CN111121766B - Astronomical and inertial integrated navigation method based on starlight vector - Google Patents

Astronomical and inertial integrated navigation method based on starlight vector Download PDF

Info

Publication number
CN111121766B
CN111121766B CN201911305233.1A CN201911305233A CN111121766B CN 111121766 B CN111121766 B CN 111121766B CN 201911305233 A CN201911305233 A CN 201911305233A CN 111121766 B CN111121766 B CN 111121766B
Authority
CN
China
Prior art keywords
error
inertial
astronomical
navigation
representing
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201911305233.1A
Other languages
Chinese (zh)
Other versions
CN111121766A (en
Inventor
陈庆伟
钱晨
吴益飞
范杰
颜斐
郭健
王潇
舒海洋
魏清华
张宇
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nanjing University of Science and Technology
Original Assignee
Nanjing University of Science and Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nanjing University of Science and Technology filed Critical Nanjing University of Science and Technology
Priority to CN201911305233.1A priority Critical patent/CN111121766B/en
Publication of CN111121766A publication Critical patent/CN111121766A/en
Application granted granted Critical
Publication of CN111121766B publication Critical patent/CN111121766B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • 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
    • 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
    • G01C21/02Navigation; Navigational instruments not provided for in groups G01C1/00 - G01C19/00 by astronomical means
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02TCLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO TRANSPORTATION
    • Y02T90/00Enabling technologies or technologies with a potential or indirect contribution to GHG emissions mitigation

Abstract

The invention discloses an astronomical and inertial integrated navigation method based on a starlight vector, which comprises the steps of establishing an inertial navigation attitude, speed and position updating model; establishing an astronomical and inertial integrated navigation state quantity model; establishing an astronomical and inertial integrated navigation measurement model; a discretized astronomical and inertial integrated navigation state quantity model and a measurement model are used for estimating a position error value, a speed error value and an attitude error value contained in an output value of an inertial navigation update model on line by using Kalman filtering; correcting the position, speed and attitude values according to the estimated values; outputting the gesture, speed and position results obtained by combining astronomical and inertial navigation, judging whether the navigation is finished, and repeating the steps if the navigation is not finished. According to the method, the installation error angle of the astronomical navigation sensor is added into the inertial and astronomical navigation state quantity model, so that the precision of astronomical and inertial integrated navigation is improved.

