CN108088464B - Deflection estimation method for correcting installation error of closed loop - Google Patents
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- G01C—MEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
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Abstract
The invention belongs to the technical field of inertial measurement, and particularly relates to a deflection estimation method for correcting installation errors in a closed loop. The method comprises nine steps, wherein the first step is to define a coordinate system, the second step is to carry out navigation operation based on an inertial system, the third step is to establish a flexural error model, the fourth step is to establish a system error equation, the fifth step is to establish a measurement equation, the sixth step is to calculate a measurement value, the seventh step is to calculate by utilizing a Kalman filtering equation, the eighth step is to carry out closed-loop correction on an installation error angle and a flexural deformation angle, and the ninth step is to repeat the closed-loop correction on the flexural deformation angle. Compared with the traditional method, the method can greatly improve the measurement precision and the estimation speed, enhance the attitude information measurement precision of different parts of the carrier platform and improve the use efficiency of related equipment.
Description
Technical Field
The invention belongs to the technical field of inertial measurement, and particularly relates to a deflection estimation method for correcting installation errors in a closed loop.
Background
The dynamic deflection deformation of the carrier platform can influence the use of the sub inertial navigation equipment on main reference information, and influence the measurement accuracy of equipment installed on the carrier platforms such as ships, aircraft wings and ground vehicles, so that the deflection deformation characteristic of the carrier platform must be effectively measured and compensated. The deflection deformation is mainly due to the influence of external stress such as temperature change, external impact, air flow, self load and the like and the surrounding environment, the structure of the carrier platform can be subjected to dynamic deformation in different degrees, and the deflection deformation can be divided into static deflection and dynamic deflection.
The static deflection deformation is a deformation phenomenon caused by expansion and contraction with heat, contraction with cold, structural stress release and the like of the carrier platform in the moving process, is mainly influenced by factors such as load, temperature, sunlight and the like, has long change period and is relatively stable, and the quasi-static deflection deformation can be considered as a constant value in a short transfer alignment time. Titterton et al in uk have shown that changes in load on ships and structural ageing cause deformation of the ship, which can produce angular changes of about 1 ° in the course of a day under the action of sunlight.
The dynamic deflection changes constantly as a function of external conditions, such as motion of the carrier, impact, etc., i.e., the dynamic deflection is a function of time. The static deformation can be approximately regarded as a fixed installation error between the main inertial navigation system and the sub inertial navigation system, while the dynamic deflection deformation is a physical quantity which is superposed on the static deflection and changes along with time, and the specific forming reason of the dynamic deflection deformation is different according to the type of the carrier platform.
In an offshore platform, the dynamic deflection deformation of a ship is a phenomenon that the ship body is not a rigid body and generates deformation and structural vibration under the action of external force, external moment and wave impact. The high-frequency deflection deformation is mainly deformation of missile launcher and hull structures caused by sea wave impact and ship maneuvering and shaking. According to the obtained deformation data measured during navigation under the six-level sea condition, the method comprises the following steps: the deformation of the installation position of the inertial navigation system around the longitudinal rocking shaft is 0.05-0.08 degrees at the position of +/-7 m along the direction of the transverse shaft and +/-1.5 m along the direction of the longitudinal shaft, and the deformation around the transverse rocking shaft is 0.17-0.2 degrees; the deformation at the installation position of the radar antenna pedestal is 0.38 degrees, and the deformation at the installation positions of the front cannon and the rear cannon is 0.23 degrees.
On an airplane platform, the flexural deformation refers to the phenomenon that the wing is not a rigid body and is deformed and structurally vibrated under the action of external force, external moment, aerodynamic load and turbulence. The deflection deformation of the carrier in flight is mainly divided into two types, one is static deflection deformation, and the other is high-frequency deflection deformation. The static deflection deformation is a low-frequency wing deformation phenomenon caused by the change of the load of the airplane due to the mechanical operation or weapon release of the airplane; the high-frequency deflection deformation is mainly the structural vibration of the airplane at 5-10 Hz caused by turbulent flow.
Currently, the common deflection measurement methods are classified into two types, one is optical measurement, and the other is achieved by high-precision inertial measurement. The high-precision inertial measurement is mainly realized by Kalman filtering and by using the attitude difference of inertial measurement distributed at different positions. And the current method can not realize on-line deflection error compensation.
