WO2020114301A1 - Magnetic-side roll angular velocity information-based rotary shell flight posture high-precision estimation method - Google Patents

Magnetic-side roll angular velocity information-based rotary shell flight posture high-precision estimation method Download PDF

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WO2020114301A1
WO2020114301A1 PCT/CN2019/121491 CN2019121491W WO2020114301A1 WO 2020114301 A1 WO2020114301 A1 WO 2020114301A1 CN 2019121491 W CN2019121491 W CN 2019121491W WO 2020114301 A1 WO2020114301 A1 WO 2020114301A1
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error
equation
projectile
attitude
velocity
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PCT/CN2019/121491
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French (fr)
Chinese (zh)
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龙达峰
曹建忠
魏晓慧
罗中良
徐瑜
徐德明
孙俊丽
谢珩
蔡远创
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惠州学院
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F42AMMUNITION; BLASTING
    • F42BEXPLOSIVE CHARGES, e.g. FOR BLASTING, FIREWORKS, AMMUNITION
    • F42B35/00Testing or checking of ammunition
    • F42B35/02Gauging, sorting, trimming or shortening cartridges or missiles

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  • the invention relates to a method for measuring the three-dimensional attitude of an aircraft or a missile space, in particular to a high-precision method for measuring the flying attitude of a rotating bomb.
  • the existing attitude filter model based on the assumption of small misalignment error angle, which ignores the high-order filter model and cannot accurately describe the strong nonlinear characteristics of the rotating projectile system, these will directly affect the design of the projectile attitude filter Problems such as the convergence speed and filter accuracy of the filter, and even the filter divergence, can also cause the large error parameter estimation results of the filter.
  • the present invention addresses the problem that the "three heights" of high overload, high self-rotation and high dynamics of the launch of the rotating bomb limit the existing mature bomb-borne attitude measurement system and cannot be directly transplanted to the rotating bomb.
  • a single-axis gyroscope and a satellite receiver form a rotating missile flight attitude measurement scheme, and a high-precision filtering estimation method suitable for the rotating bomb flight attitude is proposed for this measurement scheme.
  • a high-precision estimation method for the flying attitude of a rotating projectile based on magnetic measurement of roll angular rate includes the following steps:
  • the bomb-mounted sensor uses a three-axis geomagnetic sensor, two single-axis gyroscopes and a satellite receiver. Among them, the three-axis geomagnetic sensor is used to measure the vector information of the geomagnetic field inside the projectile.
  • the directions of each sensitive axis Mx, My and Mz and the projectile The coordinate system OX b Y b Z b has the same direction of each axis; two single-axis gyroscopes Gy and Gz are respectively installed on the Y b and Z b axes, and the gyroscopes are used to measure the Y-axis and Z-axis angular rates of the projectile Information, the X-axis angular rate information is estimated by filtering the geomagnetic sensor measurement information; the satellite receiver is used to measure the velocity and position information of the projectile, and the receiver antenna is installed on the surface of the projectile in a loop.
  • the combined filter is composed of two filters, a roll angle rate estimation filter and a high-precision filter for the flight attitude of the projectile, which are used to estimate the roll rate of the projectile and the high-precision estimation of the flight attitude of the projectile, respectively.
  • the obtained body attitude transformation matrix is:
  • the velocity error equation is a nonlinear error equation, where The term is its nonlinear part. If the nonlinear part in the velocity error equation (14) is assumed to be f 1 (x, t):
  • the body position error equation is:
  • V E , V N , and V U are the velocity of the projectile in the east, north, and sky directions;
  • R M and R N are the radius of curvature of the meridian circle and the unitary circle where the projectile is located;
  • L Is the latitude of the point where the projectile is located, ⁇ is the longitude of the point where the projectile is located, h is the height of the point where the projectile is located;
  • ⁇ V E , ⁇ V N , and ⁇ V U are the velocity error parameters of the rotating projectile, and ⁇ h, ⁇ , and ⁇ L are the position error parameters.
  • the quaternion error ⁇ Q, velocity error ⁇ v and position error ⁇ p of the rotating projectile, the gyro drift ⁇ b , and the accelerometer bias are selected as the state variables of the system It can be expressed as
  • the subtraction result of the position and velocity measured by the satellite navigation system and the corresponding position and velocity calculated by the inertial navigation system is selected as the observation variable Z(t) of the combined filter system, which is expressed as:
  • the SRUKF filtering algorithm process based on the correction coefficient is as follows:
  • the UKF filter algorithm calculates the specific steps of a cycle:
  • qr ⁇ means orthogonal triangulation of the matrix of the matrix, and
  • the table is the return value R after QR decomposition;
  • the present invention adopts a high-precision combined filter structure of the missile's flight attitude based on magnetic measurement roll angle information suitable for the attitude measurement scheme.
  • the combined filter is composed of a roll angle rate estimation filter (EKF) and a high missile flight attitude.
  • the precision filter (SRUKF) consists of the estimation of the roll rate of the projectile and the high-precision estimation of the flight attitude of the projectile.
  • the present invention adopts a high-order non-linear filtering model of a high-precision projectile body suitable for a rotating projectile with a large error angle state.
  • the filter state equation mainly includes an additive quaternion error model to describe the attitude error model of the rotating projectile in the state of large error angle, and a velocity error model and position error model to describe the rotating projectile based on the large error angle.
  • the position and velocity of the satellite navigation system measurement output and the position and velocity subtraction result of the inertial navigation solution are selected as the observation of the combined filter system.
  • the high-order filter model of the high-precision projectile attitude is formed by the above state equation and observation equation.
  • the invention adopts a high-order filtering model of the body attitude to describe the characteristics of its nonlinear system more accurately, and can improve the accuracy of the three-dimensional attitude parameter estimation of the body.
  • the present invention adopts the SRUKF body attitude filtering estimation algorithm based on the correction coefficient, which is used to complete the high-precision filtering estimation of the flying attitude of the rotating missile.
  • the SRUKF filter estimation algorithm based on the correction coefficient is different from the conventional SRUKF filter method in that there is an additional correction coefficient ⁇ in the sigma point calculation, and its size must be added to the selection and determination through a priori knowledge.
  • the improved correction coefficient SRUKF filter algorithm The problem of convergence and convergence will be better suppressed, while also taking into account the real-time performance of the estimation algorithm and the accuracy of the filter estimation.
  • Fig. 1 shows a schematic diagram of the installation method of the bomb-mounted sensor.
  • FIG. 2 shows a schematic diagram of a posture combination filtering structure of magnetic measurement roll angle information.
  • a high-precision estimation method for the flying attitude of a rotating projectile based on magnetic measurement of roll angular rate information includes the following steps:
  • the rotating projectile attitude measurement system adopts a combined geomagnetic/inertial/satellite solution.
  • the onboard sensors mainly include three-axis geomagnetic sensors, two single-axis gyroscopes and satellite receivers. The strapdown installation of each sensor is shown in Figure 1.
  • the geomagnetic sensor is used to measure the geomagnetic field vector information in the projectile.
  • the directions of its sensitive axes (Mx, My, and Mz) are completely consistent with the directions of the axes of the projectile coordinate system (OX b Y b Z b ); two single-axis gyros
  • the gyroscopes (Gy and Gz) are installed on the Y b and Z b axes respectively.
  • the gyroscope is used to measure the Y and Z angular rate information of the projectile.
  • the X axial angular rate information needs to be estimated by filtering the geomagnetic sensor measurement information.
  • the satellite receiver is used to measure the speed and position information of the projectile, and the receiver antenna is installed on the surface of the projectile in a loop.
  • the high-precision combined filter structure of the missile's flight attitude based on the magnetic roll angle information is shown in Figure 2.
  • the combined filter is composed of two roll angle rate estimation filters (EKF) and a high-resolution missile flight attitude filter (SRUKF). It is used to estimate the roll rate of the projectile and the high-precision estimation of the flight attitude parameters of the projectile, respectively.
  • Design of high-precision filter for missile flight attitude 1) Select the missile attitude angle error, velocity error and position error model and inertial device error model to construct the state equation of the combined filter system, in which the additive quaternion error model is used to describe Rotating projectile error model; using large error angle model to describe rotating projectile velocity error model and position error model.
  • the high-precision filter of the missile's flight attitude adopts a correction coefficient SRUUF filter algorithm to complete the real-time high-precision estimation of the missile's flight attitude parameters.
  • the algorithm takes into account the state parameter convergence speed and estimation accuracy.
  • the inertial navigation system itself is non-linear, especially if the gyroscope is not installed on the X axis of the elastic axis, the angular rate in the X axis is estimated using geomagnetic information, but the angular rate estimation accuracy is not high. If the lower accuracy is used again When the combined measurement scheme of the inertial device is used, the nonlinearity of the system is more obvious. If the existing error model based on the small misalignment angle assumption is used, the filter model ignoring the higher-order terms cannot accurately describe the rotating elastic system. Non-linear characteristics, these will directly affect the convergence speed and filtering accuracy of the designed body attitude filter, and even the filter is open.
  • the present invention uses an additive quaternion error model to describe the flying attitude error model of the rotating missile, which can more accurately describe the characteristics of its nonlinear system, so as to improve the accuracy of the three-dimensional attitude parameter estimation of the projectile.
  • the attitude quaternion from the body coordinate system to the navigation coordinate system The differential equation of can be expressed as:
  • the above equation (1) is the differential equation applicable to the update of the attitude quaternion under any angle.
  • attitude error propagation characteristic is a model of the attitude error of the projectile that is suitable for a large error angle.
  • the velocity error equation of the projectile can be derived as:
  • the available body attitude transformation matrix is:
  • the velocity error equation is a nonlinear error equation, where The term is its nonlinear part. If the nonlinear part in the velocity error equation (14) is assumed to be f 1 (x, t):
  • the comprehensive equations (14) and (18) can be used to accurately describe the transmission law of the projectile speed error under the condition of large misalignment error angle, and it is a kind of projectile speed error applicable to the state of large error angle model.