Description

Astronomical and inertial integrated navigation method based on starlight vector
Technical Field
The invention relates to a combined navigation technology, in particular to an astronomical and inertial combined navigation method based on a starlight vector.
Background
In recent years, along with development and development of high-altitude long-endurance unmanned aerial vehicles, requirements on a navigation system of the high-altitude long-endurance unmanned aerial vehicle are also improved, and the navigation system is required to provide high-precision position values, speed values and attitude values for the high-altitude long-endurance unmanned aerial vehicle all-weather. The unmanned aerial vehicle with high altitude and long endurance mostly uses an inertial and astronomical combined navigation system to provide high-precision position, speed and gesture information for the unmanned aerial vehicle. The traditional astronomical and inertial integrated navigation method needs to perform ground calibration on the installation error angle of the astronomical navigation sensor, the ground calibration value of the installation error angle is used as the true value of the installation error angle of the astronomical navigation sensor to deduce the astronomical and inertial integrated navigation method, but a certain difference still exists between the ground calibration value of the installation error angle and the true value of the installation error angle, which reduces the accuracy of integrated navigation. In addition, the traditional astronomical and inertial integrated navigation method needs that an astronomical navigation sensor at least identifies 3 satellites to correct error values in inertial navigation output position, speed and attitude values, but the astronomical navigation sensor is disturbed by sunlight in the daytime, and the number of the identified satellites cannot guarantee more than 3, so that the precision and reliability of astronomical and inertial integrated navigation are further reduced.
Disclosure of Invention
The invention aims to provide an astronomical and inertial integrated navigation method based on a starlight vector.
The technical solution for realizing the purpose of the invention is as follows: an astronomical and inertial integrated navigation method based on starlight vectors comprises the following steps:
step 1, establishing an inertial navigation attitude, speed and position updating model according to Newton's law of mechanics and Euler theorem of fixed point rotation of a rigid body;
step 2, establishing an astronomical and inertial combined navigation state quantity model according to error characteristics of the inertial navigation sensor and installation error angle characteristics of the astronomical navigation sensor;
step 3, establishing an astronomical and inertial integrated navigation measurement model according to the starlight vector under the inertial coordinate system and the starlight vector under the star-sensitive coordinate system;
step 4, discretizing an astronomical and inertial combined navigation state quantity model and a measurement model, and estimating a position error value, a speed error value and an attitude error value contained in an output value of an inertial navigation updating model on line by using Kalman filtering;
step 5, correcting the position, speed and attitude values obtained in the step 1 according to the estimated value in the step 4;
and 6, outputting the gesture, speed and position results obtained by combining astronomical and inertial navigation, judging whether the navigation is finished, and if not, performing the step 1.
Compared with the prior art, the invention has the remarkable advantages that: 1) The installation error angle of the astronomical navigation sensor is introduced to construct a state model, so that the precision of astronomical and inertial integrated navigation is improved; 2) And a measurement model is constructed by using the starlight vector, so that the combined navigation of astronomy and inertia can be completed under the condition that fewer than 3 stars are identified by the astronomical navigation sensor, and the reliability of the combined navigation of astronomy and inertia is improved.
Drawings
FIG. 1 is a flow chart of an astronomical and inertial integrated navigation method based on starlight vectors.
Fig. 2 is a flight trajectory diagram of an embodiment of the present invention.
FIG. 3 is a graph showing the comparison of the roll angle error results of the method of the present invention and the conventional method.
FIG. 4 is a graph showing the pitch angle error results of the method of the present invention compared to the conventional method.
FIG. 5 is a graph showing the comparison of yaw angle error results of the method of the present invention and the conventional method.
FIG. 6 is a graph showing the comparison of the east speed error results of the method of the present invention and the conventional method.
FIG. 7 is a graph showing the comparison of the north velocity error results of the method of the present invention and the conventional method.
FIG. 8 is a graph showing the comparison of the results of the tangential velocity error in the method of the present invention and the conventional method.
FIG. 9 is a graph showing the comparison of longitude error results of the method of the present invention and the conventional method.
FIG. 10 is a graph showing comparison of latitude error results of the method of the present invention and conventional methods.
FIG. 11 is a comparison of the results of the height error of the method of the present invention and the conventional method.
Detailed Description
The present invention will be further described with reference to the drawings and the specific embodiments.
As shown in fig. 1, the astronomical and inertial integrated navigation method based on the starlight vector comprises the following steps:
step 1, establishing an inertial navigation attitude, speed and position updating model
According to Newton's law of mechanics and Euler's theorem of fixed point rotation of rigid body, the attitude, speed and position updating model of inertial navigation is established under a local geographic coordinate system, namely an east-north-sky coordinate system, as follows:
and (3) updating a model by the gesture:
Figure BDA0002322902400000021
wherein, the liquid crystal display device comprises a liquid crystal display device,
Figure BDA0002322902400000022
posture transformation matrix representing carrier coordinate system to local geographic coordinate system, < >>
Figure BDA0002322902400000023
Representation->
Figure BDA0002322902400000024
Is used for the purpose of determining the derivative of (c),
Figure BDA0002322902400000031
representing the angular velocity of the inertial frame relative to the carrier frame, measured by the inertial navigation sensor gyroscope,
Figure BDA0002322902400000032
the angular velocity of the inertial coordinate system relative to the local geographic coordinate system is represented, x being the inverse of this matrix representation.
And (3) updating a model by speed:
Figure BDA0002322902400000033