Therefore, the difference of attitude measurement information of different positions of the naval vessel is considered to be utilized, an error equation of attitude difference is established, the error equation comprises inertial navigation gyro drift, fixed installation error, a flexural deformation model and the like, the estimation of installation error and flexural deformation is realized through a Kalman filtering technology, and the measurement of high-precision attitude of different positions is realized.
Disclosure of Invention
According to the problems, the invention provides a deflection estimation method for correcting installation errors in a closed loop mode.
In order to realize the purpose, the invention adopts the technical scheme that:
a deflection estimation method for correcting installation errors in a closed loop mode comprises nine steps, wherein a first step is to define a coordinate system, a second step is to perform navigation operation based on an inertial system, a third step is to establish a deflection error model, a fourth step is to establish a system error equation, a fifth step is to establish a measurement equation, a sixth step is to calculate a measurement value, a seventh step is to calculate by using a Kalman filter equation, an eighth step is to perform closed loop correction of an installation error angle and a deflection deformation angle, and a ninth step is to perform repeated closed loop correction of the deflection deformation angle, the coordinate system is defined, and an auxiliary coordinate system needs to be introduced into an attitude matching calculation method:
inertial frame i1:t0B, performing inertial solidification on a moment sub-inertial navigation calculation carrier system b;
inertial frame i2:t0The m series inertia of the moment main inertia load system is solidified;
terrestrial coordinate system e: the x axis is along the direction of the earth axis, the y axis is along the intersection line of the equatorial plane and the Greenwich meridian plane, and the z axis, the x axis and the y axis form a right-hand coordinate system in the equatorial plane;
earth inertial coordinate system i: t is t0And (4) obtaining a time terrestrial coordinate system e through inertial solidification.
The second step is based on navigation operation of an inertial system, and a quaternion is set:
Q1=[q0 q1 q2 q3]Tand an initial value Q1(0)=[1 0 0 0]T。
The analytic formula of quaternion update is as follows:
wherein:
i is a 4 multiplied by 4 order identity matrix;
calculating the angular incremental component of the projectile body relative to the inertial system for the moments k to k +1, i.e.
The angular increment sensed by the gyro is transformed to the angular increment after the computational ballistic system, obtained by:
wherein T isnIn order to solve the cycle for the navigation,is the angular velocity of the gyroscope in the x, y and z directions,the updating calculation formula of the attitude matrix is as follows:
the deflection estimation method for correcting installation errors in a closed loop mode comprises the third step of establishing a deflection error model and setting a deflection deformation model of a carrier platformNamely, the dynamic deformation angle of the child inertial navigation relative to the parent inertial navigation is as follows:
wherein theta isx,θy,θzThe dynamic deformation angle of the child inertial navigation relative to the parent inertial navigation in the x, y and z directions is shown.
Assuming a deflection deformation angular velocity variable ofμx,μy,μzFor flexural deformation angular velocities in the x, y, z directions, and assuming that the deformation processes of the three axes are independent of each other, then
The second order Markov equation of motion for the flexural deformation can be derived as
In the formula, betai=2.146/τi,τiThe relative time constant representing the deformation of the carrier platform i (i ═ x, y, z); w is ax、wyAnd wzRepresenting a white noise sequence which is driving information of deflection angles, whose variances are Qrx、QryAnd QrzAnd Q isri=4β2 iσ2 i;
In summary, the state equation of the carrier stage deflection deformation is:
the method for estimating the deflection of the closed-loop corrected installation error comprises the fourth step of establishing a system error equation, and selecting 16 error state variables as
X=[Φ Φa ξ ω ε tA]T
Wherein:
Φ=[φx φy φz]three axis attitude error angles for the inertial system X, Y, Z;
Φa=[φax φay φaz]three axis misalignment angles for carrier system X, Y, Z;
ξ=[θx θy θz]Tthree axis misalignment angular deflections for carrier system X, Y, Z;
ω=[μx μy μz]Tangular velocities for three axis misalignment angular deflection deformation of carrier system X, Y, Z;
ε=[εx εy εz]x, Y, Z three-axis gyro drift;
tA: a reference attitude delay time.
