two child nodes J, J'.
At tkAt the moment, the J-th child node is subjected to strapdown solution to obtain a position [ LJ λJ HJ]TJ-1, 2, …, N, and the other N-1 child nodes are designated as [ LJ′ λJ′ HJ′]T(J '═ 1,2, …, N, J' ≠ J). The redundant location information at the jth child node may be expressed as:
[LJ←J′ λJ←J′ HJ←J′]T=[LJ′ λJ′ HJ′]T+ΔPJ←J′(J,J′=1,2,…,N;J≠J′)
therefore, the J-th sub-node has N calculated values of latitude, longitude and altitude, namely [ L ] in total, in addition to the position information obtained by self strapdown calculationJ λJ HJ]T and [LJ←J′ λJ←J′ HJ←J′]T(J, J '═ 1,2, …, N, J' ≠ J). Position information [ L ] obtained by directly resolving the current child node J in a strapdown mannerJ λJ HJ]TIs newly recorded as
Figure BDA0002989292310000161
Remaining N-1 location information [ LJ←J′ λJ←J′ HJ←J′]T(J, J '═ 1,2, …, N; J ≠ J') is reiterated
Figure BDA0002989292310000162
Figure BDA0002989292310000163
b) Acquisition of child node redundant attitude information
T measured by fiber grating sensorkThe angular displacement information of each sub-node at the moment can construct a conversion matrix between any two sub-nodes J, J '(J, J ≠ 1,2, …, N; J ≠ J') carrier coordinate systems
Figure BDA0002989292310000164
Carrier coordinate system at jth child node (b)JSystem) and the point navigation coordinate system (n)JSystem) as a transformation matrix (attitude matrix) between
Figure BDA0002989292310000165
The attitude matrix at the other N-1 child nodes is represented as
Figure BDA0002989292310000166
The redundant attitude matrix at the jth child node can be represented as:
Figure BDA0002989292310000167
wherein ,
Figure BDA0002989292310000168
at tkAt time, there are N attitude matrices at the J-th child node. By using the N attitude matrices, N attitude information, i.e., N attitude angles, can be calculated. The specific calculation method of the attitude angle is as follows:
will be provided with
Figure BDA0002989292310000169
Is recorded as:
Figure BDA00029892923100001610
wherein ,TJxyIs a matrix
Figure BDA00029892923100001611
The x-th row and the y-th column in the formula (I), wherein x is 1,2,3, and y is 1,2, 3; the attitude angle of the J-th sub-node, including the heading angle psiJAngle of pitch thetaJAnd roll angle γJPrincipal value of, i.e.
Figure BDA00029892923100001612
And
Figure BDA00029892923100001613
respectively as follows:
Figure BDA0002989292310000171
Figure BDA0002989292310000172
Figure BDA0002989292310000173
course angle psiJAngle of pitch thetaJAnd roll angle γJAre respectively defined as [0, 2 pi ]]、
Figure BDA0002989292310000174
Figure BDA0002989292310000175
[-π,+π](ii) a Then, ψJ、θJ and γJThe true value of (c) can be determined by:
Figure BDA0002989292310000176
Figure BDA0002989292310000177
Figure BDA0002989292310000178
according to the calculation method of the attitude angle, N-1 redundant attitude matrixes at the J-th sub-node can be calculated
Figure BDA0002989292310000179
Corresponding N-1 redundant attitude angles. The attitude matrix of the child node J itself
Figure BDA00029892923100001710
The calculated attitude angle is recorded again
Figure BDA00029892923100001711
From the rest N-1 attitude matrices
Figure BDA00029892923100001712
The attitude angle calculated is recorded as
Figure BDA00029892923100001713
Figure BDA00029892923100001714
2. Calculating tkMeasuring vectors of the sub-nodes at the moment, and generating a bootstrap measurement set by using a measurement bootstrap strategy, wherein the method specifically comprises the following steps:
(1) calculating a measurement vector for a child node
tkThe latitude, longitude and altitude of the time master node m after lever arm compensation are respectively recorded as Lm、λm、HmThe heading angle, pitch angle and roll angle of the master node m are respectively recorded as psim、θm、γm. T can be obtained for any sub-node J (J ═ 1,2, …, N)kN measured vector of time
Figure BDA00029892923100001715
The expression is as follows:
Figure BDA00029892923100001716
wherein ,
Figure BDA0002989292310000181
respectively represents tkThe ith latitude, longitude and altitude of the time sub-node J are different from the latitude, longitude and altitude of the master node m after lever arm compensation;
Figure BDA0002989292310000182
respectively represents tkAnd the difference value of the ith course angle, the pitch angle and the roll angle of the sub-node J at the moment and the course angle, the pitch angle and the roll angle corresponding to the main node m.
(2) Generating a bootstrap measurement set using a measurement bootstrap policy
In the measurement vector
Figure BDA0002989292310000183
Based on the measurement result, the bootstrap measurement is generated by increasing the disturbance
Figure BDA0002989292310000184
The method comprises the following specific steps:
Figure BDA0002989292310000185
wherein ,
Figure BDA0002989292310000186
representing the original measurement vector
Figure BDA0002989292310000187
The c-th bootstrap measurement generated on the basis, c ═ 1,2, …, l, l denote bootstrap measurements
Figure BDA0002989292310000188
L is 5; hJIs a measurement matrix of the system, xJIs the state vector of the system, vJIs measurement noise, and vJWhite Gaussian noise satisfying zero mean with a covariance of
Figure BDA0002989292310000189
Figure BDA00029892923100001810
and vJHaving the same statistical properties, i.e.