wherein v represents the speed of the carrierValues in the form of v= [ v ] E v N v U ] T Respectively representing the east and north speeds and the sky speed of the carrier under a local geographic coordinate system,
Figure BDA0002322902400000034
for v derivative, < >>
Figure BDA0002322902400000035
Posture transformation matrix representing carrier coordinate system to local geographic coordinate system, < >>
Figure BDA0002322902400000036
The specific force value of the carrier in the carrier system is represented and is measured by an inertial navigation sensor accelerometer; />
Figure BDA0002322902400000037
Expressed as the angular velocity of rotation of the earth->
Figure BDA0002322902400000038
Represents the angular velocity, g, of the local geographic coordinate system relative to the geocentric fixed coordinate system n The x represents the inverse of this matrix representation for the gravitational acceleration of the position of the carrier.
A location update model:
Figure BDA00023229024000000313
in the formula (3), r= [ lambda L h ]] T The longitude, latitude and altitude values respectively representing the position of the carrier,
Figure BDA0002322902400000039
represents the derivative of R, R M And R is N The meridian radius and the mortise unitary radius of the position, v E 、v N And v U The east and north and sky speeds in the local geographic coordinate system are represented, respectively.
Step 2, establishing an astronomical and inertial combined navigation state quantity model
Step 1 in formula (1)
Figure BDA00023229024000000310
And +.2 in formula (2)>
Figure BDA00023229024000000311
The method is characterized in that the method is obtained by measuring an inertial navigation sensor gyroscope and an accelerometer, noise exists in measured values of the gyroscope and the accelerometer, error analysis is needed to be carried out on an output result of an inertial navigation updating model, and a state quantity model of astronomical and inertial integrated navigation is established based on the error analysis.
Firstly, establishing a model of gyro noise epsilon and accelerometer noise
Figure BDA00023229024000000312
Model of (2)
Figure BDA0002322902400000041
Wherein ε b And
Figure BDA0002322902400000042
the random constant zero drift representing the gyroscope and the accelerometer is a constant value; epsilon g And->
Figure BDA0002322902400000043
Is white gaussian noise.
Then the triaxial gyroscope error model epsilon x ε y ε z Triaxial accelerometer error model
Figure BDA0002322902400000044
The method comprises the following steps:
Figure BDA0002322902400000045
wherein [ epsilon ] x ε y ε z ] T Respectively representing the total measurement error of the x, y and z axis gyroscopes, [ epsilon ] bx ε by ε bz ] T Representing the random constant zero drift error component of the x, y and z axis gyroscopes [ epsilon ] gx ε gy ε gz ] T Representing gaussian white noise error components of the x-, y-, z-axis gyroscopes,
Figure BDA0002322902400000046
indicating the total measurement error of the x, y and z-axis accelerometer, < >>
Figure BDA0002322902400000047
Representing random constant zero drift error component of x, y and z axis accelerometer, +.>
Figure BDA0002322902400000048
Representing the white gaussian noise error components of the x, y, z axis accelerometer.
According to the inertial navigation system update model and the error model of the gyroscope and the accelerometer, an astronomical and inertial combined navigation state quantity model can be obtained, and the method comprises the following steps:
misalignment angle error model
Figure BDA0002322902400000049
Wherein phi = [ phi ] E φ N φ U ] T Referred to as a misalignment angle error,
Figure BDA0002322902400000051
is the derivative of phi, δv= [ δv ] E δv N δv U ] T Respectively represent east-direction speed error, north-direction speed error and sky-direction speed error, δr= [ δlδλδh ]] T Representing latitude, longitude and altitude errors, respectively. [ epsilon ] x ε y ε z ]Representing the measurement errors contained in the measurements from the tri-axial gyroscopes,
Figure BDA0002322902400000052
representing the measurement error, ω, contained in the measurement by the triaxial accelerometer ie The rotational angular velocity of the earth is represented,
Figure BDA0002322902400000053
representing a pose transformation matrix of a carrier coordinate system to a local geographic coordinate system, R M And R is N The radius of the meridian and the radius of the mortise unitary circle at the position are respectively, L and h are latitude value and height value of the position of the carrier, v E And v N The east and north velocities in the local geographic coordinate system are represented, respectively, and x represents the inverse of this matrix representation.
Speed error model
Figure BDA0002322902400000054
Wherein phi = [ phi ] E φ N φ U ] T As misalignment angle error δv= [ δv ] E δv N δv U ] T Respectively represent an east speed error value, a north speed error value and an sky speed error value,
Figure BDA0002322902400000055
is the derivative of δv, δr= [ δlδλδh] T Respectively represent latitude error value, longitude error value and altitude error value, [ epsilon ] x ε y ε z ]Representing the measurement errors contained in the measurements from the tri-axial gyroscopes,
Figure BDA0002322902400000056
representing the measurement error, ω, contained in the measurement by the triaxial accelerometer ie Indicating the rotation angular velocity of the earth as a constant value, < ->
Figure BDA0002322902400000061
Representing a pose transformation matrix of a carrier coordinate system to a local geographic coordinate system, R M And R is N The meridian radius and the mortise unitary radius of the position are respectively,is uniquely determined by the position of the carrier, L and h are latitude value and altitude value of the position of the carrier, v E 、v N And v U The east and north and sky speeds under the local geographic coordinate system are represented, respectively, x represents the inverse of this matrix representation.
Position error model:
Figure BDA0002322902400000062
δr=[δL δλ δh] T to represent the latitude error value, the longitude error value and the altitude error value respectively,
Figure BDA0002322902400000063
is the derivative of δr, R M And R is N The radius of the meridian and the radius of the mortise circle at the position are respectively determined uniquely by the position of the carrier, L and h are the latitude value and the height value of the position of the carrier, v E 、v N And v U The east and north and sky speeds in the local geographic coordinate system are represented, respectively.
Gyroscope error model
Figure BDA0002322902400000064
Wherein 0 is 3*3 For a matrix of 3*3 zero values, [ epsilon ] bx ε by ε bz ] T Represents the random constant zero drift of the three-axis gyroscope,
Figure BDA0002322902400000065
is [ epsilon ] bx ε by ε bz ] T Is a derivative of (a).
Accelerometer error model:
Figure BDA0002322902400000066
wherein 0 is 3*3 Is a matrix of zeros of 3*3,
Figure BDA0002322902400000071
representing the random constant zero drift of the triaxial accelerometer,
Figure BDA0002322902400000072
is->
Figure BDA0002322902400000073
Is a derivative of (a).