Written in the form of a state equation as follows
WhereinT represents transposition; and B is a system noise vector. Wherein,may be obtained by inertial system based navigation solutions.
The deflection estimation method for correcting the installation error of the closed loop comprises the fifth step of establishing a measurement equation which is as follows
Wherein,outputting a triaxial angular rate for the gyroscope; the calculation of A and B requires the use of a matrixObtained by the following formula:
wherein t is0The specific calculation method of each matrix represents the initial filtering time is as follows:
wherein, γ0、ψ0And theta0Respectively is a rolling angle, a course angle and a pitch angle of the reference inertial navigation system at the initial moment,
wherein L is0And λ0Respectively, longitude and latitude of the initial time reference inertial navigation system.
for a change matrix from an earth system to an inertial system, the calculation method comprises the following steps:
wherein, ω isieIs the earth rotation angular rate and t is time.
Wherein λ and L are longitude and latitude of the reference inertial navigation system, respectively.
Wherein gamma, psi and theta are respectively a roll angle, a course angle and a pitch angle of the reference inertial navigation system.
A method for estimating the deflection of a closed loop correcting installation error, the sixth step is to calculate a measurement value,
a deflection estimation method for correcting installation errors in a closed loop, wherein the seventh step is calculated by using a Kalman filtering equation,
after the error model is established, a Kalman filtering method is selected as a parameter identification method, and the formula is as follows:
state one-step prediction
State estimation
Filter gain matrix
One-step prediction error variance matrix
Estimation error variance matrix
Pk=[I-KkHk]Pk,k-1
Wherein,in order to predict the value of the one-step state,estimate the matrix for the state, phik,k-1For a state one-step transition matrix, HkFor measuring the matrix, ZkMeasurement of quantitative value, KkFor filtering the gain matrix, RkFor observing noise arrays, Pk,k-1For one-step prediction of error variance matrix, PkTo estimate the error variance matrix, Γk,k-1For system noise driven arrays, Qk-1Is a system noise matrix.
A deflection estimation method for correcting installation errors in a closed loop mode comprises the following steps of correcting an installation error angle and a deflection deformation angle in the closed loop mode in eight steps:
A deflection estimation method for correcting installation errors in a closed loop mode is characterized in that the step nine is repeated for correcting a deflection deformation angle in a closed loop mode, the error angle and the deflection deformation angle are corrected in the step one to eight, but the error angle and the deflection deformation angle are not converged and cannot reach the required precision, so that the error angle and the deflection deformation angle need to be repeatedly corrected, the step one to eight are repeated until the estimation results of the error angle and the deflection deformation angle are converged, and the method is finished.
The invention has the beneficial effects that:
according to the method, the attitude information of a plurality of sets of inertial navigation systems is utilized, the estimation of the inertial navigation gyro drift, the fixed mounting error, the flexural deformation model and other error information can be realized through the Kalman filtering technology, the fixed mounting error and the flexural deformation are corrected in a closed loop mode, the measurement precision and the estimation speed can be greatly improved compared with the traditional method, the attitude information measurement precision of different parts of a carrier platform can be enhanced, and the use efficiency of related equipment is improved.
Detailed Description
The specific embodiment of the invention is as follows:
the method provided by the invention comprises nine steps, wherein the first step is to define a coordinate system, the second step is to perform navigation operation based on an inertial system, the third step is to establish a flexural error model, the fourth step is to establish a system error equation, the fifth step is to establish a measurement equation, the sixth step is to calculate a measurement value, the seventh step is to calculate by using a Kalman filtering equation, the eighth step is to perform closed-loop correction on an installation error angle and a flexural deformation angle, and the ninth step is to repeat the closed-loop correction on the flexural deformation angle.
Step one, defining a coordinate system
In the pose matching calculation method, an auxiliary coordinate system needs to be introduced:
(1) inertial frame i1:t0B, performing inertial solidification on a moment sub-inertial navigation calculation carrier system b;
(2) inertial frame i2:t0The m series inertia of the moment main inertia load system is solidified;
(3) terrestrial coordinate system e: the x axis is along the direction of the earth axis, the y axis is along the intersection line of the equatorial plane and the Greenwich meridian plane, and the z axis, the x axis and the y axis form a right-hand coordinate system in the equatorial plane;
(4) earth inertial coordinate system i: t is t0And (4) obtaining a time terrestrial coordinate system e through inertial solidification.