  • the body position error equation is:
  • V E , V N , and V U are the velocity of the projectile in the east, north, and sky directions;
  • R M and R N are the radius of curvature of the meridian circle and the unitary circle where the projectile is located;
  • L Is the latitude of the point where the projectile is located, ⁇ is the longitude of the point where the projectile is located, h is the height of the point where the projectile is located;
  • ⁇ V E , ⁇ V N , and ⁇ V U are the velocity error parameters of the rotating projectile, and ⁇ h, ⁇ , and ⁇ L are the position error parameters.
  • the quaternion error ⁇ Q, velocity error ⁇ v and position error ⁇ p of the rotating projectile, gyro drift ⁇ b and accelerometer bias are selected as the state variables of the system It can be expressed as
  • the above-mentioned high-precision filtering model of the rotating projectile attitude is a strong nonlinear equation system.
  • the filtering methods such as UKF and SRUKF based on the nonlinear function probability density distribution can effectively avoid the model error caused by the approximation of the nonlinear equation.
  • the problem of filtering accuracy is prone to state covariance matrix P losing positive definiteness, resulting in filtering divergence.
  • the present invention adopts a SRUKF body attitude filtering algorithm based on correction coefficients to improve the convergence speed and parameter estimation accuracy of the filtering algorithm.
  • the SRUKF filtering algorithm process based on the correction coefficient is as follows:
  • the UKF filter algorithm calculates the specific steps of a cycle:
  • qr ⁇ means to perform orthogonal triangulation (QR decomposition) of the matrix of the matrix, and
  • the table is the return value R after QR decomposition;
  • the above-mentioned modified coefficient SRUKF filter estimation algorithm is different from the conventional SRUKF filter method in the calculation of sigma points.
  • the sigma point calculation formula (28) there is an additional correction coefficient ⁇ , and its size must be added to the selection through prior knowledge. . Since the correction coefficient satisfies ⁇ >1, the sigma point after time update Error variance S k, k-1 and the predicted value in advance The error variance S zk will increase, but the observation noise variance matrix R k will not change.
  • the measurement correction gain K k will also increase, which means that the weight of the new measurement value is added Large, which reduces the impact of stale measurement information on the estimated value, so the problem of open convergence of the improved correction coefficient SRUKF filter algorithm will be better suppressed.

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Abstract

With respect to the problem in which "three highs," namely high overloading, high self-spinning, and high dynamic, of a rotary shell launch restrict an existing mature shell-mounted posture measurement system from being directly migrated for application to a rotary shell, employed is a rotary shell flight posture measurement solution consisting of a triaxial geomagnetic sensor, two monoaxial gyroscopes, and a satellite receiver. With respect to the measurement solution, provided is a high-precision filter estimation method applicable for rotary shell flight posture, comprising the following steps: (1) a rotary shell flight posture combined measurement, comprising 1.1, a shell-mounted sensor and a mounting scheme and 1.2, a shell flight posture high-precision combined filter structure; (2) a rotary shell high-precision offset model, comprising 2.1, a rotary shell posture offset model, 2.2, a rotary shell speed offset model, and 2.3, a position offset equation; (3) a shell body posture high-order nonlinear filter model; and (4) a shell posture high-precision real-time filtering algorithm for a filter updating process.

Description

基于磁测滚转角速率信息的旋转弹飞行姿态高精度估计方法High-precision estimation method for flying attitude of rotating projectile based on information of magnetic measurement roll angle rate 技术领域Technical field
本发明涉及飞行器或者弹体空间三维姿态的测量方法,具体为一种适用于的旋转弹飞行姿态高精度测量方法。The invention relates to a method for measuring the three-dimensional attitude of an aircraft or a missile space, in particular to a high-precision method for measuring the flying attitude of a rotating bomb.
背景技术Background technique
由于旋转弹发射高过载、高自旋转和高动态的“三高”特殊的弹载应用环境,现有成熟的弹载姿态测量系统无法直接移植应用于旋转弹药,存在可靠性差、飞行三维姿态参数测试不全或测量精度较低等问题。为解决上述问题,目前通常采用INS+GPS组合、地磁+GPS或地磁+INS+GPS等组合测量方案,并采用相应滤波算法完成弹体飞行姿态参数的估计,但所采用滤波器结构、滤波模型或滤波算法等存在一定的局限性,所设计滤波器的收敛性、实时性以及估计精度不理想。比如采用现有基于小失准误差角假设的姿态滤波模型,其忽略了高阶项的滤波模型并不能精确地描述旋转弹系统的强非线性特性,这些将直接影响到所设计弹体姿态滤波器的收敛速度与滤波精度,甚至滤波发散等问题,也会造成滤波器大误差参数估计结果。Due to the "three high" special bomb-loading application environment of high overload, high self-rotation and high dynamics of rotating bombs, the existing mature bomb-borne attitude measurement system cannot be directly transplanted to rotating ammunition, which has poor reliability and flight three-dimensional attitude parameters Problems such as incomplete testing or low measurement accuracy. In order to solve the above problems, currently combined measurement schemes such as INS+GPS combination, geomagnetism+GPS or geomagnetism+INS+GPS are used, and the corresponding filter algorithm is used to complete the estimation of the flight attitude parameters of the projectile, but the filter structure and filter model used Or filtering algorithm, etc. have certain limitations, the convergence, real-time performance and estimation accuracy of the designed filter are not ideal. For example, the existing attitude filter model based on the assumption of small misalignment error angle, which ignores the high-order filter model and cannot accurately describe the strong nonlinear characteristics of the rotating projectile system, these will directly affect the design of the projectile attitude filter Problems such as the convergence speed and filter accuracy of the filter, and even the filter divergence, can also cause the large error parameter estimation results of the filter.
因此,寻求一种适用于旋转弹飞行姿态高精度测量方法,对解决旋转弹制导化改造中飞行姿态测量难题具有重要的理论价值与现实意义。Therefore, it is of great theoretical value and practical significance to find a high-precision measurement method suitable for the rotational attitude of the rotating missile, which is of great theoretical value and practical significance in solving the difficult problem of the flying attitude measurement in the guidance and transformation of the rotating missile.
发明内容Summary of the invention
本发明针对旋转弹发射高过载、高自旋转和高动态的“三高”限制了现有成熟的弹载姿态测量系统无法直接移植应用于旋转弹的问题,采用了基于三轴地磁传感器、两个单轴陀螺仪和卫星接收机组成旋转弹飞行姿态测量方案,针对该测量方案提出了一种适用于旋转弹飞行姿态高精度滤波估计方法。The present invention addresses the problem that the "three heights" of high overload, high self-rotation and high dynamics of the launch of the rotating bomb limit the existing mature bomb-borne attitude measurement system and cannot be directly transplanted to the rotating bomb. A single-axis gyroscope and a satellite receiver form a rotating missile flight attitude measurement scheme, and a high-precision filtering estimation method suitable for the rotating bomb flight attitude is proposed for this measurement scheme.
本发明是采用如下技术方案实现的:The present invention is implemented using the following technical solution:
一种基于磁测滚转角速率信息的旋转弹飞行姿态高精度估计方法,包括如下步骤:A high-precision estimation method for the flying attitude of a rotating projectile based on magnetic measurement of roll angular rate includes the following steps:
(1)、旋转弹飞行姿态组合测量(1) Combined measurement of the flying attitude of the rotating bomb
1.1、弹载传感器及安装方式1.1, bomb-mounted sensor and installation method
弹载传感器采用三轴地磁传感器、两个单轴陀螺仪和卫星接收机,其中,三轴地磁传感器用于测量弹体内的地磁场矢量信息,其各敏感轴方向Mx、My和Mz与弹体坐标系OX bY bZ b各轴方向完全一致;两个单轴陀螺仪Gy和Gz分别捷联安装于Y b和Z b轴上,陀螺仪用于测量弹体Y轴和Z轴角速率信息,X轴向角速率信息由地磁传感器测量信息滤波估算得到;卫星接收机用于测量弹体速度和位置信息,接收机天线环形安装于弹体表面。 The bomb-mounted sensor uses a three-axis geomagnetic sensor, two single-axis gyroscopes and a satellite receiver. Among them, the three-axis geomagnetic sensor is used to measure the vector information of the geomagnetic field inside the projectile. The directions of each sensitive axis Mx, My and Mz and the projectile The coordinate system OX b Y b Z b has the same direction of each axis; two single-axis gyroscopes Gy and Gz are respectively installed on the Y b and Z b axes, and the gyroscopes are used to measure the Y-axis and Z-axis angular rates of the projectile Information, the X-axis angular rate information is estimated by filtering the geomagnetic sensor measurement information; the satellite receiver is used to measure the velocity and position information of the projectile, and the receiver antenna is installed on the surface of the projectile in a loop.
1.2、弹体飞行姿态高精度组合滤波结构1.2. High-precision combined filter structure for missile flight attitude
组合滤波器由滚转角速率估计滤波器和弹体飞行姿态高精度滤波器两个滤波器组成,分别用于完成弹体滚转速率的估计和弹体飞行姿态参数的高精度估计。The combined filter is composed of two filters, a roll angle rate estimation filter and a high-precision filter for the flight attitude of the projectile, which are used to estimate the roll rate of the projectile and the high-precision estimation of the flight attitude of the projectile, respectively.