Since the three-axis installation error angle of the astronomical navigation sensor is constant, the symbol representation mode is assumed to be δa= [ δa ] x δA y δA z ] T An installation error angle error model can be obtained:
Figure BDA0002322902400000074
wherein 0 is 3*3 A matrix of values of 3*3, representing δa= [ δa ] x δA y δA z ] T The astronomical navigation sensor is mounted with a three-axis error angle,
Figure BDA0002322902400000075
is [ delta A ] x δA y δA z ] T Is a derivative of (a).
And (3) sorting and combining the formulas (7) to (12) to obtain an astronomical and inertial combined navigation state quantity model as follows:
Figure BDA0002322902400000076
Figure BDA0002322902400000077
astronomical and inertial combined navigation attitude error, speed error, position error, gyroscope triaxial null shift, accelerometer triaxial null shift, astronomical navigation triaxial installation error angle, < >>
Figure BDA00023229024000000717
Is the derivative of the state quantity X, f (X (t), t) is the astronomical and inertial combined navigation state transfer function, w is the process noise, and w (t) is w at the moment t.
Step 3, establishing an astronomical and inertial integrated navigation measurement model
Assuming that an astronomical navigation sensor recognizes n stars, the starlight vectors of the n stars under an inertial coordinate system are
Figure BDA0002322902400000078
And a star vector in the star-sensitive coordinate system of +.>
Figure BDA0002322902400000079
Wherein the starlight vector of the ith star in the inertial coordinate system +.>
Figure BDA00023229024000000710
Star vector in star-sensitive coordinate system>
Figure BDA00023229024000000711
Column vectors of 3*1, will first be +.>
Figure BDA00023229024000000712
And->
Figure BDA00023229024000000713
Unifying to a local geographic coordinate system to get +.>
Figure BDA00023229024000000714
And->
Figure BDA00023229024000000715
The process is as follows:
Figure BDA00023229024000000716
wherein, therein
Figure BDA0002322902400000081
Represents the coordinate transformation from the inertial system to the geocentric fixed coordinate system, which is uniquely determined by the current time t,
Figure BDA0002322902400000082
coordinate transformation matrix representing geocentric-geodetic coordinate system given by inertial navigation to local-geodetic coordinate system,/v>
Figure BDA0002322902400000083
Coordinate transformation representing star-sensitive system to aircraft carrier system, as fixed value, +.>
Figure BDA0002322902400000084
Representing the gesture conversion matrix given by inertial navigation, I 3*3 Representing 3*3, δa represents the three-axis installation error angle of the astronomical navigation sensor.
Then subjecting the mixture obtained in the formula (14)
Figure BDA0002322902400000085
And->
Figure BDA0002322902400000086
And taking difference, taking measurement, and establishing a measurement model of astronomical and inertial integrated navigation on the ith star to obtain:
Z i =h i (X(t),t)+V i (t) A (15)
h i (X (t), t) represents the measurement function of the ith star of astronomical and inertial integrated navigation, V i And (t) represents the measurement noise contained in the star vector measurement value of the ith star at time t.
And (3) combining the measurement models of the n stars to obtain a whole astronomical and inertial integrated navigation measurement model:
Figure BDA0002322902400000087
step 4, discretizing the astronomical and inertial combined navigation state quantity model and the measurement model, and estimating the state quantity by using Kalman filtering
Discretizing the astronomical and inertial integrated navigation state quantity model obtained in the step 2 and the astronomical and inertial integrated navigation measurement model obtained in the step 3:
i.e.
Figure BDA0002322902400000088
Discretizing to obtain
Figure BDA0002322902400000089
Wherein X is K At t K Moment astronomical and inertial combined navigation state quantity X K-1 At t K-1 Time astronomical and inertial combined navigation state quantity phi K,K-1 At t K-1 From time to t K Moment astronomical and inertial combined navigation state transition matrix, w K-1 At t K-1 Time state noise matrix, Z K At t K Time measurement matrix, H K At t K Measurement coefficient matrix of time, V K At t K And measuring a noise matrix at the moment.
Then, estimating the astronomical and inertial combined navigation state quantity by adopting Kalman filtering:
Figure BDA0002322902400000091
wherein X is k|k-1 Is the state quantity X K-1 Is one-step predictive estimate of P k-1|k-1 At t K-1 Time filtering state estimation covariance matrix, Q k-1 At t K-1 Time state noise w K-1 Covariance matrix, P k|k-1 At t K-1 From time to t K State one-step prediction covariance matrix of moment, R k Representing t K Time measurement noise V K Covariance matrix, K k At t K Time filtering gain matrix, P k|k At t K Time instant filter state estimationCovariance matrix, X k|k Is the state quantity X K Is a Kalman filter estimate; x is X k|k The deployment format is as follows:
Figure BDA0002322902400000092
wherein the attitude error estimation value is: phi (phi) k|k =[φ E,k|k φ N,k|k φ U,k|k ] T The speed error estimate is: δv k|k =[δv E,k|k δv N,k|k δv U,k|k ] T Position error estimate δr k|k =[δL k|k δλ k|k δh k|k ] T
Step 5, correcting the output result of the inertial navigation updating model according to the Kalman filtering estimated value
Using the attitude error estimated value phi obtained in step 5 k|k =φ[ E,k|k φ N,k|k φ U,k|k ] T Position error estimation δr k|k =[δL k|k δλ k|k δh k|k ] T And a velocity error estimate δv k|k =[δv E,k|k δv N,k|k δv U,k|k ] T Correcting the attitude conversion matrix obtained by updating inertial navigation by the model in the step 1
Figure BDA0002322902400000093
The speed value v and the position value r are used for obtaining a combined navigation output result gesture conversion matrix +.>
Figure BDA0002322902400000094
Velocity value v Combination of two or more kinds of materials And a position value r Combination of two or more kinds of materials
The correction process is as follows:
Figure BDA0002322902400000095
step 6, outputting the position, speed and attitude information of the carrier
Output step 5Position r after correction Combination of two or more kinds of materials Velocity v Combination of two or more kinds of materials And gesture conversion matrix
Figure BDA0002322902400000101
And judging whether the navigation needs to be continued, if so, returning to the step 1, otherwise, ending the navigation.
The method needs the astronomical navigation sensor to have a measured value, if no measured value is output, the attitude conversion matrix determined in the step 1 is directly output
Figure BDA0002322902400000102
A velocity value v and a position value r.
Examples
To verify the performance of the method of the present invention, simulation experiments were performed using the trajectories of fig. 2. The errors of the traditional method and the method in the attitude, the speed and the position are compared with those shown in fig. 3-11, so that the method is smaller than the traditional method, and the precision of combined astronomical and inertial navigation is obviously improved.