Step two, navigation operation based on inertia system
Setting quaternion:
Q1=[q0 q1 q2 q3]Tand an initial value Q1(0)=[1 0 0 0]T。
The analytic formula of quaternion update is as follows:
wherein:
i is a 4 multiplied by 4 order identity matrix;
calculating the angular incremental component of the projectile body relative to the inertial system for the moments k to k +1, i.e.
The angular increment sensed by the gyro is transformed to the angular increment after the computational ballistic system, obtained by:
wherein T isnIn order to solve the cycle for the navigation,is the angular velocity of the gyroscope in the x, y and z directions,the updating calculation formula of the attitude matrix is as follows:
step three, establishing a flexural error model
The establishment of the carrier platform flexural deformation model involves the professional knowledge in the aspects of complex elastic mechanics and the like, and the flexure cannot be simply ignored or the flexural deformation is taken as a constant condition. Causing deformation of the carrier platformThe reasons for (1) mainly include the effects of various factors such as impact, which is consistent with the condition of white noise excitation; in addition, carrier platform deflections, both inertial and restoring moments, can be considered as typical mass-spring systems. The second order Markov process modeling can adapt to the common flexural deformation and can ensure the considerable precision, therefore, the second order Markov process is adopted to build a mathematical model for the flexural deformation of the carrier platform.
Deflection of carrier platformNamely, the dynamic deformation angle of the child inertial navigation relative to the parent inertial navigation is as follows:
wherein theta isx,θy,θzThe dynamic deformation angle of the child inertial navigation relative to the parent inertial navigation in the x, y and z directions is shown.
Assuming a deflection deformation angular velocity variable ofμx,μy,μzFor flexural deformation angular velocities in the x, y, z directions, and assuming that the deformation processes of the three axes are independent of each other, then
The second order Markov equation of motion for the flexural deformation can be derived as
In the formula, betai=2.146/τi,τiThe relative time constant representing the deformation of the carrier platform i (i ═ x, y, z); w is ax、wyAnd wzRepresenting a white noise sequence which is driving information of deflection angles, whose variances are Qrx、QryAnd QrzAnd Q isri=4β2 iσ2 i。
In summary, the state equation of the carrier stage deflection deformation is:
step four, establishing a system error equation
According to the error characteristics of the inertial navigation system, selecting 16 error state variables as
X=[Φ Φa ξ ω ε tA]T
Wherein:
Φ=[φx φy φz]three axis attitude error angles for the inertial system X, Y, Z;
Φa=[φax φay φaz]three axis misalignment angles for carrier system X, Y, Z;
ξ=[θx θy θz]Tthree axis misalignment angular deflections for carrier system X, Y, Z;
ω=[μx μy μz]Tangular velocities for three axis misalignment angular deflection deformation of carrier system X, Y, Z;
ε=[εx εy εz]x, Y, Z three-axis gyro drift;
tA: a reference attitude delay time.
Written in the form of a state equation as follows
WhereinT represents transposition; and B is a system noise vector. Wherein,may be obtained by inertial system based navigation solutions.
Step five, establishing a measurement equation
The measurement equation is as follows
Wherein,outputting a triaxial angular rate for the gyroscope; the calculation of A and B requires the use of a matrixObtained by the following formula:
wherein t is0The specific calculation method of each matrix represents the initial filtering time is as follows:
wherein, γ0、ψ0And theta0Respectively is a rolling angle, a course angle and a pitch angle of the reference inertial navigation system at the initial moment,
wherein L is0And λ0Respectively, longitude and latitude of the initial time reference inertial navigation system.
for a change matrix from an earth system to an inertial system, the calculation method comprises the following steps:
wherein, ω isieIs the earth rotation angular rate and t is time.
Wherein λ and L are longitude and latitude of the reference inertial navigation system, respectively.
Wherein gamma, psi and theta are respectively a roll angle, a course angle and a pitch angle of the reference inertial navigation system.