(2)、旋转弹高精度误差模型(2), high-precision error model of rotating bomb
根据捷联惯性导航理论,弹体坐标系到导航坐标系的姿态四元数
Figure PCTCN2019121491-appb-000001
的微分方程表示为:
According to the strapdown inertial navigation theory, the attitude quaternion from the body coordinate system to the navigation coordinate system
Figure PCTCN2019121491-appb-000001
The differential equation of is expressed as:
Figure PCTCN2019121491-appb-000002
Figure PCTCN2019121491-appb-000002
上式中,
Figure PCTCN2019121491-appb-000003
为四元数矩阵,是反对阵矩阵形式:
In the above formula,
Figure PCTCN2019121491-appb-000003
It is a quaternion matrix, which is in the form of an anti-matrix matrix:
Figure PCTCN2019121491-appb-000004
Figure PCTCN2019121491-appb-000004
其中,
Figure PCTCN2019121491-appb-000005
为弹体坐标系相对于惯性坐标系的角速度在弹体坐标系上的投影分量
Figure PCTCN2019121491-appb-000006
Figure PCTCN2019121491-appb-000007
即为导航坐标系相对与惯性坐标系的角速度在导航坐标系上的投影分量
Figure PCTCN2019121491-appb-000008
Figure PCTCN2019121491-appb-000009
为导航坐标系相对与惯性坐标系的角速度在载体坐标系上的投影分量。
among them,
Figure PCTCN2019121491-appb-000005
Is the projected component of the angular velocity of the projectile coordinate system relative to the inertial coordinate system on the projectile coordinate system
Figure PCTCN2019121491-appb-000006
Figure PCTCN2019121491-appb-000007
It is the projection component of the angular velocity of the navigation coordinate system relative to the inertial coordinate system on the navigation coordinate system
Figure PCTCN2019121491-appb-000008
Figure PCTCN2019121491-appb-000009
It is the projection component of the angular velocity of the navigation coordinate system relative to the inertial coordinate system on the carrier coordinate system.
Figure PCTCN2019121491-appb-000010
Figure PCTCN2019121491-appb-000011
分别表示为:
Figure PCTCN2019121491-appb-000010
with
Figure PCTCN2019121491-appb-000011
Represented as:
Figure PCTCN2019121491-appb-000012
Figure PCTCN2019121491-appb-000012
由于角速率分量
Figure PCTCN2019121491-appb-000013
是通过传感器测量所得,其测量值
Figure PCTCN2019121491-appb-000014
必然存在测量误差
Figure PCTCN2019121491-appb-000015
其表示为:
Due to angular rate component
Figure PCTCN2019121491-appb-000013
It is measured by the sensor and its measured value
Figure PCTCN2019121491-appb-000014
There must be measurement error
Figure PCTCN2019121491-appb-000015
It is expressed as:
Figure PCTCN2019121491-appb-000016
Figure PCTCN2019121491-appb-000016
捷联解算所得到的角速度
Figure PCTCN2019121491-appb-000017
也存在解算误差,其表示为:
The angular velocity obtained by the strapdown solution
Figure PCTCN2019121491-appb-000017
There is also a solution error, which is expressed as:
Figure PCTCN2019121491-appb-000018
Figure PCTCN2019121491-appb-000018
把上式(3)和(4)代入姿态四元数微分方程(1),得到实际解算时的姿态四元数更微分方程为:Substituting the above equations (3) and (4) into the attitude quaternion differential equation (1), the more differential equation of the attitude quaternion when the actual solution is obtained is:
Figure PCTCN2019121491-appb-000019
Figure PCTCN2019121491-appb-000019
因此,把式(5)减去式(1)得到如下形式:Therefore, subtracting equation (1) from equation (5) yields the following form:
Figure PCTCN2019121491-appb-000020
Figure PCTCN2019121491-appb-000020
Figure PCTCN2019121491-appb-000021
则得到姿态四元数误差方程为:
make
Figure PCTCN2019121491-appb-000021
Then the error equation of the attitude quaternion is:
Figure PCTCN2019121491-appb-000022
Figure PCTCN2019121491-appb-000022
上式(7)中最后两项表达式满足如下关系:The last two expressions in the above formula (7) satisfy the following relationship:
Figure PCTCN2019121491-appb-000023
Figure PCTCN2019121491-appb-000023
其中,
Figure PCTCN2019121491-appb-000024
Figure PCTCN2019121491-appb-000025
分别定义为:
among them,
Figure PCTCN2019121491-appb-000024
with
Figure PCTCN2019121491-appb-000025
They are defined as:
Figure PCTCN2019121491-appb-000026
Figure PCTCN2019121491-appb-000026
Figure PCTCN2019121491-appb-000027
Figure PCTCN2019121491-appb-000027
上式
Figure PCTCN2019121491-appb-000028
Figure PCTCN2019121491-appb-000029
中,满足如下关系:
The above formula
Figure PCTCN2019121491-appb-000028
with
Figure PCTCN2019121491-appb-000029
In, satisfy the following relationship:
Figure PCTCN2019121491-appb-000030
Figure PCTCN2019121491-appb-000030
把上式关系代入(7),得姿态四元数误差方程式:Substituting the above relationship into (7), the attitude quaternion error equation is obtained:
Figure PCTCN2019121491-appb-000031
Figure PCTCN2019121491-appb-000031
2.2、旋转弹速度误差模型2.2. Rotating bomb speed error model
由比力方程推导出弹体速度误差方程为:The velocity error equation derived from the specific force equation is:
Figure PCTCN2019121491-appb-000032
Figure PCTCN2019121491-appb-000032
上式中,
Figure PCTCN2019121491-appb-000033
为姿态变换矩阵的计算误差,由于
Figure PCTCN2019121491-appb-000034
是关于四元数误差
Figure PCTCN2019121491-appb-000035
的非线性函数,所以
Figure PCTCN2019121491-appb-000036
也是关于
Figure PCTCN2019121491-appb-000037
的非线性函数;
Figure PCTCN2019121491-appb-000038
为加速度计在导航系下的 等效零偏,满足
Figure PCTCN2019121491-appb-000039
δK A和δA分别为加速度计的刻度系数误差矩阵和安装误差矩阵;V n为导航系下速度分量;δV n为速度误差;
Figure PCTCN2019121491-appb-000040
地球自转角速度;
Figure PCTCN2019121491-appb-000041
地球自转角速度误差;
Figure PCTCN2019121491-appb-000042
为导航坐标系相对地球的角速;
Figure PCTCN2019121491-appb-000043
为导航坐标系相对地球的角速误差;f b为加速度计比力。
In the above formula,
Figure PCTCN2019121491-appb-000033
Is the calculation error of the attitude transformation matrix, because
Figure PCTCN2019121491-appb-000034
Is about quaternion error
Figure PCTCN2019121491-appb-000035
Nonlinear function, so
Figure PCTCN2019121491-appb-000036
Also about
Figure PCTCN2019121491-appb-000037
Nonlinear function
Figure PCTCN2019121491-appb-000038
Is the equivalent zero offset of the accelerometer under the navigation system, satisfying
Figure PCTCN2019121491-appb-000039
δK A and δA are respectively the scale factor error matrix and the installation error matrix of the accelerometer; V n is the speed component under the navigation system; δ V n is the speed error;
Figure PCTCN2019121491-appb-000040
Earth's rotation angular velocity;
Figure PCTCN2019121491-appb-000041
Earth rotation angular velocity error;
Figure PCTCN2019121491-appb-000042
The angular velocity of the navigation coordinate system relative to the earth;
Figure PCTCN2019121491-appb-000043
Is the angular velocity error of the navigation coordinate system relative to the earth; f b is the accelerometer specific force.
若加速度计事前经校准后,可不考虑δK A和δA,则弹体速度误差方程为: If the accelerometer is calibrated beforehand, δK A and δA can be disregarded, then the body velocity error equation is:
Figure PCTCN2019121491-appb-000044
Figure PCTCN2019121491-appb-000044
根据上述式(11)所述转换关系,得弹体姿态变换矩阵有:According to the conversion relationship described in the above formula (11), the obtained body attitude transformation matrix is:
Figure PCTCN2019121491-appb-000045
Figure PCTCN2019121491-appb-000045
因此,姿态变换矩阵的计算误差
Figure PCTCN2019121491-appb-000046
为:
Therefore, the calculation error of the attitude transformation matrix
Figure PCTCN2019121491-appb-000046
for:
Figure PCTCN2019121491-appb-000047
Figure PCTCN2019121491-appb-000047
如前所述,
Figure PCTCN2019121491-appb-000048
代入上式(16)得到
Figure PCTCN2019121491-appb-000049
As mentioned before,
Figure PCTCN2019121491-appb-000048
Substitute into the above formula (16) to get
Figure PCTCN2019121491-appb-000049
Figure PCTCN2019121491-appb-000050
Figure PCTCN2019121491-appb-000050
又由于
Figure PCTCN2019121491-appb-000051
Figure PCTCN2019121491-appb-000052
简化为:
Again
Figure PCTCN2019121491-appb-000051
then
Figure PCTCN2019121491-appb-000052
Simplified to:
Figure PCTCN2019121491-appb-000053
Figure PCTCN2019121491-appb-000053
当姿态角误差较大时,
Figure PCTCN2019121491-appb-000054
Figure PCTCN2019121491-appb-000055
是非线性的,其中
Figure PCTCN2019121491-appb-000056
的计算公式为:
When the attitude angle error is large,
Figure PCTCN2019121491-appb-000054
Correct
Figure PCTCN2019121491-appb-000055
Is nonlinear, where
Figure PCTCN2019121491-appb-000056
The calculation formula is:
Figure PCTCN2019121491-appb-000057
Figure PCTCN2019121491-appb-000057
由上述的推导关系可知,速度误差方程体现出是一个非线性的误差方程,其中
Figure PCTCN2019121491-appb-000058
项即为其非线性部分,若假设速度误差方程(14)中非线性部分为f 1(x,t):
From the above derivation, we can see that the velocity error equation is a nonlinear error equation, where
Figure PCTCN2019121491-appb-000058
The term is its nonlinear part. If the nonlinear part in the velocity error equation (14) is assumed to be f 1 (x, t):
Figure PCTCN2019121491-appb-000059
Figure PCTCN2019121491-appb-000059
在对非线性的速度误差方程进行线性化处理时,f 1(x,t)对
Figure PCTCN2019121491-appb-000060
的雅克比矩阵公式为:
When linearizing the nonlinear velocity error equation, f 1 (x, t) is
Figure PCTCN2019121491-appb-000060
The formula of the Jacobian matrix is:
Figure PCTCN2019121491-appb-000061
Figure PCTCN2019121491-appb-000061
上式δu i(i=1,2,3,4)表示
Figure PCTCN2019121491-appb-000062
的第i行,其中,
Figure PCTCN2019121491-appb-000063
Figure PCTCN2019121491-appb-000064
分别定义为:
The above formula δu i (i=1, 2, 3, 4) represents
Figure PCTCN2019121491-appb-000062
The i-th line, where,
Figure PCTCN2019121491-appb-000063
with
Figure PCTCN2019121491-appb-000064
They are defined as:
Figure PCTCN2019121491-appb-000065
Figure PCTCN2019121491-appb-000065
因此,综合方程(14)和(18)用于准确的描述弹体在大失准误差角情况下的弹体速度误差传规律,是一种适用于大误差角状态下的弹体速度误差模型。Therefore, the comprehensive equations (14) and (18) are used to accurately describe the transmission law of the projectile velocity error in the case of large misalignment error angle, and it is a model of projectile velocity error applicable to the state of large error angle. .