Figure BDA00029892923100001811
White Gaussian noise satisfying zero mean, its covariance
Figure BDA00029892923100001812
By the method, NxL bootstrap measurement data can be obtained
Figure BDA00029892923100001813
Defining a bootstrap measurement set:
Figure BDA00029892923100001814
wherein
Figure BDA00029892923100001815
Representing the original measurement vector, i.e.
Figure BDA00029892923100001816
3. And (3) sampling the elements in the bootstrap measurement set obtained in the step (2) by using a Metropolis-Hastings sampling criterion to obtain an effective measurement set of the child nodes, wherein the specific steps are as follows:
(1) calculating confidence and acceptance probability
From N bootstrap measurements, a set was collected according to Metropolis-Hastings sampling principle
Figure BDA00029892923100001817
In the random selection of two sets
Figure BDA00029892923100001818
Then randomly extracting an element from the two sets
Figure BDA00029892923100001819
And
Figure BDA00029892923100001820
and calculating corresponding credibility
Figure BDA00029892923100001821
And
Figure BDA00029892923100001822
the calculation formula of the reliability is as follows:
Figure BDA00029892923100001823
wherein
Figure BDA0002989292310000191
Is a measure of the mean value of the prediction,
Figure BDA0002989292310000192
representative of the measurement noise vJCovariance matrix
Figure BDA0002989292310000193
Determinant (c).
In obtaining confidence level
Figure BDA0002989292310000194
And
Figure BDA0002989292310000195
on the basis of (1), calculating the acceptance probability according to the following formula:
Figure BDA0002989292310000196
i.e. probability of acceptance
Figure BDA0002989292310000197
Is taken as
Figure BDA0002989292310000198
And a minimum value between 1.
(2) Constructing valid metrology collections
Firstly, a random number χ satisfying uniform distribution U (0,1) is generated, and an effective measurement set ΩJThe determination method of (2) is as follows:
Figure BDA0002989292310000199
in the formula, if the elements are randomly extracted
Figure BDA00029892923100001910
And
Figure BDA00029892923100001911
if the corresponding acceptance probability is greater than or equal to the generated random number χ, then it will be
Figure BDA00029892923100001912
As an effective measurement set omegaJThe elements of (1); otherwise, will
Figure BDA00029892923100001913
As an effective measurement set omegaJOf (1). The above process is a sampling process for determining the effective measurement vector.
Repeating the sampling for L times, wherein L is 2N, and L effective measurement vectors in the effective measurement set are respectively defined as zJ(1),zJ(2),…zJ(L) these effective measurement vectors constitute an effective measurement set omegaJ
4. Aiming at the effective measurement set obtained in the step 3, calculating the weight of each effective measurement vector and a measurement noise matrix, and the specific steps are as follows:
(1) computing a coherence distance and a coherence matrix
Defining an effective metrology set omegaJAny two of the measurement vectors zJ(ξ) and zJThe confidence distance between (ζ) is
Figure BDA00029892923100001914
The calculation method is as follows:
Figure BDA00029892923100001915
calculating a consistency distance based thereon
Figure BDA00029892923100001916
And the consistency matrix ΨJThe calculation method is as follows:
Figure BDA00029892923100001917
Figure BDA0002989292310000201
wherein ,
Figure BDA0002989292310000202
represents omegaJThe maximum value of the confidence distance between any two measurement vectors.
(2) Calculating weights of effective measurement vectors and measurement noise matrix
Obtain the consistency matrix ΨJThen, the maximum module eigenvalue lambda and the corresponding eigenvector beta of the matrix are calculated, and the eigenvector beta is unitized to obtain
Figure BDA0002989292310000203
Order weight vector
Figure BDA0002989292310000204
At this time, the process of the present invention,
Figure BDA0002989292310000205
the effective measurement set omega can be used to represent the corresponding effective measurement vectorJThe overall degree of support of all elements in.
According to the basic principle of calculating the variance in the mathematical statistics, the measurement noise matrix corresponding to each element in the effective measurement set is calculated
Figure BDA0002989292310000206
The calculation method is as follows:
Figure BDA0002989292310000207
Figure BDA0002989292310000208
5. using sequential filtering to perform data fusion on the child node, and applying the fusion result to the child node tkThe correction of the moment motion parameters comprises the following specific steps:
(1) establishing airborne distributed POS transfer alignment model
The transfer alignment model adopts a matching mode of 'position + attitude', and the system state vector is a 15-dimensional state vector and comprises a platform misalignment angle of a child node J
Figure BDA0002989292310000209
Error in velocity
Figure BDA00029892923100002010
Position error (δ L)J、δλJ、δHJ) Gyro constant drift
Figure BDA00029892923100002011
And adding a constant offset
Figure BDA00029892923100002012
And N is the number of subsystems. Wherein,
Figure BDA00029892923100002013
Figure BDA00029892923100002014
east, north and sky misalignment angles of the J-th child node respectively;
Figure BDA00029892923100002015
respectively, J-th sub-node is at nJEast, north and sky speed errors under the system; delta LJ、δλJ、δHJRespectively a latitude error, a longitude error and an altitude error of the J-th child node;
Figure BDA00029892923100002016
and
Figure BDA00029892923100002017
the sub-IMU at the J-th sub-node is under its carrier coordinate system (b)JSystem) gyro constant drift and add a constant bias;
Figure BDA00029892923100002018
at the J-th child node, respectively, the child IMU is at bJThe gyroscope on the x axis, the y axis and the z axis is subjected to random constant drift;
Figure BDA00029892923100002019
at the J-th child node, respectively, the child IMU is at bJThe accelerometer is constantly biased in the x, y and z axes. The system state vector thus has the form:
Figure BDA0002989292310000211
a) establishment of equation of state
The system state equation has the form:
Figure BDA0002989292310000212
wherein the system noise
Figure BDA0002989292310000213
Is zero mean white Gaussian noise, its variance matrix
Figure BDA0002989292310000214
Determined by the noise levels of the gyroscopes and accelerometers in the IMU.