Step six, calculating a measured value
Step seven, calculating by using a Kalman filtering equation
After the error model is established, a Kalman filtering method is selected as a parameter identification method, a Kalman filtering equation adopts a form in a document Kalman filtering and integrated navigation principle (first edition, edited by Qin Yongyuan and the like), and a specific formula is as follows:
state one-step prediction
State estimation
Filter gain matrix
One-step prediction error variance matrix
Estimation error variance matrix
Pk=[I-KkHk]Pk,k-1
Wherein,in order to predict the value of the one-step state,estimate the matrix for the state, phik,k-1For a state one-step transition matrix, HkFor measuring the matrix, ZkMeasurement of quantitative value, KkFor filtering the gain matrix, RkFor observing noise arrays, Pk,k-1For one-step prediction of error variance matrix, PkTo estimate the error variance matrix, Γk,k-1For system noise driven arrays, Qk-1Is a system noise matrix.
Step eight, closed-loop correction of installation error angle and deflection deformation angle
The correction method comprises the following steps:
Nine steps, repeated deflection deformation angle closed loop correction
Since the error angle and the deflection deformation angle are corrected in the above steps one to eight, but the error angle and the deflection deformation angle are not converged and cannot reach the required precision, the error angle and the deflection deformation angle need to be repeatedly corrected, so the above steps one to eight are repeated until the estimation results of the error angle and the deflection deformation angle are converged, and the method is ended.
Claims (6)
1. A deflection estimation method for correcting installation errors in a closed loop mode comprises nine steps, wherein a first step is to define a coordinate system, a second step is to perform navigation operation based on an inertial system, a third step is to establish a deflection error model, a fourth step is to establish a system error equation, a fifth step is to establish a measurement equation, a sixth step is to calculate a measurement value, a seventh step is to calculate by using a Kalman filtering equation, an eighth step is to perform closed loop correction of an installation error angle and a deflection deformation angle, and a ninth step is to perform repeated closed loop correction of the deflection deformation angle, and the method is characterized in that: the step defines a coordinate system, and in the attitude matching calculation method, an auxiliary coordinate system needs to be introduced: inertial frame i1:t0B, performing inertial solidification on a moment sub-inertial navigation calculation carrier system b; inertial frame i2:t0The m series inertia of the moment main inertia load system is solidified; terrestrial coordinate system e: the x axis is along the direction of the earth axis, the y axis is along the intersection line of the equatorial plane and the Greenwich meridian plane, and the z axis, the x axis and the y axis form a right-hand coordinate system in the equatorial plane; earth inertial coordinate system i: t is t0The e system of the earth coordinate system is obtained by inertial solidification at any moment;
secondly, navigation operation based on an inertial system;
setting quaternion:
Q1=[q0 q1 q2 q3]Tand an initial value Q1(0)=[1 0 0 0]T;
The analytic formula of quaternion update is as follows:
wherein:
i is a 4 multiplied by 4 order identity matrix;
calculating the angular increment component of the elastic system relative to the inertia system for the time k to k +1, namely converting the angular increment sensed by the gyro into the angular increment after the elastic system is calculated, and obtaining the following formula:
wherein T isnIn order to solve the cycle for the navigation,is the angular velocity of the gyroscope in the x, y and z directions,the updating calculation formula of the attitude matrix is as follows:
thirdly, establishing a flexural error model;
deflection of carrier platformNamely, the dynamic deformation angle of the child inertial navigation relative to the parent inertial navigation is as follows:
wherein theta isx,θy,θzThe dynamic deformation angle of the child inertial navigation relative to the parent inertial navigation in the x, y and z directions is obtained;
assuming a deflection deformation angular velocity variable ofμx,μy,μzIs the angle of deflection in the x, y, z directionsSpeed, provided that the deformation processes of the three axes are independent of each other, then
The second order Markov equation of motion for the flexural deformation can be derived as
In the formula, betai=2.146/τi,τiThe relative time constant representing the deformation of the carrier platform i, i ═ x, y, z; w is ax、wyAnd wzRepresenting a white noise sequence which is driving information of deflection angles, whose variances are Qrx、QryAnd QrzAnd Q isri=4β2 iσ2 i;