2.3、位置误差方程2.3. Position error equation
弹体位置误差方程为:The body position error equation is:
Figure PCTCN2019121491-appb-000066
Figure PCTCN2019121491-appb-000066
式(24)中,V E、V N、V U分别为弹体沿东、北、天方向的速度;R M和R N分别为弹体所在点子午圈和卯酉圈的曲率半径;L为弹体所在点纬度,λ为弹体所在点经度,h为弹体所在点的高度;δV E,δV N,δV U为旋转弹速度误差参数,δh,δλ和δL为位置误差参数。 In equation (24), V E , V N , and V U are the velocity of the projectile in the east, north, and sky directions; R M and R N are the radius of curvature of the meridian circle and the unitary circle where the projectile is located; L Is the latitude of the point where the projectile is located, λ is the longitude of the point where the projectile is located, h is the height of the point where the projectile is located; δV E , δV N , and δV U are the velocity error parameters of the rotating projectile, and δh, δλ, and δL are the position error parameters.
(3)、弹体姿态高阶非线性滤波模型(3) High-order nonlinear filtering model of projectile attitude
选取旋转弹姿态四元数误差δQ、速度误差δv和位置误差δp以及陀螺漂移ε b、加速度计零偏作为系统的状态变量
Figure PCTCN2019121491-appb-000067
其可表示为
The quaternion error δQ, velocity error δv and position error δp of the rotating projectile, the gyro drift ε b , and the accelerometer bias are selected as the state variables of the system
Figure PCTCN2019121491-appb-000067
It can be expressed as
Figure PCTCN2019121491-appb-000068
Figure PCTCN2019121491-appb-000068
选取上述推导所得弹体飞行姿态误差方程(12)、速度误差方程(14)和位置误差方程(24)共同构成了滤波器状态方程组,将其简化为如下一般形式:The flight attitude error equation (12), velocity error equation (14) and position error equation (24) obtained by the above derivation form the filter state equation group, which is simplified to the following general form:
Figure PCTCN2019121491-appb-000069
Figure PCTCN2019121491-appb-000069
上式中f[X(t),t]是关于自变量X(t)的非线性函数,系统过程白噪声w(t)满足E[w(t)]=0和E[w(t),w T(τ)]=Q(t)δ(t-τ); In the above formula, f[X(t), t] is a nonlinear function about the independent variable X(t), and the system process white noise w(t) satisfies E[w(t)]=0 and E[w(t) , W T (τ)] = Q(t)δ(t-τ);
选取卫星导航系统测量输出的位置和速度与惯导相应解算的位置和速度相减结果作为组合滤波系统的观测变量Z(t),其表示为:The subtraction result of the position and velocity measured by the satellite navigation system and the corresponding position and velocity calculated by the inertial navigation system is selected as the observation variable Z(t) of the combined filter system, which is expressed as:
Figure PCTCN2019121491-appb-000070
Figure PCTCN2019121491-appb-000070
上式中L GPS,λ GPS,h GPS和v i,GPS(i=N,E,U)分别表示为卫星导航系统测量输出的位置和速度信息,下标为INS变量表示为惯导解算的位置和速度信息;量测噪声v(t)满足E[v(t)]=0和E[v(t),v T(τ)]=R(t)δ(t-τ); In the above formula, L GPS , λ GPS , h GPS and v i, GPS (i=N, E, U) represent the position and speed information measured and output by the satellite navigation system, respectively, and the subscript is the INS variable, which represents the inertial navigation solution. Position and velocity information; measurement noise v(t) satisfies E[v(t)]=0 and E[v(t), v T (τ)]=R(t)δ(t-τ);
因此,综合上述状态方程(25)和量测方程(26)共同构成了适用于大误差角状态下的弹体姿态高阶非线性滤波模型。Therefore, the above-mentioned state equation (25) and measurement equation (26) are combined to form a high-order nonlinear filtering model for the attitude of the projectile in the state of large error angle.
(4)、弹体姿态高精度实时滤波算法(4) High-precision real-time filtering algorithm for projectile attitude
基于修正系数的SRUKF滤波算法流程如下:The SRUKF filtering algorithm process based on the correction coefficient is as follows:
4.1、滤波初始化:4.1, filter initialization:
Figure PCTCN2019121491-appb-000071
Figure PCTCN2019121491-appb-000071
对于任一时段UKF滤波算法计算一个循环的具体步骤:For any period of time, the UKF filter algorithm calculates the specific steps of a cycle:
4.2、对于给定的
Figure PCTCN2019121491-appb-000072
和P k-1(k=0,2,...n),首先计算状态一步预测
Figure PCTCN2019121491-appb-000073
及一步预报误差协方差阵P k,k-1,包括sigma点计算及其传播过程:
4.2. For a given
Figure PCTCN2019121491-appb-000072
And P k-1 (k = 0, 2, ... n), first calculate the state and predict one step
Figure PCTCN2019121491-appb-000073
And one-step forecast error covariance matrix P k,k-1 , including sigma point calculation and its propagation process:
4.2.1、计算sigma点
Figure PCTCN2019121491-appb-000074
即为:
4.2.1. Calculate sigma points
Figure PCTCN2019121491-appb-000074
That is:
Figure PCTCN2019121491-appb-000075
Figure PCTCN2019121491-appb-000075
4.2.2、计算
Figure PCTCN2019121491-appb-000076
通过状态方程f(·)传播的sigma点,即为:
4.2.2, calculation
Figure PCTCN2019121491-appb-000076
The sigma point propagating through the state equation f(·) is:
Figure PCTCN2019121491-appb-000077
Figure PCTCN2019121491-appb-000077
上式中qr{·}表示对其矩阵进行矩阵的正交三角分解,而
Figure PCTCN2019121491-appb-000078
表为其QR分解后的返回值R;公式S′=cholupdate{S,u,±v}是等价于SS T=P,S′=chol{P±vuu T};
In the above formula, qr{·} means orthogonal triangulation of the matrix of the matrix, and
Figure PCTCN2019121491-appb-000078
The table is the return value R after QR decomposition; the formula S′=cholupdate{S,u,±v} is equivalent to SS T =P, S′=chol{P±vuu T };
4.3、利用UT变换,求sigma点
Figure PCTCN2019121491-appb-000079
和P k,k-1通过量测方程的传播,包括如下两更新计算过程:
4.3. Use UT transform to find sigma points
Figure PCTCN2019121491-appb-000079
Propagation of P k,k-1 through the measurement equation includes the following two update calculation processes:
4.3.1、首先,计算sigma点
Figure PCTCN2019121491-appb-000080
和P k,k-1通过量测方程h(·)的对X k的传播:
4.3.1. First, calculate the sigma point
Figure PCTCN2019121491-appb-000080
And P k,k-1 by measuring the propagation of equation h(·) to X k :
Figure PCTCN2019121491-appb-000081
Figure PCTCN2019121491-appb-000081
4.3.2、然后,计算输出的一步提前预测值:4.3.2 Then, calculate the output one-step forecast value in advance:
Figure PCTCN2019121491-appb-000082
Figure PCTCN2019121491-appb-000082
4.4、最后,利用得到的新的量测值,进行滤波更新过程:4.4. Finally, use the new measured values to perform the filter update process:
Figure PCTCN2019121491-appb-000083
Figure PCTCN2019121491-appb-000083
本发明方案具有如下优点:The solution of the present invention has the following advantages:
1、本发明采用了适用于该姿态测量方案的基于磁测滚转角信息的弹体飞行姿态高精度组合滤波结构,该组合滤波器由滚转角速率估计滤波器(EKF)和弹体飞行姿态高精度滤波器(SRUKF)组成,分别用于完成弹体滚转速率的估计和弹体飞行姿态高精度估计。1. The present invention adopts a high-precision combined filter structure of the missile's flight attitude based on magnetic measurement roll angle information suitable for the attitude measurement scheme. The combined filter is composed of a roll angle rate estimation filter (EKF) and a high missile flight attitude. The precision filter (SRUKF) consists of the estimation of the roll rate of the projectile and the high-precision estimation of the flight attitude of the projectile.
2、本发明采用了适用于大误差角状态的旋转弹用高精度弹体姿态高阶非线性滤波模型。滤波状态方程主要包括采用加性四元数误差模型来描述大误差角状态下旋转弹姿态误差模型、采用基于大误差角来描述旋转弹速度误差模型和位置误差模型。选取卫星导航系统测量输出的位置和速度与惯导解算的位置和速度相减结果作为组合滤波系统的观测量,由上述状态方程和观测方程共同构成高精度弹体姿态高阶滤波模型。本发明采用弹体姿态高阶滤波模型可以更准确地描述其非线性系统的特性,可以提高弹体三维姿态参数估计的精度。2. The present invention adopts a high-order non-linear filtering model of a high-precision projectile body suitable for a rotating projectile with a large error angle state. The filter state equation mainly includes an additive quaternion error model to describe the attitude error model of the rotating projectile in the state of large error angle, and a velocity error model and position error model to describe the rotating projectile based on the large error angle. The position and velocity of the satellite navigation system measurement output and the position and velocity subtraction result of the inertial navigation solution are selected as the observation of the combined filter system. The high-order filter model of the high-precision projectile attitude is formed by the above state equation and observation equation. The invention adopts a high-order filtering model of the body attitude to describe the characteristics of its nonlinear system more accurately, and can improve the accuracy of the three-dimensional attitude parameter estimation of the body.