Claims (5)

1. The astronomical and inertial integrated navigation method based on the starlight vector is characterized by comprising the following steps of:
step 1, establishing an inertial navigation attitude, speed and position updating model according to Newton's law of mechanics and Euler theorem of fixed point rotation of a rigid body;
step 2, establishing an astronomical and inertial combined navigation state quantity model according to error characteristics of the inertial navigation sensor and installation error angle characteristics of the astronomical navigation sensor;
step 3, establishing an astronomical and inertial integrated navigation measurement model according to the starlight vector under the inertial coordinate system and the starlight vector under the star-sensitive coordinate system;
step 4, discretizing an astronomical and inertial combined navigation state quantity model and a measurement model, and estimating a position error value, a speed error value and an attitude error value contained in an output value of an inertial navigation updating model on line by using Kalman filtering;
step 5, correcting the position, speed and attitude values obtained in the step 1 according to the estimated value in the step 4;
step 6, outputting the gesture, speed and position results obtained by combining astronomical and inertial navigation, judging whether the navigation is finished, and if not, performing step 1;
in the step 2, the specific method for constructing the astronomical and inertial combined navigation state quantity model is as follows:
firstly, establishing a model of gyro noise epsilon and accelerometer noise
Figure QLYQS_1
Model of (2)
Figure QLYQS_2
Wherein ε b And
Figure QLYQS_3
the random constant zero drift representing the gyroscope and the accelerometer is a constant value; epsilon g And->
Figure QLYQS_4
Is Gaussian white noise;
then determining the error model epsilon of the triaxial gyroscope x ε y ε z Triaxial accelerometer error model
Figure QLYQS_5
The method comprises the following steps:
Figure QLYQS_6
wherein [ epsilon ] x ε y ε z ] T Respectively representing the total measurement error of the x, y and z axis gyroscopes, [ epsilon ] bx ε by ε bz ] T Representing the random constant zero drift error component of the x, y and z axis gyroscopes [ epsilon ] gx ε gy ε gz ] T Representing gaussian white noise error components of the x-, y-, z-axis gyroscopes,
Figure QLYQS_7
indicating the total measurement error of the x, y and z-axis accelerometer, < >>
Figure QLYQS_8
Representing random constant zero drift error component of x, y and z axis accelerometer, +.>
Figure QLYQS_9
Representing Gaussian white noise error components of the x, y and z-axis accelerometers;
finally, according to the inertial navigation system updating model and the error model of the gyroscope and the accelerometer, obtaining an astronomical and inertial combined navigation state quantity model, comprising:
misalignment angle error model
Figure QLYQS_10
Wherein phi = [ phi ] E φ N φ U ] T Referred to as a misalignment angle error,
Figure QLYQS_11
is the derivative of phi, δv= [ δv ] E δv N δv U ] T Respectively represent east-direction speed error, north-direction speed error and sky-direction speed error, δr= [ δlδλδh ]] T Respectively representing latitude error, longitude error and altitude error, [ epsilon ] x ε y ε z ]Representing the measurement error contained in the measurement by the triaxial gyroscope,/->
Figure QLYQS_12
Representing the measurement error, ω, contained in the measurement by the triaxial accelerometer ie Indicating the rotational angular velocity of the earth>
Figure QLYQS_13
Representing a pose transformation matrix of a carrier coordinate system to a local geographic coordinate system, R M And R is N The radius of the meridian and the radius of the mortise unitary circle at the position are respectively, L and h are latitude value and height value of the position of the carrier, v E And v N Respectively representing the east and north speeds in the local geographic coordinate system, x representing the inverse of this matrix representation;
speed error model
Figure QLYQS_14
Wherein phi = [ phi ] E φ N φ U ] T As misalignment angle error δv= [ δv ] E δv N δv U ] T Respectively represent an east speed error value, a north speed error value and an sky speed error value,
Figure QLYQS_15
is the derivative of δv, δr= [ δlδλδh] T Respectively represent latitude error value, longitude error value and altitude error value, [ epsilon ] x ε y ε z ]Representing the measurement errors contained in the measurements from the tri-axial gyroscopes,
Figure QLYQS_16
representing the measurement error, ω, contained in the measurement by the triaxial accelerometer ie Indicating the rotation angular velocity of the earth as a constant value, < ->
Figure QLYQS_17
Representing a pose transformation matrix of a carrier coordinate system to a local geographic coordinate system, R M And R is N The radius of the meridian and the radius of the mortise circle at the position are respectively determined uniquely by the position of the carrier, L and h are the latitude value and the height value of the position of the carrier, v E 、v N And v U Respectively representing the east and north and the sky speeds in a local geographic coordinate system, x representing the inverse matrix representation;
position error model:
Figure QLYQS_18
δr=[δL δλ δh] T to represent the latitude error value, the longitude error value and the altitude error value respectively,
Figure QLYQS_19
is the derivative of δr, R M And R is N The radius of the meridian and the radius of the mortise circle at the position are respectively determined uniquely by the position of the carrier, L and h are the latitude value and the height value of the position of the carrier, v E 、v N And v U The east and north and sky speeds in the local geographic coordinate system are represented, respectively;
gyroscope error model
Figure QLYQS_20
Wherein 0 is 3*3 For a matrix of 3*3 zero values, [ epsilon ] bx ε by ε bz ] T Represents the random constant zero drift of the three-axis gyroscope,
Figure QLYQS_21
is [ epsilon ] bx ε by ε bz ] T Is a derivative of (2);
accelerometer error model:
Figure QLYQS_22
wherein 0 is 3*3 Is a matrix of zeros of 3*3,
Figure QLYQS_23
representing the random constant zero drift of the triaxial accelerometer,
Figure QLYQS_24
is->
Figure QLYQS_25
Is a derivative of (2);
installing an error angle error model:
Figure QLYQS_26
wherein 0 is 3*3 A matrix of values of 3*3, representing δa= [ δa ] x δA y δA z ] T The astronomical navigation sensor is mounted with a three-axis error angle,
Figure QLYQS_27
is [ delta A ] x δA y δA z ] T Is a derivative of (2);
the astronomical and inertial combined navigation state quantity models obtained by arranging and combining the formulas (7) to (12) are as follows:
Figure QLYQS_28
Figure QLYQS_29
astronomical and inertial combined navigation attitude error, speed error, position error, gyroscope triaxial null shift, accelerometer triaxial null shift, astronomical navigation triaxial installation error angle, < >>
Figure QLYQS_30
Is the derivative of the state quantity X, f (X (t), t) is the astronomical and inertial combined navigation state transfer function, w is the process noise, and w (t) is w at the moment t.
2. The astronomical and inertial integrated navigation method based on starlight vector according to claim 1, wherein in step 1, the inertial navigation gesture, speed and position update model is specifically:
according to Newton's law of mechanics and Euler's theorem of fixed point rotation of rigid body, the attitude, speed and position updating model of inertial navigation is established under a local geographic coordinate system, namely an east-north-sky coordinate system, as follows:
and (3) updating a model by the gesture:
Figure QLYQS_31
wherein, the liquid crystal display device comprises a liquid crystal display device,
Figure QLYQS_32
posture transformation matrix representing carrier coordinate system to local geographic coordinate system, < >>
Figure QLYQS_33
Representation->
Figure QLYQS_34
Derivative of>
Figure QLYQS_35
Representing the angular velocity of the inertial frame relative to the carrier frame, measured by the inertial navigation sensor gyro,/->
Figure QLYQS_36
Representing the angular velocity of the inertial coordinate system relative to the local geographic coordinate system, x representing the inverse of this matrix representation;
and (3) updating a model by speed:
Figure QLYQS_37
wherein v represents the velocity value of the carrier in the form of v= [ v ] E v N v U ] T Respectively representing the east and north speeds and the sky speed of the carrier under a local geographic coordinate system,
Figure QLYQS_38
for v derivative, < >>
Figure QLYQS_39
Posture transformation matrix representing carrier coordinate system to local geographic coordinate system, < >>
Figure QLYQS_40
The specific force value of the carrier in the carrier system is represented and is measured by an inertial navigation sensor accelerometer; />
Figure QLYQS_41
Expressed as the angular velocity of rotation of the earth->
Figure QLYQS_42
Represents the angular velocity, g, of the local geographic coordinate system relative to the geocentric fixed coordinate system n The x represents the gravitational acceleration of the carrier at the position opposite to the matrix representation;
a location update model:
Figure QLYQS_43
in the formula (3), r= [ lambda L h ]] T The longitude, latitude and altitude values respectively representing the position of the carrier,
Figure QLYQS_44
represents the derivative of R, R M And R is N The meridian radius and the mortise unitary radius of the position, v E 、v N And v U The east and north and sky speeds in the local geographic coordinate system are represented, respectively.
3. The astronomical and inertial integrated navigation method based on the starlight vector according to claim 1, wherein in step 3, the specific method for establishing the astronomical and inertial integrated navigation measurement model is as follows:
assuming that an astronomical navigation sensor recognizes n stars, the starlight vectors of the n stars under an inertial coordinate system are
Figure QLYQS_46
And a star vector in the star-sensitive coordinate system of +.>
Figure QLYQS_48
Wherein the starlight vector of the ith star in the inertial coordinate system +.>
Figure QLYQS_51
Star vector in star-sensitive coordinate system>
Figure QLYQS_47
Column vectors of 3*1, will first be +.>
Figure QLYQS_49
And->
Figure QLYQS_50
Unifying to a local geographic coordinate system to get +.>
Figure QLYQS_52
And->
Figure QLYQS_45
The process is as follows:
Figure QLYQS_53
wherein, therein
Figure QLYQS_54
Representing the coordinate transformation from the inertial system to the geocentric geodetic system, which is uniquely determined by the current time t,/->
Figure QLYQS_55
Representing geocentric coordinates given by inertial navigationCoordinate transformation matrix tied to local geographic coordinate system,/->
Figure QLYQS_56
Coordinate transformation representing star-sensitive system to aircraft carrier system, as fixed value, +.>
Figure QLYQS_57
Representing the gesture conversion matrix given by inertial navigation, I 3*3 Representing a 3*3 identity matrix, and delta A representing an astronomical navigation sensor triaxial installation error angle;
then subjecting the mixture obtained in the formula (14)
Figure QLYQS_58
And->
Figure QLYQS_59
And taking difference, taking measurement, and establishing a measurement model of astronomical and inertial integrated navigation on the ith star to obtain:
Z i =h i (X(t),t)+V i (t) A (15)
h i (X (t), t) represents the measurement function of the ith star of astronomical and inertial integrated navigation, V i (t) represents the measurement noise contained in the star vector measurement value of the ith star at time t;
and (3) combining the measurement models of the n stars to obtain a whole astronomical and inertial integrated navigation measurement model:
Figure QLYQS_60
4. the astronomical and inertial integrated navigation method based on the starlight vector according to claim 1, wherein the specific process of step 4 is as follows:
discretizing the astronomical and inertial integrated navigation state quantity model obtained in the step 2 and the astronomical and inertial integrated navigation measurement model obtained in the step 3:
i.e.
Figure QLYQS_61
Discretizing to obtain
Figure QLYQS_62
Wherein X is K At t K Moment astronomical and inertial combined navigation state quantity X K-1 At t K-1 Time astronomical and inertial combined navigation state quantity phi K,K-1 At t K-1 From time to t K Moment astronomical and inertial combined navigation state transition matrix, w K-1 At t K-1 Time state noise matrix, Z K At t K Time measurement matrix, H K At t K Measurement coefficient matrix of time, V K At t K Measuring a noise matrix at the moment;
then, estimating the astronomical and inertial combined navigation state quantity by adopting Kalman filtering:
Figure QLYQS_63
wherein X is kk-1 Is the state quantity X K-1 Is one-step predictive estimate of P k-1k-1 At t K-1 Time filtering state estimation covariance matrix, Q k-1 At t K-1 Time state noise w K-1 Covariance matrix, P kk-1 At t K-1 From time to t K State one-step prediction covariance matrix of moment, R k Representing t K Time measurement noise V K Covariance matrix, K k At t K Time filtering gain matrix, P kk At t K Time filtering state estimation covariance matrix X kk Is the state quantity X K Is a Kalman filter estimate; x is X kk The deployment format is as follows:
Figure QLYQS_64
wherein the attitude error estimation value is: phi (phi) k|k =[φ E,k|k φ N,k|k φ U,k|k ] T The speed error estimate is: δv k|k =[δv E,k|k δv N,k|k δv U,k|k ] T Position error estimate δr k|k =[δL k|k δλ k|k δh k|k ] T
5. The astronomical and inertial integrated navigation method based on the starlight vector according to claim 1, wherein the specific process of the step 5 is as follows:
using the attitude error estimated value phi obtained in step 5 k|k =[φ E,k|k φ N,k|k φ U,k|k ] T Position error estimation δr k|k =[δL k|k δλ k|k δh k|k ] T And a velocity error estimate δv k|k =[δv E,k|k δv N,k|k δv U,k|k ] T Correcting the attitude conversion matrix obtained by updating inertial navigation by the model in the step 1
Figure QLYQS_65
The speed value v and the position value r are used for obtaining a combined navigation output result gesture conversion matrix +.>
Figure QLYQS_66
Velocity value v Combination of two or more kinds of materials And a position value r Combination of two or more kinds of materials The correction process is as follows:
Figure QLYQS_67
CN201911305233.1A 2019-12-17 2019-12-17 Astronomical and inertial integrated navigation method based on starlight vector Active CN111121766B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201911305233.1A CN111121766B (en) 2019-12-17 2019-12-17 Astronomical and inertial integrated navigation method based on starlight vector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201911305233.1A CN111121766B (en) 2019-12-17 2019-12-17 Astronomical and inertial integrated navigation method based on starlight vector