In summary, the state equation of the carrier stage deflection deformation is:
establishing a system error equation;
according to the error characteristics of the inertial navigation system, selecting 16 error state variables as
X=[Φ Φa ξ ω ε tA]T
Wherein:
Φ=[φx φy φz]three axis attitude error angles for the inertial system X, Y, Z;
Φa=[φax φay φaz]three axis misalignment angles for carrier system X, Y, Z;
ξ=[θx θy θz]Tis a vector system X, Y, Z IIIDeflection deformation of an installation error angle of each shaft;
ω=[μx μy μz]Tangular velocities for three axis misalignment angular deflection deformation of carrier system X, Y, Z;
ε=[εx εy εz]x, Y, Z three-axis gyro drift;
tA: a reference attitude delay time;
written in the form of a state equation:
2. A closed-loop, installation error corrected, deflection estimation method as set forth in claim 1, wherein: step five, establishing a measurement equation;
the measurement equation is as follows:
wherein,outputting a triaxial angular rate for the gyroscope; the calculation of A and B requires the use of a matrixObtained by the following formula:
wherein t is0The specific calculation method of each matrix represents the initial filtering time is as follows:
wherein, γ0、ψ0And theta0Respectively is a rolling angle, a course angle and a pitch angle of the reference inertial navigation system at the initial moment,
wherein L is0And λ0Respectively representing the longitude and the latitude of the initial time reference inertial navigation system;
for a matrix of changes from the earth system to the inertial systemThe calculation method comprises the following steps:
wherein, ω isieThe rotation angular rate of the earth, and t is time;
wherein, λ and L are respectively longitude and latitude of the reference inertial navigation system;
wherein gamma, psi and theta are respectively a rolling angle, a course angle and a pitch angle of the reference inertial navigation system;
4. A closed-loop, installation error corrected, deflection estimation method as set forth in claim 1, wherein: seventhly, calculating by using a Kalman filtering equation;
after the error model is established, a Kalman filtering method is selected as a parameter identification method, and the specific formula is as follows:
state one-step prediction
State estimation
Filter gain matrix
One-step prediction error variance matrix
Estimation error variance matrix
Pk=[I-KkHk]Pk,k-1
Wherein,in order to predict the value of the one-step state,estimate the matrix for the state, phik,k-1For a state one-step transition matrix, HkFor measuring the matrix, ZkMeasurement of quantitative value, KkFor filtering the gain matrix, RkFor observing noise arrays, Pk,k-1For one-step prediction of error variance matrix, PkTo estimate the error variance matrix, Γk,k-1For system noise driven arrays, Qk-1Is a system noise matrix.
5. A closed-loop, installation error corrected, deflection estimation method as set forth in claim 2, wherein: step eight, correcting the installation error angle and the deflection deformation angle in a closed loop manner;
the correction method comprises the following steps:
6. A closed-loop, installation error corrected, deflection estimation method as set forth in claim 1, wherein: the step nine is repeated for the deflection deformation angle closed loop correction, and since the error angle and the deflection deformation angle are corrected in the steps one to eight, but the error angle and the deflection deformation angle are not converged and cannot reach the required precision, the error angle and the deflection deformation angle are required to be repeatedly corrected, and the steps one to eight are repeated until the estimation results of the error angle and the deflection deformation angle are converged.
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Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0989585A (en) * | 1995-09-22 | 1997-04-04 | Tokimec Inc | Inertial navigation system |
CN104567930A (en) * | 2014-12-30 | 2015-04-29 | 南京理工大学 | Transfer alignment method capable of estimating and compensating wing deflection deformation |
CN104977001A (en) * | 2014-04-02 | 2015-10-14 | 北京自动化控制设备研究所 | Relative navigation method applied to individual indoor navigation system |
-
2016
- 2016-11-22 CN CN201611031747.9A patent/CN108088464B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0989585A (en) * | 1995-09-22 | 1997-04-04 | Tokimec Inc | Inertial navigation system |
CN104977001A (en) * | 2014-04-02 | 2015-10-14 | 北京自动化控制设备研究所 | Relative navigation method applied to individual indoor navigation system |
CN104567930A (en) * | 2014-12-30 | 2015-04-29 | 南京理工大学 | Transfer alignment method capable of estimating and compensating wing deflection deformation |
Non-Patent Citations (1)
Title |
---|
"舰载武器SINS速度+姿态匹配传递对准建模与仿真";申亮亮 等;《鱼雷技术》;20081031;第16卷(第5期);正文第22-27页 * |
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