3、本发明采用了基于修正系数的SRUKF弹体姿态滤波估计算法,用于完成旋转弹飞行姿态高精度滤波估计。基于修正系数的SRUKF滤波估计算法与常规SRUKF滤波方法不同之处在于sigma点计算中多了一项修正系数μ,其大小必须通过先验知识来加于选择确定,改进后的修正系数SRUKF滤波算法的收敛发敞的问题将得到较好的抑制,同时也兼顾估计算法的实时性与滤波估计精度。3. The present invention adopts the SRUKF body attitude filtering estimation algorithm based on the correction coefficient, which is used to complete the high-precision filtering estimation of the flying attitude of the rotating missile. The SRUKF filter estimation algorithm based on the correction coefficient is different from the conventional SRUKF filter method in that there is an additional correction coefficient μ in the sigma point calculation, and its size must be added to the selection and determination through a priori knowledge. The improved correction coefficient SRUKF filter algorithm The problem of convergence and convergence will be better suppressed, while also taking into account the real-time performance of the estimation algorithm and the accuracy of the filter estimation.
附图说明BRIEF DESCRIPTION
图1表示弹载传感器安装方式示意图。Fig. 1 shows a schematic diagram of the installation method of the bomb-mounted sensor.
图2表示磁测滚转角信息的姿态组合滤波结构示意图。FIG. 2 shows a schematic diagram of a posture combination filtering structure of magnetic measurement roll angle information.
具体实施方式detailed description
下面结合附图对本发明的具体实施例进行详细说明。The specific embodiments of the present invention will be described in detail below with reference to the drawings.
一种基于磁测滚转角速率信息的旋转弹飞行姿态高精度估计方法,包括如下步骤:A high-precision estimation method for the flying attitude of a rotating projectile based on magnetic measurement of roll angular rate information includes the following steps:
1、旋转弹飞行姿态组合测量方案1. The combined measurement scheme of the flying attitude of the rotating bomb
1.1、弹载传感器及安装方式1.1, bomb-mounted sensor and installation method
旋转弹姿态测量系统采用地磁/惯性/卫星组合方案,弹载传感器主要有三轴地磁传感器、两个单轴陀螺仪和卫星接收机,各传感器捷联安装方式如图1所示。地磁传感器的用于测量弹体内的地磁场矢量信息,其各敏感轴方向(Mx、My和Mz)与弹体坐标系(OX bY bZ b)各轴方向完全一致;两个单轴陀螺仪(Gy和Gz)分别捷联安装于Y b和Z b轴上,陀螺仪用于测量弹体Y轴和Z轴角速率信息,X轴向角速率信息需要由地磁传感器测量信息滤波估算得到;卫 星接收机用于测量弹体速度和位置信息,接收机天线环形安装于弹体表面。 The rotating projectile attitude measurement system adopts a combined geomagnetic/inertial/satellite solution. The onboard sensors mainly include three-axis geomagnetic sensors, two single-axis gyroscopes and satellite receivers. The strapdown installation of each sensor is shown in Figure 1. The geomagnetic sensor is used to measure the geomagnetic field vector information in the projectile. The directions of its sensitive axes (Mx, My, and Mz) are completely consistent with the directions of the axes of the projectile coordinate system (OX b Y b Z b ); two single-axis gyros The gyroscopes (Gy and Gz) are installed on the Y b and Z b axes respectively. The gyroscope is used to measure the Y and Z angular rate information of the projectile. The X axial angular rate information needs to be estimated by filtering the geomagnetic sensor measurement information. The satellite receiver is used to measure the speed and position information of the projectile, and the receiver antenna is installed on the surface of the projectile in a loop.
1.2、弹体飞行姿态高精度组合滤波结构1.2. High-precision combined filter structure for missile flight attitude
基于磁测滚转角信息的弹体飞行姿态高精度组合滤波结构如图2所示,组合滤波器由滚转角速率估计滤波器(EKF)和弹体飞行姿态高精度滤波器(SRUKF)两个滤波器组成,分别用于完成弹体滚转速率的估计和弹体飞行姿态参数的高精度估计。弹体飞行姿态高精度滤波器设计:1)选取弹体姿态角误差、速度误差和位置误差模型以及惯性器件误差模型构建组合滤波系统的状态方程,其中,利用加性四元数误差模型来描述旋转弹姿态误差模型;采用基于大误差角模型来描述旋转弹速度误差模型和位置误差模型。2)选取卫星导航系统测量输出的速度和位置与相对应的捷联惯性解算结果相减作为组合滤波系统的观测量。3)弹体飞行姿态高精度滤波器采用了一种基于修正系数SRUKF滤波算法完成弹体飞行姿态参数的实时高精度估计,该算法兼顾状态参数收敛速度和估计精度问题。The high-precision combined filter structure of the missile's flight attitude based on the magnetic roll angle information is shown in Figure 2. The combined filter is composed of two roll angle rate estimation filters (EKF) and a high-resolution missile flight attitude filter (SRUKF). It is used to estimate the roll rate of the projectile and the high-precision estimation of the flight attitude parameters of the projectile, respectively. Design of high-precision filter for missile flight attitude: 1) Select the missile attitude angle error, velocity error and position error model and inertial device error model to construct the state equation of the combined filter system, in which the additive quaternion error model is used to describe Rotating projectile error model; using large error angle model to describe rotating projectile velocity error model and position error model. 2) Select the speed and position of the measurement output of the satellite navigation system and the corresponding strapdown inertial solution result to be subtracted as the observation of the combined filter system. 3) The high-precision filter of the missile's flight attitude adopts a correction coefficient SRUUF filter algorithm to complete the real-time high-precision estimation of the missile's flight attitude parameters. The algorithm takes into account the state parameter convergence speed and estimation accuracy.
2、旋转弹高精度误差模型2. High precision error model of rotating bomb
2.1、旋转弹姿态误差模型2.1. Rotating projectile error model
考虑到惯性导航系统本身是非线性的,特别是弹轴X轴上没有安装陀螺仪,X轴向角速率是采用地磁信息估算所得,但角速率估计精度并不高,若再采用的较低精度的惯性器件的组合测量方案时,系统的非线性程度更为明显,若采用现有的基于小失准角假设的误差模型,忽略了高阶项的滤波模型并不能精确地描述旋转弹系统的非线性特性,这些将直接影响到所设计弹体姿态滤波器的收敛速度与滤波精度,甚至滤波发敞。因此,本发明采用了基于加性四元数误差模型来描述旋转弹飞行姿态误差模型,可以更准确地描述其非线性系统的特性,以提高弹体三维姿态参数估计的精度。根据捷联惯性导航理论,弹体坐标系到导航坐标系的姿态四元数
Figure PCTCN2019121491-appb-000084
的微分方程可以表示为:
Considering that the inertial navigation system itself is non-linear, especially if the gyroscope is not installed on the X axis of the elastic axis, the angular rate in the X axis is estimated using geomagnetic information, but the angular rate estimation accuracy is not high. If the lower accuracy is used again When the combined measurement scheme of the inertial device is used, the nonlinearity of the system is more obvious. If the existing error model based on the small misalignment angle assumption is used, the filter model ignoring the higher-order terms cannot accurately describe the rotating elastic system. Non-linear characteristics, these will directly affect the convergence speed and filtering accuracy of the designed body attitude filter, and even the filter is open. Therefore, the present invention uses an additive quaternion error model to describe the flying attitude error model of the rotating missile, which can more accurately describe the characteristics of its nonlinear system, so as to improve the accuracy of the three-dimensional attitude parameter estimation of the projectile. According to the strapdown inertial navigation theory, the attitude quaternion from the body coordinate system to the navigation coordinate system
Figure PCTCN2019121491-appb-000084
The differential equation of can be expressed as:
Figure PCTCN2019121491-appb-000085
Figure PCTCN2019121491-appb-000085
上式中,
Figure PCTCN2019121491-appb-000086
为四元数矩阵,是反对阵矩阵形式:
In the above formula,
Figure PCTCN2019121491-appb-000086
It is a quaternion matrix, which is in the form of an anti-matrix matrix:
Figure PCTCN2019121491-appb-000087
Figure PCTCN2019121491-appb-000087
其中,
Figure PCTCN2019121491-appb-000088
为弹体坐标系(b系)相对于惯性坐标系(i系)的角速度在b系上的投影分量
Figure PCTCN2019121491-appb-000089
Figure PCTCN2019121491-appb-000090
即为导航坐标系(n系)相对与惯性坐标系(i系)的角速度在n系上的投影分量
Figure PCTCN2019121491-appb-000091
Figure PCTCN2019121491-appb-000092
为导航坐标系相对与惯性坐标系的角速度在载体坐标系上的投 影分量;
Figure PCTCN2019121491-appb-000093
Figure PCTCN2019121491-appb-000094
分别表示为:
among them,
Figure PCTCN2019121491-appb-000088
Is the projected component of the angular velocity of the body coordinate system (b system) relative to the inertial coordinate system (i system) on the b system
Figure PCTCN2019121491-appb-000089
Figure PCTCN2019121491-appb-000090
That is, the projected component of the angular velocity of the navigation coordinate system (n system) relative to the inertial coordinate system (i system) on the n system
Figure PCTCN2019121491-appb-000091
Figure PCTCN2019121491-appb-000092
The projected component of the angular velocity of the navigation coordinate system relative to the inertial coordinate system on the carrier coordinate system;
Figure PCTCN2019121491-appb-000093
with
Figure PCTCN2019121491-appb-000094
Represented as:
Figure PCTCN2019121491-appb-000095
Figure PCTCN2019121491-appb-000095
上式(1)即为适用于任何角度情况下的姿态四元数更新的微分方程。The above equation (1) is the differential equation applicable to the update of the attitude quaternion under any angle.