in the formula ,FJThe state transition matrix is expressed in the following specific form:
Figure BDA0002989292310000215
wherein ,
Figure BDA0002989292310000216
Figure BDA0002989292310000217
Figure BDA0002989292310000221
Figure BDA0002989292310000222
Figure BDA0002989292310000223
Figure BDA0002989292310000224
Figure BDA0002989292310000225
Figure BDA0002989292310000226
wherein ,ωieRepresenting the rotational angular velocity of the earth;
Figure BDA0002989292310000231
and
Figure BDA0002989292310000232
respectively, the sub IMU at the sub-node J in the navigation coordinate system (n)JSystem), northbound, and skyward specific force components;
Figure BDA0002989292310000233
and
Figure BDA0002989292310000234
respectively, the child nodes J in the navigation coordinate system (n)JSystem) east-wise, north-wise and sky-wise speeds;
Figure BDA0002989292310000235
and
Figure BDA0002989292310000236
the main curvature radius of the child node J along the meridian circle and the prime circle is respectively; t is the filter period. GJThe system noise matrix of the child node J is expressed in the following specific form:
Figure BDA0002989292310000237
b) establishment of measurement equation
L valid measurement vectors z of child node JJA specific expression of (τ) (τ ═ 1,2, …, L) is:
Figure BDA0002989292310000238
wherein ,
Figure BDA0002989292310000239
respectively representing the difference values of the tau-th latitude, longitude and altitude calculation value of the child node J and the latitude, longitude and altitude of the master node m after lever arm compensation;
Figure BDA00029892923100002310
and
Figure BDA00029892923100002311
respectively representing differences of the tau-th course angle, the pitch angle and the roll angle calculated value of the child node J and the course angle, the pitch angle and the roll angle corresponding to the master node m;
the measurement equation has the following expression form:
Figure BDA00029892923100002312
zJ(τ) corresponding measurement matrix
Figure BDA00029892923100002313
Has the following forms:
Figure BDA00029892923100002314
wherein
Figure BDA00029892923100002315
Figure BDA0002989292310000241
TaAs a master node's attitude matrix, i.e.
Figure BDA0002989292310000242
And order
Figure BDA0002989292310000243
Representation matrix TaThe elements in the s-th row and T-th column, i.e. TaCan be expressed as:
Figure BDA0002989292310000244
because any child node of each child node in the airborne distributed POS can obtain the redundant motion parameter information converted to the position of the other child nodes, the redundant measurement vector can be obtained according to the method in the step 2, and therefore, for the child node J, the measurement vector can be expressed as:
Figure BDA0002989292310000245
measurement vector
Figure BDA0002989292310000246
The corresponding measurement matrix can be expressed as
Figure BDA0002989292310000247
(2) Data fusion using sequential filtering
Firstly, time updating is carried out, and for the J-th child node, the time is updated according to the last time tk-1Filtered estimate of
Figure BDA0002989292310000248
And transferring the alignment model to obtain the current tkOne-step predictive estimate of time of day
Figure BDA0002989292310000249
The calculation formula is as follows:
Figure BDA00029892923100002410
wherein ,ΓJIs to transfer the state of the continuous system to the matrix FJAnd discretizing to obtain a transfer matrix of the discrete system.
In the same way, according to the estimated mean square error array P of the last momentJ(k-1| k-1) and the transfer alignment model may be derived for the current tkThe mean square error matrix is predicted by one step at a moment, and the calculation formula is as follows:
Figure BDA00029892923100002411
wherein ,ΞJIs to drive the array G with continuous system noiseJAnd discretizing to obtain a noise driving array of the discrete system.
Then, the effective measurement vector obtained in the step (3) is used for measurement updating, and the J-th sub-node is located at the current tkThe L measured direction at that time are respectively recorded as
Figure BDA0002989292310000251
The data fusion formula of the J-th child node is as follows:
when in use
Figure BDA0002989292310000252
When the measurement is updated, the following steps are carried out:
Figure BDA0002989292310000253
wherein ,
Figure BDA0002989292310000254
and
Figure BDA0002989292310000255
are respectively as
Figure BDA0002989292310000256
The corresponding measurement matrix and the measurement noise matrix;
Figure BDA0002989292310000257
to use
Figure BDA0002989292310000258
Calculating a filter gain matrix during measurement updating;
Figure BDA0002989292310000259
indicating use of
Figure BDA00029892923100002510
Calculating to obtain a state estimation value during measurement updating;
Figure BDA00029892923100002511
is composed of
Figure BDA00029892923100002512
A corresponding estimated mean square error matrix; i is and
Figure BDA00029892923100002513
unit arrays with the same dimension.