Publications (2)

Publication Number Publication Date
CN111121766A CN111121766A (en) 2020-05-08
CN111121766B true CN111121766B (en) 2023-07-07

Family

ID=70499509

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201911305233.1A Active CN111121766B (en) 2019-12-17 2019-12-17 Astronomical and inertial integrated navigation method based on starlight vector

Country Status (1)

Country Link
CN (1) CN111121766B (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111947653A (en) * 2020-08-13 2020-11-17 北京航空航天大学 Dual-mode inertial/visual/astronomical navigation method for lunar surface inspection tour detector
CN111947652B (en) * 2020-08-13 2022-09-20 北京航空航天大学 Inertia/vision/astronomy/laser ranging combined navigation method suitable for lunar lander
CN113218390B (en) * 2021-05-27 2022-09-27 西北工业大学 Rotation inertia astronomy combined navigation method based on attitude and star altitude angle fusion
CN113252029B (en) * 2021-06-04 2021-10-22 华中光电技术研究所(中国船舶重工集团公司第七一七研究所) Astronomical navigation attitude transfer method based on optical gyroscope measurement information
CN113551667A (en) * 2021-07-21 2021-10-26 北京航空航天大学 Spacecraft inertia/fixed star light vector/sun Doppler velocity combined navigation method
CN113551668A (en) * 2021-07-21 2021-10-26 北京航空航天大学 Spacecraft inertia/fixed star light vector/star light refraction combined navigation method
CN117606474B (en) * 2024-01-24 2024-03-29 北京神导科技股份有限公司 Inertial astronomical combined navigation time synchronization method based on quaternion second-order interpolation