由于角速率分量
Figure PCTCN2019121491-appb-000096
是通过传感器测量所得,其测量值
Figure PCTCN2019121491-appb-000097
必然存在测量误差
Figure PCTCN2019121491-appb-000098
其可表示为:
Due to angular rate component
Figure PCTCN2019121491-appb-000096
It is measured by the sensor and its measured value
Figure PCTCN2019121491-appb-000097
There must be measurement errors
Figure PCTCN2019121491-appb-000098
It can be expressed as:
Figure PCTCN2019121491-appb-000099
Figure PCTCN2019121491-appb-000099
捷联解算所得到的角速度
Figure PCTCN2019121491-appb-000100
也存在解算误差,其也可以表示为:
The angular velocity obtained by the strapdown solution
Figure PCTCN2019121491-appb-000100
There are also solution errors, which can also be expressed as:
Figure PCTCN2019121491-appb-000101
Figure PCTCN2019121491-appb-000101
把上式(3)和(4)代入姿态四元数微分方程(1),可得到实际解算时的姿态四元数更微分方程为:Substituting the above equations (3) and (4) into the attitude quaternion differential equation (1), the more differential equation of the attitude quaternion during actual solution can be obtained as:
Figure PCTCN2019121491-appb-000102
Figure PCTCN2019121491-appb-000102
因此,把式(5)减去式(1)可得到如下形式:Therefore, subtracting equation (1) from equation (5) gives the following form:
Figure PCTCN2019121491-appb-000103
Figure PCTCN2019121491-appb-000103
Figure PCTCN2019121491-appb-000104
则可以得到姿态四元数误差方程为:
make
Figure PCTCN2019121491-appb-000104
Then we can get the attitude quaternion error equation as:
Figure PCTCN2019121491-appb-000105
Figure PCTCN2019121491-appb-000105
上式(7)中最后两项表达式满足如下关系:The last two expressions in the above formula (7) satisfy the following relationship:
Figure PCTCN2019121491-appb-000106
Figure PCTCN2019121491-appb-000106
其中,
Figure PCTCN2019121491-appb-000107
Figure PCTCN2019121491-appb-000108
分别定义为:
among them,
Figure PCTCN2019121491-appb-000107
with
Figure PCTCN2019121491-appb-000108
They are defined as:
Figure PCTCN2019121491-appb-000109
Figure PCTCN2019121491-appb-000109
Figure PCTCN2019121491-appb-000110
Figure PCTCN2019121491-appb-000110
上式
Figure PCTCN2019121491-appb-000111
Figure PCTCN2019121491-appb-000112
中,满足如下关系:
The above formula
Figure PCTCN2019121491-appb-000111
with
Figure PCTCN2019121491-appb-000112
In, satisfy the following relationship:
Figure PCTCN2019121491-appb-000113
Figure PCTCN2019121491-appb-000113
把上式关系代入(7),可得姿态四元数误差方程式:Substituting the above relationship into (7), we can get the attitude quaternion error equation:
Figure PCTCN2019121491-appb-000114
Figure PCTCN2019121491-appb-000114
需要说明的是,本发明所述姿态四元数误差方程式(12)的推导过程,并没有假定是小失准误差角的情况,因此其可用于描述在大失准角误差下的弹体飞行姿态误差传播特性,是一种适用于大误差角状态下的弹体姿态误差模型。It should be noted that the derivation process of the attitude quaternion error equation (12) of the present invention does not assume the case of a small misalignment error angle, so it can be used to describe the flight of a missile under a large misalignment error The attitude error propagation characteristic is a model of the attitude error of the projectile that is suitable for a large error angle.
2.2、旋转弹速度误差模型2.2. Rotating bomb speed error model
由比力方程可推导出弹体速度误差方程为:From the specific force equation, the velocity error equation of the projectile can be derived as:
Figure PCTCN2019121491-appb-000115
Figure PCTCN2019121491-appb-000115
上式中,
Figure PCTCN2019121491-appb-000116
为姿态变换矩阵的计算误差,由于
Figure PCTCN2019121491-appb-000117
是关于四元数误差
Figure PCTCN2019121491-appb-000118
的非线性函数,所以
Figure PCTCN2019121491-appb-000119
也是关于
Figure PCTCN2019121491-appb-000120
的非线性函数;
Figure PCTCN2019121491-appb-000121
为加速度计在导航系下的等效零偏,满足
Figure PCTCN2019121491-appb-000122
δK A和δA分别为加速度计的刻度系数误差矩阵和安装误差矩阵;V n为导航系下速度分量。δV n为速度误差;
Figure PCTCN2019121491-appb-000123
地球自转角速度;
Figure PCTCN2019121491-appb-000124
地球自转角速度误差;
Figure PCTCN2019121491-appb-000125
为导航坐标系相对地球的角速;
Figure PCTCN2019121491-appb-000126
为导航坐标系相对地球的角速误差;f b为加速度计比力。
In the above formula,
Figure PCTCN2019121491-appb-000116
Is the calculation error of the attitude transformation matrix, because
Figure PCTCN2019121491-appb-000117
Is about quaternion error
Figure PCTCN2019121491-appb-000118
Nonlinear function, so
Figure PCTCN2019121491-appb-000119
Also about
Figure PCTCN2019121491-appb-000120
Nonlinear function
Figure PCTCN2019121491-appb-000121
Is the equivalent zero offset of the accelerometer under the navigation system, satisfying
Figure PCTCN2019121491-appb-000122
δK A and δA are the scale factor error matrix and installation error matrix of the accelerometer respectively; V n is the velocity component under the navigation system. δV n is the speed error;
Figure PCTCN2019121491-appb-000123
Earth's rotation angular velocity;
Figure PCTCN2019121491-appb-000124
Earth rotation angular velocity error;
Figure PCTCN2019121491-appb-000125
The angular velocity of the navigation coordinate system relative to the earth;
Figure PCTCN2019121491-appb-000126
Is the angular velocity error of the navigation coordinate system relative to the earth; f b is the specific force of the accelerometer.
若加速度计事前经通校准后,可不考虑δK A和δA,则弹体速度误差方程为: If the accelerometer is calibrated beforehand, δK A and δA can be disregarded, then the velocity error equation of the projectile is:
Figure PCTCN2019121491-appb-000127
Figure PCTCN2019121491-appb-000127
根据上述式(11)所述转换关系,可得弹体姿态变换矩阵有:According to the conversion relationship described in equation (11) above, the available body attitude transformation matrix is:
Figure PCTCN2019121491-appb-000128
Figure PCTCN2019121491-appb-000128
因此,姿态变换矩阵的计算误差
Figure PCTCN2019121491-appb-000129
可写为:
Therefore, the calculation error of the attitude transformation matrix
Figure PCTCN2019121491-appb-000129
Can be written as:
Figure PCTCN2019121491-appb-000130
Figure PCTCN2019121491-appb-000130
如前所述,
Figure PCTCN2019121491-appb-000131
代入上式(16)可整理得到
Figure PCTCN2019121491-appb-000132
As mentioned before,
Figure PCTCN2019121491-appb-000131
Substituting into the above formula (16) can be sorted out
Figure PCTCN2019121491-appb-000132
Figure PCTCN2019121491-appb-000133
Figure PCTCN2019121491-appb-000133
又由于
Figure PCTCN2019121491-appb-000134
Figure PCTCN2019121491-appb-000135
可简写为:
Again
Figure PCTCN2019121491-appb-000134
then
Figure PCTCN2019121491-appb-000135
Can be abbreviated as:
Figure PCTCN2019121491-appb-000136
Figure PCTCN2019121491-appb-000136
当姿态角误差较大时,
Figure PCTCN2019121491-appb-000137
Figure PCTCN2019121491-appb-000138
是非线性的,其中
Figure PCTCN2019121491-appb-000139
的计算公式为:
When the attitude angle error is large,
Figure PCTCN2019121491-appb-000137
Correct
Figure PCTCN2019121491-appb-000138
Is nonlinear, where
Figure PCTCN2019121491-appb-000139
The calculation formula is:
Figure PCTCN2019121491-appb-000140
Figure PCTCN2019121491-appb-000140
由上述的推导关系可知,速度误差方程体现出是一个非线性的误差方程,其中
Figure PCTCN2019121491-appb-000141
项即为其非线性部分,若假设速度误差方程(14)中非线性部分为f 1(x,t):
From the above derivation, we can see that the velocity error equation is a nonlinear error equation, where
Figure PCTCN2019121491-appb-000141
The term is its nonlinear part. If the nonlinear part in the velocity error equation (14) is assumed to be f 1 (x, t):
Figure PCTCN2019121491-appb-000142
Figure PCTCN2019121491-appb-000142
在对非线性的速度误差方程进行线性化处理时,f 1(x,t)对
Figure PCTCN2019121491-appb-000143
的雅克比矩阵公式为:
When linearizing the nonlinear velocity error equation, f 1 (x, t) is
Figure PCTCN2019121491-appb-000143
The formula of the Jacobian matrix is:
Figure PCTCN2019121491-appb-000144
Figure PCTCN2019121491-appb-000144
上式δu i(i=1,2,3,4)表示
Figure PCTCN2019121491-appb-000145
的第i行,其中,
Figure PCTCN2019121491-appb-000146
Figure PCTCN2019121491-appb-000147
分别定义为:
The above formula δu i (i=1, 2, 3, 4) represents
Figure PCTCN2019121491-appb-000145
The i-th line, where,
Figure PCTCN2019121491-appb-000146
with
Figure PCTCN2019121491-appb-000147
They are defined as:
Figure PCTCN2019121491-appb-000148
Figure PCTCN2019121491-appb-000148
因此,综合方程(14)和(18)可以用于准确的描述弹体在大失准误差角情况下的弹体速度误差传规律,是一种适用于大误差角状态下的弹体速度误差模型。Therefore, the comprehensive equations (14) and (18) can be used to accurately describe the transmission law of the projectile speed error under the condition of large misalignment error angle, and it is a kind of projectile speed error applicable to the state of large error angle model.