When in use
Figure BDA00029892923100002514
When carrying out measurement update in proper order, have:
Figure BDA00029892923100002515
wherein ,
Figure BDA00029892923100002516
and
Figure BDA00029892923100002517
are respectively as
Figure BDA00029892923100002518
A corresponding measurement matrix and a measurement noise matrix;
Figure BDA00029892923100002519
to use
Figure BDA00029892923100002520
Calculating a filter gain matrix during measurement updating;
Figure BDA00029892923100002521
indicating use of
Figure BDA00029892923100002522
Amount of progressMeasuring a state estimation value obtained by calculation during updating;
Figure BDA00029892923100002523
is composed of
Figure BDA00029892923100002524
And (4) corresponding estimation mean square error matrix.
Executing the data fusion formula, and when the flow runs to the condition that tau is equal to L, obtaining the result
Figure BDA00029892923100002525
As the current tkThe final data fusion result at the J-th child node at time instant, i.e.
Figure BDA00029892923100002526
wherein ,
Figure BDA00029892923100002527
containing tkLatitude error delta L after data fusion of J-th sub-node at momentJ(k) Longitude error δ λJ(k) And height error deltaHJ(k) And also includes n after data fusionJEast-down velocity error under tie
Figure BDA00029892923100002528
Error in north direction velocity
Figure BDA0002989292310000261
And speed error in the sky
Figure BDA0002989292310000262
And east misalignment angle after data fusion
Figure BDA0002989292310000263
Angle of north misalignment
Figure BDA0002989292310000264
And angle of vertical misalignment
Figure BDA0002989292310000265
(3) Motion parameter correction
Using the above fusion result to tkAnd correcting the result of the J-th sub-node strapdown calculation at the moment. The calibration procedure is as follows:
a) position correction
Figure BDA0002989292310000266
wherein ,LJ(k)、λJ(k)、HJ(k) Respectively represents tkAt the moment, the J-th child node is subjected to strapdown resolving to obtain latitude, longitude and altitude; l isJ(k)|new、λJ(k)|new、HJ(k)|newRespectively represents tkThe corrected latitude, longitude, and altitude of the jth child at time instant.
b) Velocity correction
Figure BDA0002989292310000267
wherein ,
Figure BDA0002989292310000268
respectively represents tkAt the moment, the J-th child node is subjected to strapdown calculation to obtain an east-direction speed, a north-direction speed and a sky-direction speed;
Figure BDA0002989292310000269
respectively represents tkAnd the east-direction speed, the north-direction speed and the sky-direction speed corrected by the J-th sub-node at the moment.
c) Attitude correction
Calculating tkNavigation coordinate system n of J-th sub-node at momentJAnd calculating a navigation coordinate system nJ' conversion matrix between
Figure BDA00029892923100002610
Figure BDA0002989292310000271
Modified transformation matrix
Figure BDA0002989292310000272
Comprises the following steps:
Figure BDA0002989292310000273
wherein ,
Figure BDA0002989292310000274
is tkObtaining an attitude matrix after performing strapdown calculation on J sub-nodes at the moment;
using modified transformation matrices
Figure BDA0002989292310000275
Calculating tkCourse angle psi of sub-node J at timeJ(k)|newAngle of pitch thetaJ(k)|newAnd roll angle γJ(k)|new
6. Repeating the steps 1 to 5 for other sub-nodes which are not subjected to data fusion and motion parameter correction until all the sub-nodes finish tkThe method comprises the following specific steps of time data fusion and motion parameter correction:
(1) let tkThe child node number k at which steps 1 to 5 have been completedN,kNIs 1;
(2) if k isNN is the number of the child nodes, which indicates that the child nodes still do not finish data fusion and correction of motion parameters, kN=kN+1, pair number kNThe child node repeats the first 5 steps;
(3) if k isNN, then step 6 is stopped, indicating that all child nodes have completed tkAnd (4) data fusion of time and correction of motion parameters.
7、tk=tk+1Execution of the step1 to 6, until the data fusion and the correction of the motion parameters of all the child nodes at all the time are completed.
Those skilled in the art will appreciate that the invention may be practiced without these specific details. For those skilled in the art, variations can be made in the specific embodiments and applications without departing from the spirit of the invention. In view of the above, the present disclosure should not be construed as limiting the invention.

Claims (8)

1. A data fusion method for an airborne distributed position and attitude measurement system comprises the following specific steps:
1.1 calculating tkRedundant position and attitude information at the time child node;
1.2 calculating tkMeasuring vectors of the sub-nodes at the moment, and generating a bootstrap measurement set by using a measurement bootstrap strategy;
1.3 sampling elements in the bootstrap measurement set by using a Metropolis-Hastings sampling criterion to obtain an effective measurement set of the child nodes;
1.4 calculating the weight and the measurement noise matrix of each effective measurement vector in the effective measurement set;
1.5 data fusion for the child node using sequential filtering, applying the fusion result to the child node tkCorrecting the motion parameters at the moment;
1.6 repeating steps 1.1 to 1.5 for other sub-nodes without data fusion and motion parameter correction until all sub-nodes finish tkData fusion and correction of motion parameters at the moment;
1.7 tk=tk+1and executing the steps 1.1 to 1.6 until the data fusion and the correction of the motion parameters of all the child nodes at all the time are completed.