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102519470A (en) * 2011-12-09 2012-06-27 南京航空航天大学 Multi-level embedded integrated navigation system and navigation method
CN107036598A (en) * 2017-03-30 2017-08-11 南京航空航天大学 Dual quaterion inertia/celestial combined navigation method based on gyro error amendment
CN108731674A (en) * 2018-06-08 2018-11-02 西北工业大学 A kind of inertia celestial combined navigation system and computational methods based on single-shaft-rotation modulation
CN108871326A (en) * 2018-07-09 2018-11-23 北京航空航天大学 A kind of single-shaft-rotation modulation inertia-astronomy deep integrated navigation method

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102519470A (en) * 2011-12-09 2012-06-27 南京航空航天大学 Multi-level embedded integrated navigation system and navigation method
CN107036598A (en) * 2017-03-30 2017-08-11 南京航空航天大学 Dual quaterion inertia/celestial combined navigation method based on gyro error amendment
CN108731674A (en) * 2018-06-08 2018-11-02 西北工业大学 A kind of inertia celestial combined navigation system and computational methods based on single-shaft-rotation modulation
CN108871326A (en) * 2018-07-09 2018-11-23 北京航空航天大学 A kind of single-shaft-rotation modulation inertia-astronomy deep integrated navigation method

Also Published As

Publication number Publication date
CN111121766A (en) 2020-05-08

Similar Documents

Publication Publication Date Title
CN111121766B (en) Astronomical and inertial integrated navigation method based on starlight vector
CN110487301B (en) Initial alignment method of radar-assisted airborne strapdown inertial navigation system
CN107655476B (en) Pedestrian high-precision foot navigation method based on multi-information fusion compensation
CN112629538B (en) Ship horizontal attitude measurement method based on fusion complementary filtering and Kalman filtering
CN110501024B (en) Measurement error compensation method for vehicle-mounted INS/laser radar integrated navigation system
CN109459044B (en) GNSS dual-antenna assisted vehicle-mounted MEMS inertial navigation combined navigation method
EP2557394B1 (en) System for processing pulse signals within an inertial navigation system
CN107588769B (en) Vehicle-mounted strapdown inertial navigation, odometer and altimeter integrated navigation method
CN106990426B (en) Navigation method and navigation device
JP4782111B2 (en) System and method for estimating position, attitude and / or direction of flight of a vehicle
CN110017837B (en) Attitude anti-magnetic interference combined navigation method
CN111156994A (en) INS/DR &amp; GNSS loose integrated navigation method based on MEMS inertial component
CN110207691B (en) Multi-unmanned vehicle collaborative navigation method based on data link ranging
CN112504275B (en) Water surface ship horizontal attitude measurement method based on cascade Kalman filtering algorithm
CN104697526A (en) Strapdown inertial navitation system and control method for agricultural machines
CN103245359A (en) Method for calibrating fixed errors of inertial sensor in inertial navigation system in real time
CN112577519B (en) Aerospace vehicle star sensor installation error online calibration method
CN110296719B (en) On-orbit calibration method
CN111189442A (en) Multi-source navigation information state prediction method of unmanned aerial vehicle based on CEPF
CN110849360A (en) Distributed relative navigation method for multi-machine cooperative formation flight
CN112880669A (en) Spacecraft starlight refraction and uniaxial rotation modulation inertia combined navigation method
CN112556724A (en) Initial coarse alignment method for low-cost navigation system of micro aircraft in dynamic environment
CN113916222B (en) Combined navigation method based on Kalman filtering estimation variance constraint
CN114964222A (en) Vehicle-mounted IMU attitude initialization method, and mounting angle estimation method and device
CN109084755B (en) Accelerometer zero offset estimation method based on gravity apparent velocity and parameter identification

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
CB03 Change of inventor or designer information

Inventor after: Chen Qingwei

Inventor after: Zhang Yu

Inventor after: Qian Chen

Inventor after: Wu Yifei

Inventor after: Fan Jie

Inventor after: Yan Fei

Inventor after: Guo Jian

Inventor after: Wang Xiao

Inventor after: Shu Haiyang

Inventor after: Wei Qinghua

Inventor before: Fan Jie

Inventor before: Zhang Yu

Inventor before: Yan Fei

Inventor before: Qian Chen

Inventor before: Chen Qingwei

Inventor before: Guo Jian

Inventor before: Wu Yifei

Inventor before: Wang Xiao

Inventor before: Shu Haiyang

Inventor before: Wei Qinghua

CB03 Change of inventor or designer information
GR01 Patent grant
GR01 Patent grant