2.3、位置误差方程2.3. Position error equation
弹体位置误差方程为:The body position error equation is:
Figure PCTCN2019121491-appb-000149
Figure PCTCN2019121491-appb-000149
式(24)中,V E、V N、V U分别为弹体沿东、北、天方向的速度;R M和R N分别为弹体所在点子午圈和卯酉圈的曲率半径;L为弹体所在点纬度,λ为弹体所在点经度,h为弹体所在点的高度;δV E,δV N,δV U为旋转弹速度误差参数,δh,δλ和δL为位置误差参数。 In equation (24), V E , V N , and V U are the velocity of the projectile in the east, north, and sky directions; R M and R N are the radius of curvature of the meridian circle and the unitary circle where the projectile is located; L Is the latitude of the point where the projectile is located, λ is the longitude of the point where the projectile is located, h is the height of the point where the projectile is located; δV E , δV N , and δV U are the velocity error parameters of the rotating projectile, and δh, δλ, and δL are the position error parameters.
3、弹体姿态高阶非线性滤波模型3. High-order nonlinear filtering model of projectile attitude
选取旋转弹姿态四元数误差δQ、速度误差δv和位置误差δp以及陀螺漂移ε b、加速度计零偏作为系统的状态变量
Figure PCTCN2019121491-appb-000150
其可表示为
The quaternion error δQ, velocity error δv and position error δp of the rotating projectile, gyro drift ε b and accelerometer bias are selected as the state variables of the system
Figure PCTCN2019121491-appb-000150
It can be expressed as
Figure PCTCN2019121491-appb-000151
Figure PCTCN2019121491-appb-000151
选取上述推导所得弹体飞行姿态误差方程(12)、速度误差方程(14)和位置误差方 程(24)共同构成了滤波器状态方程组,将其简化为如下一般形式:The flight attitude error equation (12), velocity error equation (14) and position error equation (24) obtained by the above derivation form the filter state equation group, which is simplified to the following general form:
Figure PCTCN2019121491-appb-000152
Figure PCTCN2019121491-appb-000152
上式中f[X(t),t]是关于自变量X(t)的非线性函数,系统过程白噪声w(t)满足E[w(t)]=0和E[w(t),w T(τ)]=Q(t)δ(t-τ)。 In the above formula, f[X(t), t] is a nonlinear function about the independent variable X(t), and the system process white noise w(t) satisfies E[w(t)]=0 and E[w(t) , W T (τ)]=Q(t)δ(t-τ).
选取卫星导航系统测量输出的位置和速度与惯导相应解算的位置和速度相减结果作为组合滤波系统的观测变量Z(t),其可表示为:The position and velocity of the satellite navigation system measurement output and the corresponding position and velocity of the inertial navigation are subtracted as the observation variable Z(t) of the combined filter system, which can be expressed as:
Figure PCTCN2019121491-appb-000153
Figure PCTCN2019121491-appb-000153
上式中L GPS,λ GPS,h GPS和v i,GPS(i=N,E,U)分别表示为卫星导航系统测量输出的位置和速度信息,下标为INS变量表示为惯导解算的位置和速度信息。量测噪声v(t)满足E[v(t)]=0和E[v(t),v T(τ)]=R(t)δ(t-τ)。因此,综合上述状态方程(25)和量测方程(26)共同构成了适用于大误差角状态下的弹体姿态高阶非线性滤波模型。 In the above formula, L GPS , λ GPS , h GPS and v i, GPS (i=N, E, U) represent the position and velocity information measured and output by the satellite navigation system, respectively, and the subscript is the INS variable, which represents the inertial navigation solution. Location and speed information. The measurement noise v(t) satisfies E[v(t)]=0 and E[v(t), v T (τ)]=R(t)δ(t-τ). Therefore, the above-mentioned equation of state (25) and measurement equation (26) are combined to form a high-order nonlinear filtering model for the attitude of the projectile in the state of large error angle.
4、弹体姿态高精度实时滤波算法4. High-precision real-time filtering algorithm for projectile attitude
上述旋转弹姿态高精度滤波模型是强非线性方程组,基于非线性函数概率密度分布进行近似方法的UKF和SRUKF等滤波方法可以有效避免了对非线性方程近似所产生的模型误差过大而影响滤波精度的问题。但SRUKF与传统的UKF滤波方法在一些情况下容易出现状态协方差矩阵P失去正定性而导致滤波发散现象。针对上述问题,本发明采用基于修正系数的SRUKF弹体姿态滤波算法,以提高滤波算法的收敛速度与参数估计精度。The above-mentioned high-precision filtering model of the rotating projectile attitude is a strong nonlinear equation system. The filtering methods such as UKF and SRUKF based on the nonlinear function probability density distribution can effectively avoid the model error caused by the approximation of the nonlinear equation. The problem of filtering accuracy. However, in some cases, SRUKF and traditional UKF filtering methods are prone to state covariance matrix P losing positive definiteness, resulting in filtering divergence. In response to the above problems, the present invention adopts a SRUKF body attitude filtering algorithm based on correction coefficients to improve the convergence speed and parameter estimation accuracy of the filtering algorithm.
基于修正系数的SRUKF滤波算法流程如下:The SRUKF filtering algorithm process based on the correction coefficient is as follows:
4.1、滤波初始化:4.1, filter initialization:
Figure PCTCN2019121491-appb-000154
Figure PCTCN2019121491-appb-000154
对于任一时段UKF滤波算法计算一个循环的具体步骤:For any period of time, the UKF filter algorithm calculates the specific steps of a cycle:
4.2、对于给定的
Figure PCTCN2019121491-appb-000155
和P k-1(k=0,2,...n),首先计算状态一步预测
Figure PCTCN2019121491-appb-000156
及一步预报误差协方差阵P k,k-1,包括sigma点计算及其传播过程:
4.2. For a given
Figure PCTCN2019121491-appb-000155
And P k-1 (k = 0, 2, ... n), first calculate the state and predict one step
Figure PCTCN2019121491-appb-000156
And one-step forecast error covariance matrix P k,k-1 , including sigma point calculation and its propagation process:
4.2.1、计算sigma点
Figure PCTCN2019121491-appb-000157
即为:
4.2.1. Calculate sigma points
Figure PCTCN2019121491-appb-000157
That is:
Figure PCTCN2019121491-appb-000158
Figure PCTCN2019121491-appb-000158
4.2.2、计算
Figure PCTCN2019121491-appb-000159
通过状态方程f(·)传播的sigma点,即为:
4.2.2, calculation
Figure PCTCN2019121491-appb-000159
The sigma point propagating through the state equation f(·) is:
Figure PCTCN2019121491-appb-000160
Figure PCTCN2019121491-appb-000160
上式中qr{·}表示对其矩阵进行矩阵的正交三角分解(QR分解),而
Figure PCTCN2019121491-appb-000161
表为其QR分解后的返回值R;公式S′=cholupdate{S,u,±v}是等价于SS T=P,S′=chol{P±vuu T}。
In the above formula, qr{·} means to perform orthogonal triangulation (QR decomposition) of the matrix of the matrix, and
Figure PCTCN2019121491-appb-000161
The table is the return value R after QR decomposition; the formula S′=cholupdate{S,u,±v} is equivalent to SS T =P, S′=chol{P±vuu T }.
4.3、利用UT变换,求sigma点
Figure PCTCN2019121491-appb-000162
和P k,k-1通过量测方程的传播,包括如下两更新计算过程:
4.3. Use UT transform to find sigma points
Figure PCTCN2019121491-appb-000162
Propagation of P k,k-1 through the measurement equation includes the following two update calculation processes:
4.3.1、首先,计算sigma点
Figure PCTCN2019121491-appb-000163
和P k,k-1通过量测方程h(·)的对X k的传播:
4.3.1. First, calculate the sigma point
Figure PCTCN2019121491-appb-000163
And P k,k-1 by measuring the propagation of equation h(·) to X k :
Figure PCTCN2019121491-appb-000164
Figure PCTCN2019121491-appb-000164
4.3.2、然后,计算输出的一步提前预测值:4.3.2 Then, calculate the output one-step forecast value in advance:
Figure PCTCN2019121491-appb-000165
Figure PCTCN2019121491-appb-000165
4.4、最后,利用得到的新的量测值,进行滤波更新过程:4.4. Finally, use the new measured values to perform the filter update process:
Figure PCTCN2019121491-appb-000166
Figure PCTCN2019121491-appb-000166
上述经修正系数的SRUKF滤波估计算法与常规SRUKF滤波方法不同之处在于sigma点计算,在sigma点计算公式(28)中多了一项修正系数μ,其大小必须通过先验知识来加于选择。由于修正系数满足μ>1,所以在时间更新后sigma点
Figure PCTCN2019121491-appb-000167
的误差方差S k,k-1和提前预测值
Figure PCTCN2019121491-appb-000168
的误差方差S zk都必将会增大,但是其观测噪声方差阵R k不变,因此,量测修正的增益K k也将随之增大,这意味着利用新量测值的权重加大,也即降低了陈旧量测信息对估计值的影响,所以,改进后的修正系数SRUKF滤波算法的收敛发敞的问题将得到较好的抑制。通过上述基于修正系数的SRUKF滤波算法流程,最终实现旋转弹飞行参数的高精度估计。
The above-mentioned modified coefficient SRUKF filter estimation algorithm is different from the conventional SRUKF filter method in the calculation of sigma points. In the sigma point calculation formula (28), there is an additional correction coefficient μ, and its size must be added to the selection through prior knowledge. . Since the correction coefficient satisfies μ>1, the sigma point after time update
Figure PCTCN2019121491-appb-000167
Error variance S k, k-1 and the predicted value in advance
Figure PCTCN2019121491-appb-000168
The error variance S zk will increase, but the observation noise variance matrix R k will not change. Therefore, the measurement correction gain K k will also increase, which means that the weight of the new measurement value is added Large, which reduces the impact of stale measurement information on the estimated value, so the problem of open convergence of the improved correction coefficient SRUKF filter algorithm will be better suppressed. Through the SRUKF filter algorithm flow based on the correction coefficients mentioned above, the high-precision estimation of the flight parameters of the rotating bomb is finally achieved.
应当指出,对于本技术领域的一般技术人员来说,在不脱离本发明原理的前提下,还可以做出若干改进和应用,这些改进和应用也视为本发明的保护范围。It should be noted that, for a person of ordinary skill in the art, without departing from the principles of the present invention, several improvements and applications can be made, and these improvements and applications are also considered to be within the scope of the present invention.