2. The data fusion method of the airborne distributed position and attitude measurement system according to claim 1, characterized in that: in the step 1.1, t is calculatedkThe specific steps of the redundant position and attitude information at the time child node are as follows:
2.1 child node strapdown resolution
The definition of the relevant reference coordinate system includes: e is a terrestrial coordinate system; the navigation coordinate systems of the main node and the sub-nodes are northeast geographic coordinate systems, the navigation coordinate system of the main node is represented by n, and the navigation coordinate system and the calculation navigation coordinate system of the J-th sub-node are respectively represented by nJ and n′JJ is 1,2, …, N is the number of child nodes; the origin of the carrier coordinate system is the center of gravity of the carrier, the x-axis is right along the transverse axis of the carrier, the y-axis is forward along the longitudinal axis of the carrier, the z-axis is upward along the vertical axis of the carrier, and the coordinate system is fixed on the carrier and is called as a right-front upper carrier coordinate system, and b is usedm、bJA carrier coordinate system representing the main POS and the jth sub-node, J ═ 1,2, …, N;
each child node is solved through strapdown to obtain tkThe position [ L ] of each timeJ λJ HJ]TAttitude [ psiJ θJγJ]TAnd velocity
Figure FDA0002989292300000021
wherein ,LJ、λJ and HJRespectively representing the latitude, longitude and altitude of the J-th sub-node; psiJ、θJ and γJRespectively representing a course angle, a pitch angle and a roll angle of the J-th sub-node;
Figure FDA0002989292300000022
and
Figure FDA0002989292300000023
respectively representing the east speed, the north speed and the sky speed of the J-th child node;
2.2 acquisition of redundant position and attitude information of child nodes
a) Acquisition of child node redundant location information
T can be obtained by a fiber grating sensor arranged on the wingkStrain information of any sub-node at any moment, and further displacement of the strain information relative to the initial position of the strain information and any two sub-nodes JAnd J' relative position information DeltaPJ←J′,ΔPJ←J′Represents the difference in latitude, longitude, and altitude between any two child nodes J, J ', J, J' is 1,2, …, N; j is not equal to J';
at tkAt the moment, the J-th child node is subjected to strapdown solution to obtain a position [ LJ λJ HJ]TJ-1, 2, …, N, and the other N-1 child nodes are designated as [ LJ′ λJ′ HJ′]TJ '═ 1,2, …, N, J' ≠ J; the redundant location information at the jth child node may be expressed as:
[LJ←J′ λJ←J′ HJ←J′]T=[LJ′ λJ′ HJ′]T+ΔPJ←J′(J,J′=1,2,…,N;J≠J′)
therefore, the J-th sub-node has N calculated values of latitude, longitude and altitude, namely [ L ] in total, in addition to the position information obtained by self strapdown calculationJ λJ HJ]T and [LJ←J′ λJ←J′ HJ←J′]TJ, J '═ 1,2, …, N, J' ≠ J; position information [ L ] obtained by directly resolving the current child node J in a strapdown mannerJ λJ HJ]TIs newly recorded as
Figure FDA0002989292300000024
Remaining N-1 location information [ LJ←J′λJ←J′ HJ←J′]TIs newly recorded as
Figure FDA0002989292300000025
b) Acquisition of child node redundant attitude information
T measured by fiber grating sensorkThe angular displacement information of each child node at the moment can construct a conversion matrix between carrier coordinate systems of any two child nodes J, J
Figure FDA0002989292300000031
Carrier coordinate system b at jth sub-nodeJIs calculated with the point and navigates the coordinate system nJThe transformation matrix between the systems is expressed as
Figure FDA0002989292300000032
The transformation matrix is also called an attitude matrix, and the attitude matrices at the other N-1 sub-nodes are expressed as
Figure FDA0002989292300000033
The redundant attitude matrix at the jth child node can be represented as:
Figure FDA0002989292300000034
wherein ,
Figure FDA0002989292300000035
at tkAt the moment, N attitude matrixes exist at the J-th sub-node; by utilizing the N attitude matrixes, N attitude information, namely N attitude angles, can be calculated; the specific calculation method of the attitude angle is as follows:
will be provided with
Figure FDA0002989292300000036
Is recorded as:
Figure FDA0002989292300000037
wherein ,TJxyIs a matrix
Figure FDA0002989292300000038
The x-th row and the y-th column in the formula (I), wherein x is 1,2,3, and y is 1,2, 3; the attitude angle of the J-th sub-node, including the heading angle psiJAngle of pitch thetaJAnd roll angle γJPrincipal value of, i.e.
Figure FDA0002989292300000039
And
Figure FDA00029892923000000310
respectively as follows:
Figure FDA00029892923000000311
course angle psiJAngle of pitch thetaJAnd roll angle γJAre respectively defined as [0, 2 pi ]]、
Figure FDA00029892923000000312
Figure FDA00029892923000000313
[-π,+π](ii) a Then, ψJ、θJ and γJThe true value of (c) can be determined by:
Figure FDA0002989292300000041
according to the calculation method of the attitude angle, N-1 redundant attitude matrixes at the J-th sub-node can be calculated
Figure FDA0002989292300000042
Corresponding N-1 redundant pose information, J ═ 1,2, …, N; j is not equal to J'; the attitude matrix of the child node J itself
Figure FDA0002989292300000043
The calculated attitude angle is recorded again
Figure FDA0002989292300000044
From the rest N-1 attitude matrices
Figure FDA0002989292300000045
The attitude angle calculated is recorded as
Figure FDA0002989292300000046
Figure FDA0002989292300000047
3. The data fusion method of the airborne distributed position and attitude measurement system according to claim 2, characterized in that: in the step 1.2, t is calculatedkThe method comprises the following specific steps of measuring vectors of the sub-nodes at the moment and generating a bootstrap measurement set by using a measurement bootstrap strategy:
3.1 calculating the measurement vector of the child node
tkThe latitude, longitude and altitude of the time master node m after lever arm compensation are respectively recorded as Lm、λm、HmThe heading angle, pitch angle and roll angle of the master node m are respectively recorded as psim、θm、γm(ii) a For any sub-node J, J ═ 1,2, …, N, t can be obtainedkN measured vector at time
Figure FDA0002989292300000048
The expression is as follows:
Figure FDA0002989292300000049
wherein ,
Figure FDA00029892923000000410
respectively represents tkThe ith latitude, longitude and altitude of the time sub-node J are different from the latitude, longitude and altitude of the master node m after lever arm compensation;
Figure FDA00029892923000000411
respectively represents tkThe difference value of the ith course angle, the pitch angle and the roll angle of the sub-node J at the moment and the course angle, the pitch angle and the roll angle corresponding to the main node m;
3.2 generating a bootstrap measurement set by using a measurement bootstrap strategy
In the measurement vector
Figure FDA00029892923000000412
Based on the measurement result, the bootstrap measurement is generated by increasing the disturbance
Figure FDA0002989292300000051
The method comprises the following specific steps:
Figure FDA0002989292300000052
wherein ,
Figure FDA0002989292300000053
representing the original measurement vector
Figure FDA0002989292300000054
The c-th bootstrap measurement generated on the basis, c ═ 1,2, …, l, l denote bootstrap measurements
Figure FDA0002989292300000055
L is 5; hJIs a measurement matrix of the system, xJIs the state vector of the system, vJIs measurement noise, and vJWhite Gaussian noise satisfying zero mean with a covariance of
Figure FDA0002989292300000056
Figure FDA0002989292300000057
and vJHaving the same statistical properties, i.e.
Figure FDA0002989292300000058
White Gaussian noise satisfying zero mean, its covariance
Figure FDA0002989292300000059
By the method, NxL bootstrap measurement data can be obtained
Figure FDA00029892923000000510
Defining a bootstrap measurement set:
Figure FDA00029892923000000511
wherein
Figure FDA00029892923000000512
Representing the original measurement vector, i.e.
Figure FDA00029892923000000513
4. The data fusion method of the airborne distributed position and attitude measurement system according to claim 3, characterized in that: in step 1.3, the Metropolis-Hastings sampling criterion is used to sample elements in the bootstrap measurement set to obtain an effective measurement set of child nodes, and the specific steps are as follows:
4.1 calculate confidence and acceptance probability
From N bootstrap measurements, a set was collected according to Metropolis-Hastings sampling principle
Figure FDA00029892923000000514
In the random selection of two sets
Figure FDA00029892923000000515
Then randomly extracting an element from the two sets
Figure FDA00029892923000000516
And
Figure FDA00029892923000000517
and calculating corresponding credibility
Figure FDA00029892923000000518
And
Figure FDA00029892923000000519
the calculation formula of the reliability is as follows:
Figure FDA00029892923000000520
wherein
Figure FDA00029892923000000521
Is a measure of the mean value of the prediction,
Figure FDA00029892923000000522
representative of the measurement noise vJCovariance matrix
Figure FDA00029892923000000523
Determinant of (4);
in obtaining confidence level
Figure FDA00029892923000000524
And
Figure FDA00029892923000000525
on the basis of (1), calculating the acceptance probability according to the following formula:
Figure FDA0002989292300000061
i.e. probability of acceptance
Figure FDA0002989292300000062
Is taken as
Figure FDA0002989292300000063
And a minimum value between 1;
4.2 building efficient metrology collections
Firstly, a random number χ satisfying uniform distribution U (0,1) is generated, and an effective measurement set ΩJThe determination method of (2) is as follows:
Figure FDA0002989292300000064
in the formula, if the elements are randomly extracted
Figure FDA0002989292300000065
And
Figure FDA0002989292300000066
if the corresponding acceptance probability is greater than or equal to the generated random number χ, then it will be
Figure FDA0002989292300000067
As an effective measurement set omegaJThe elements of (1); otherwise, will
Figure FDA0002989292300000068
As an effective measurement set omegaJThe elements of (1); the above process is a sampling process for determining an effective measurement vector;
repeating the sampling for L times, wherein L is 2N, and L effective measurement vectors in the effective measurement set are respectively defined as zJ(1),zJ(2),…zJ(L) these effective measurement vectors constitute an effective measurement set omegaJ
5. The data fusion method of the airborne distributed position and attitude measurement system according to claim 4, characterized in that: the specific steps of calculating the weight of each effective measurement vector in the effective measurement set and measuring the noise matrix in step 1.4 are as follows:
5.1 calculate the consistency distance and consistency matrix
Defining an effective metrology set omegaJAny two of the measurement vectors zJ(ξ) and zJThe confidence distance between (ζ) is
Figure FDA0002989292300000069
The calculation method is as follows:
Figure FDA00029892923000000610
calculating a consistency distance based thereon
Figure FDA00029892923000000611
And the consistency matrix ΨJThe calculation method is as follows:
Figure FDA0002989292300000071
wherein ,
Figure FDA0002989292300000072
represents omegaJThe maximum value of the confidence distance between any two measurement vectors;
5.2 calculating weights of effective measurement vectors and measurement noise matrix
Obtain the consistency matrix ΨJThen, the maximum module eigenvalue lambda and the corresponding eigenvector beta of the matrix are calculated, and the eigenvector beta is unitized to obtain
Figure FDA0002989292300000073
Order weight vector
Figure FDA0002989292300000074
At this time, the process of the present invention,
Figure FDA0002989292300000075
can be used to represent the corresponding valid measurement vector is valid measurement set omegaJThe overall degree of support of all elements in;
according to the basic principle of calculating the variance in the mathematical statistics, the measurement noise matrix corresponding to each element in the effective measurement set is calculated
Figure FDA0002989292300000076
The calculation method is as follows:
Figure FDA0002989292300000077
6. the data fusion method of the airborne distributed position and attitude measurement system according to claims 1 and 4, characterized in that: in the step 1.5, sequential filtering is used for carrying out data fusion on the child nodes, and the fusion result is used for the child nodes tkThe correction of the moment motion parameters comprises the following specific steps:
6.1 building airborne distributed POS transfer alignment model
The transfer alignment model adopts a matching mode of 'position + attitude', and the system state vector is a 15-dimensional state vector and comprises a platform misalignment angle of a child node J
Figure FDA0002989292300000078
Error in velocity
Figure FDA0002989292300000079
Position error δ LJ、δλJ、δHJConstant drift of gyro
Figure FDA00029892923000000710
And adding a constant offset
Figure FDA00029892923000000711
N is the number of subsystems; wherein,
Figure FDA00029892923000000712
east, north and sky misalignment angles of the J-th child node respectively;
Figure FDA00029892923000000713
respectively, J-th sub-node is at nJEast, north and sky speed errors under the system; delta LJ、δλJ、δHJRespectively a latitude error, a longitude error and an altitude error of the J-th child node;
Figure FDA00029892923000000714
and
Figure FDA0002989292300000081
respectively, the sub IMU at the J-th sub-node is in the carrier coordinate system bJThe gyro constant drift and the addition constant bias are tied down;
Figure FDA0002989292300000082
at the J-th child node, respectively, the child IMU is at bJThe gyroscope on the x axis, the y axis and the z axis is subjected to random constant drift;
Figure FDA0002989292300000083
at the J-th child node, respectively, the child IMU is at bJAccelerometer constant offsets in the x, y and z axes; the system state vector thus has the form:
Figure FDA0002989292300000084
Figure FDA0002989292300000085
Figure FDA0002989292300000086
a) establishment of equation of state
The system state equation has the form:
Figure FDA0002989292300000087
wherein the system noise
Figure FDA0002989292300000088
Is zero mean white Gaussian noise, its variance matrix
Figure FDA0002989292300000089
Determined by the noise levels of the gyroscopes and accelerometers in the IMU;
in the formula ,FJThe state transition matrix is expressed in the following specific form:
Figure FDA00029892923000000810
wherein ,
Figure FDA00029892923000000811
Figure FDA0002989292300000091
Figure FDA0002989292300000092
Figure FDA0002989292300000093
Figure FDA0002989292300000094
Figure FDA0002989292300000095
wherein ,ωieRepresenting the rotational angular velocity of the earth;
Figure FDA0002989292300000096
and
Figure FDA0002989292300000097
respectively, the sub IMU at the sub node J in the navigation coordinate system nJEast, north and sky specific force components in the system;
Figure FDA0002989292300000098
and
Figure FDA0002989292300000099
respectively a child node J in a navigation coordinate system nJAn east-direction speed, a north-direction speed and a sky-direction speed under the system;
Figure FDA0002989292300000101
and
Figure FDA0002989292300000102
the main curvature radius of the child node J along the meridian circle and the prime circle is respectively; t is a filtering period; gJThe system noise matrix of the child node J is expressed in the following specific form:
Figure FDA0002989292300000103
b) establishment of measurement equation
L valid measurement vectors z of child node JJ(τ), τ ═ 1,2, …, and the specific expression for L is:
Figure FDA0002989292300000104
wherein ,
Figure FDA0002989292300000105
respectively representing the difference values of the tau-th latitude, longitude and altitude calculation value of the child node J and the latitude, longitude and altitude of the master node m after lever arm compensation;
Figure FDA0002989292300000106
and
Figure FDA0002989292300000107
respectively representing differences of the tau-th course angle, the pitch angle and the roll angle calculated value of the child node J and the course angle, the pitch angle and the roll angle corresponding to the master node m;
the measurement equation has the following expression form:
Figure FDA0002989292300000108
zJ(τ) corresponding measurement matrix
Figure FDA0002989292300000109
Has the following forms:
Figure FDA00029892923000001010
wherein ,
Figure FDA00029892923000001011
Figure FDA0002989292300000111
Taas a master node's attitude matrix, i.e.
Figure FDA0002989292300000112
And order
Figure FDA0002989292300000113
Representation matrix TaThe elements in the s-th row and T-th column, i.e. TaCan be expressed as:
Figure FDA0002989292300000114
6.2 data fusion Using sequential Filtering
Firstly, time updating is carried out, and for the J-th child node, the time is updated according to the last time tk-1Filtered estimate of
Figure FDA0002989292300000115
And transferring the alignment model to obtain the current tkOne-step predictive estimate of time of day
Figure FDA0002989292300000116
The calculation formula is as follows:
Figure FDA0002989292300000117
wherein ,ΓJIs to transfer the state of the continuous system to the matrix FJObtaining a transfer matrix of a discrete system after discretization;
in the same way, according to the estimated mean square error array P of the last momentJ(k-1| k-1) and the transfer alignment model may be derived for the current tkOne step predictive mean square of timeError matrix, the calculation formula is as follows:
Figure FDA0002989292300000118
wherein ,ΞJIs to drive the noise of the continuous system to the array GJDiscretizing to obtain a noise driving array of a discrete system;
then, the effective measurement vector obtained in the step 1.3 is used for measurement updating, and the J-th sub-node is located at the current tkThe L measured direction at that time are respectively recorded as
Figure FDA0002989292300000121
The data fusion formula of the J-th child node is as follows:
when in use
Figure FDA0002989292300000122
When the measurement is updated, the following steps are carried out:
Figure FDA0002989292300000123
Figure FDA0002989292300000124
Figure FDA0002989292300000125
wherein ,
Figure FDA0002989292300000126
and
Figure FDA0002989292300000127
are respectively as
Figure FDA0002989292300000128
The corresponding measurement matrix and the measurement noise matrix;
Figure FDA0002989292300000129
to use
Figure FDA00029892923000001210
Calculating a filter gain matrix during measurement updating;
Figure FDA00029892923000001211
indicating use of
Figure FDA00029892923000001212
Calculating to obtain a state estimation value during measurement updating; p1 J(k | k) is
Figure FDA00029892923000001213
A corresponding estimated mean square error matrix; i is and
Figure FDA00029892923000001214
unit arrays with the same dimension;
when in use
Figure FDA00029892923000001215
When carrying out measurement update in proper order, have:
Figure FDA00029892923000001216
Figure FDA00029892923000001217
Figure FDA00029892923000001218
wherein ,
Figure FDA00029892923000001219
and
Figure FDA00029892923000001220
are respectively as
Figure FDA00029892923000001221
The corresponding measurement matrix and the measurement noise matrix;
Figure FDA00029892923000001222
to use
Figure FDA00029892923000001223
Calculating a filter gain matrix during measurement updating;
Figure FDA00029892923000001224
indicating use of
Figure FDA00029892923000001225
Calculating to obtain a state estimation value during measurement updating;
Figure FDA00029892923000001226
is composed of
Figure FDA00029892923000001227
A corresponding estimated mean square error matrix;
executing the data fusion formula, and when the flow runs to the condition that tau is equal to L, obtaining the result
Figure FDA00029892923000001228
As the current tkThe final data fusion result at the J-th child node at time instant, i.e.
Figure FDA00029892923000001229
wherein ,
Figure FDA00029892923000001230
containing tkLatitude error delta L after data fusion of J-th sub-node at momentJ(k) Longitude error δ λJ(k) And height error deltaHJ(k) And also includes n after data fusionJEast-down velocity error under tie
Figure FDA00029892923000001231
Error in north direction velocity
Figure FDA0002989292300000131
And speed error in the sky
Figure FDA0002989292300000132
And east misalignment angle after data fusion
Figure FDA0002989292300000133
Angle of north misalignment
Figure FDA0002989292300000134
And angle of vertical misalignment
Figure FDA0002989292300000135
6.3 motion parameter correction
Using the above fusion result to tkAnd correcting the result of the J-th sub-node strapdown calculation at the moment, wherein the correction steps are as follows:
a) position correction
Figure FDA0002989292300000136
wherein ,LJ(k)、λJ(k)、HJ(k) Respectively represents tkThe J-th sub-node at the moment is obtained by the quick-link solutionLatitude, longitude and altitude to; l isJ(k)|new、λJ(k)|new、HJ(k)|newRespectively represents tkLatitude, longitude and altitude after J-th child node correction at the moment;
b) velocity correction
Figure FDA0002989292300000137
wherein ,
Figure FDA0002989292300000138
respectively represents tkAt the moment, the J-th child node is subjected to strapdown calculation to obtain an east-direction speed, a north-direction speed and a sky-direction speed;
Figure FDA0002989292300000139
respectively represents tkThe east speed, the north speed and the sky speed after the J-th sub-node correction at the moment;
c) attitude correction
Calculating tkNavigation coordinate system n of J-th sub-node at momentJAnd calculating a navigation coordinate system nJ' conversion matrix between
Figure FDA00029892923000001310
Figure FDA0002989292300000141
Modified transformation matrix
Figure FDA0002989292300000142
Comprises the following steps:
Figure FDA0002989292300000143
wherein ,
Figure FDA0002989292300000144
is tkPerforming strapdown calculation on the J-th sub-node at the moment to obtain an attitude matrix;
using modified transformation matrices
Figure FDA0002989292300000145
Calculating tkCourse angle psi of sub-node J at timeJ(k)|newAngle of pitch thetaJ(k)|newAnd roll angle γJ(k)|new
7. The data fusion method of the airborne distributed position and attitude measurement system according to claim 1, characterized in that: in the step 1.6, the steps 1.1 to 1.5 are repeated for other child nodes which are not subjected to data fusion and motion parameter correction until all the child nodes finish tkThe method comprises the following steps of time data fusion and motion parameter correction:
7.1 hypothesis tkThe child node number k at which steps 1.1 to 1.5 have been completedN,kNIs 1;
7.2 if kNN is the number of the child nodes, which indicates that the child nodes still do not finish data fusion and correction of motion parameters, kN=kN+1, pair number kNThe child node of (1) repeats steps 1.1 to 1.5;
7.3 if kNN, then step 1.6 is stopped, indicating that all child nodes have completed tkAnd (4) data fusion of time and correction of motion parameters.
8. The data fusion method of the airborne distributed position and attitude measurement system according to claim 1, characterized in that: in the step 1.7, t is enabledk=tk+1And executing the steps 1.1 to 1.6 until the data fusion and the correction of the motion parameters of all the child nodes at all the time are completed.
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