Claims (1)

  1. 一种基于磁测滚转角速率信息的旋转弹飞行姿态高精度估计方法,其特征在于:包括如下步骤:A high-precision estimation method for the flying attitude of a rotating projectile based on magnetic measurement of rolling angular rate information is characterized by the following steps:
    (1)、旋转弹飞行姿态组合测量(1) Combined measurement of the flying attitude of the rotating bomb
    1.1、弹载传感器及安装方式1.1, bomb-mounted sensor and installation method
    弹载传感器采用三轴地磁传感器、两个单轴陀螺仪和卫星接收机,其中,三轴地磁传感器用于测量弹体内的地磁场矢量信息,其各敏感轴方向Mx、My和Mz与弹体坐标系OX bY bZ b各轴方向完全一致;两个单轴陀螺仪Gy和Gz分别捷联安装于Y b和Z b轴上,陀螺仪用于测量弹体Y轴和Z轴角速率信息,X轴向角速率信息由地磁传感器测量信息滤波估算得到;卫星接收机用于测量弹体速度和位置信息,接收机天线环形安装于弹体表面; The bomb-mounted sensor uses a three-axis geomagnetic sensor, two single-axis gyroscopes and a satellite receiver. Among them, the three-axis geomagnetic sensor is used to measure the vector information of the geomagnetic field in the body of the missile. The coordinate system OX b Y b Z b has the same direction of each axis; two single-axis gyroscopes Gy and Gz are respectively installed on the Y b and Z b axes, and the gyroscopes are used to measure the Y-axis and Z-axis angular rates of the projectile Information, the X-axis angular rate information is estimated by filtering the geomagnetic sensor measurement information; the satellite receiver is used to measure the speed and position information of the projectile, and the receiver antenna is installed on the surface of the projectile in a loop;
    1.2、弹体飞行姿态高精度组合滤波结构1.2. High-precision combined filter structure for missile flight attitude
    组合滤波器由滚转角速率估计滤波器和弹体飞行姿态高精度滤波器两个滤波器组成,分别用于完成弹体滚转速率的估计和弹体飞行姿态参数的高精度估计;The combined filter is composed of two filters, a roll angle rate estimation filter and a high-precision filter for the flying attitude of the missile, which are used to complete the estimation of the roll rate of the missile and the high-precision estimation of the flying attitude of the missile, respectively;
    (2)、旋转弹高精度误差模型(2), high-precision error model of rotating bomb
    2.1、旋转弹姿态误差模型2.1. Rotating projectile error model
    根据捷联惯性导航理论,弹体坐标系到导航坐标系的姿态四元数
    Figure PCTCN2019121491-appb-100001
    的微分方程表示为:
    According to the strapdown inertial navigation theory, the attitude quaternion from the body coordinate system to the navigation coordinate system
    Figure PCTCN2019121491-appb-100001
    The differential equation of is expressed as:
    Figure PCTCN2019121491-appb-100002
    Figure PCTCN2019121491-appb-100002
    上式中,
    Figure PCTCN2019121491-appb-100003
    为四元数矩阵,是反对阵矩阵形式:
    In the above formula,
    Figure PCTCN2019121491-appb-100003
    It is a quaternion matrix, which is in the form of an anti-matrix matrix:
    Figure PCTCN2019121491-appb-100004
    Figure PCTCN2019121491-appb-100004
    其中,
    Figure PCTCN2019121491-appb-100005
    为弹体坐标系相对于惯性坐标系的角速度在弹体坐标系上的投影分量
    Figure PCTCN2019121491-appb-100006
    即为导航坐标系相对与惯性坐标系的角速度在导航坐标系上的投影分量
    Figure PCTCN2019121491-appb-100007
    Figure PCTCN2019121491-appb-100008
    分别表示为:
    among them,
    Figure PCTCN2019121491-appb-100005
    Is the projected component of the angular velocity of the projectile coordinate system relative to the inertial coordinate system on the projectile coordinate system
    Figure PCTCN2019121491-appb-100006
    It is the projection component of the angular velocity of the navigation coordinate system relative to the inertial coordinate system on the navigation coordinate system
    Figure PCTCN2019121491-appb-100007
    with
    Figure PCTCN2019121491-appb-100008
    Represented as:
    Figure PCTCN2019121491-appb-100009
    Figure PCTCN2019121491-appb-100009
    由于角速率分量
    Figure PCTCN2019121491-appb-100010
    是通过传感器测量所得,其测量值
    Figure PCTCN2019121491-appb-100011
    必然存在测量误差
    Figure PCTCN2019121491-appb-100012
    其表示为:
    Due to angular rate component
    Figure PCTCN2019121491-appb-100010
    It is measured by the sensor and its measured value
    Figure PCTCN2019121491-appb-100011
    There must be measurement error
    Figure PCTCN2019121491-appb-100012
    It is expressed as:
    Figure PCTCN2019121491-appb-100013
    Figure PCTCN2019121491-appb-100013
    捷联解算所得到的角速度
    Figure PCTCN2019121491-appb-100014
    也存在解算误差,其表示为:
    The angular velocity obtained by the strapdown solution
    Figure PCTCN2019121491-appb-100014
    There is also a solution error, which is expressed as:
    Figure PCTCN2019121491-appb-100015
    Figure PCTCN2019121491-appb-100015
    把上式(3)和(4)代入姿态四元数微分方程(1),得到实际解算时的姿态四元数更微分方程为:Substituting the above equations (3) and (4) into the attitude quaternion differential equation (1), the more differential equation of the attitude quaternion when the actual solution is obtained is:
    Figure PCTCN2019121491-appb-100016
    Figure PCTCN2019121491-appb-100016
    因此,把式(5)减去式(1)得到如下形式:Therefore, subtracting equation (1) from equation (5) yields the following form:
    Figure PCTCN2019121491-appb-100017
    Figure PCTCN2019121491-appb-100017
    Figure PCTCN2019121491-appb-100018
    则得到姿态四元数误差方程为:
    make
    Figure PCTCN2019121491-appb-100018
    Then the error equation of the attitude quaternion is:
    Figure PCTCN2019121491-appb-100019
    Figure PCTCN2019121491-appb-100019
    上式(7)中最后两项表达式满足如下关系:The last two expressions in the above formula (7) satisfy the following relationship:
    Figure PCTCN2019121491-appb-100020
    Figure PCTCN2019121491-appb-100020
    其中,
    Figure PCTCN2019121491-appb-100021
    Figure PCTCN2019121491-appb-100022
    分别定义为:
    among them,
    Figure PCTCN2019121491-appb-100021
    with
    Figure PCTCN2019121491-appb-100022
    They are defined as:
    Figure PCTCN2019121491-appb-100023
    Figure PCTCN2019121491-appb-100023
    Figure PCTCN2019121491-appb-100024
    Figure PCTCN2019121491-appb-100024
    上式
    Figure PCTCN2019121491-appb-100025
    Figure PCTCN2019121491-appb-100026
    中,满足如下关系:
    The above formula
    Figure PCTCN2019121491-appb-100025
    with
    Figure PCTCN2019121491-appb-100026
    In, satisfy the following relationship:
    Figure PCTCN2019121491-appb-100027
    Figure PCTCN2019121491-appb-100027
    把上式关系代入(7),得姿态四元数误差方程式:Substituting the above relationship into (7), the attitude quaternion error equation is obtained:
    Figure PCTCN2019121491-appb-100028
    Figure PCTCN2019121491-appb-100028
    2.2、旋转弹速度误差模型2.2. Rotating bomb speed error model
    由比力方程推导出弹体速度误差方程为:The velocity error equation derived from the specific force equation is:
    Figure PCTCN2019121491-appb-100029
    Figure PCTCN2019121491-appb-100029
    上式中,
    Figure PCTCN2019121491-appb-100030
    为姿态变换矩阵的计算误差,由于
    Figure PCTCN2019121491-appb-100031
    是关于四元数误差
    Figure PCTCN2019121491-appb-100032
    的非线性函数,所以
    Figure PCTCN2019121491-appb-100033
    也是关于
    Figure PCTCN2019121491-appb-100034
    的非线性函数;
    Figure PCTCN2019121491-appb-100035
    为加速度计在导航系下的等效零偏,满足
    Figure PCTCN2019121491-appb-100036
    δK A和δA分别为加速度计的刻度系数误差矩阵和安装误差矩阵;V n为导航系下速度分量;δV n为速度误差;
    Figure PCTCN2019121491-appb-100037
    地球自转角速度;
    Figure PCTCN2019121491-appb-100038
    地球自转角速度误差;
    Figure PCTCN2019121491-appb-100039
    为导航坐标系相对地球的角速;
    Figure PCTCN2019121491-appb-100040
    为导航坐标系相对地球的角速误差;f b为加速度计比力;
    In the above formula,
    Figure PCTCN2019121491-appb-100030
    Is the calculation error of the attitude transformation matrix, because
    Figure PCTCN2019121491-appb-100031
    Is about quaternion error
    Figure PCTCN2019121491-appb-100032
    Nonlinear function, so
    Figure PCTCN2019121491-appb-100033
    Also about
    Figure PCTCN2019121491-appb-100034
    Nonlinear function
    Figure PCTCN2019121491-appb-100035
    Is the equivalent zero offset of the accelerometer under the navigation system, satisfying
    Figure PCTCN2019121491-appb-100036
    δK A and δA are respectively the scale factor error matrix and the installation error matrix of the accelerometer; V n is the speed component under the navigation system; δ V n is the speed error;
    Figure PCTCN2019121491-appb-100037
    Earth's rotation angular velocity;
    Figure PCTCN2019121491-appb-100038
    Earth rotation angular velocity error;
    Figure PCTCN2019121491-appb-100039
    The angular velocity of the navigation coordinate system relative to the earth;
    Figure PCTCN2019121491-appb-100040
    Is the angular velocity error of the navigation coordinate system relative to the earth; f b is the specific force of the accelerometer;
    若加速度计事前经校准后,则不考虑δK A和δA,则弹体速度误差方程为: If the accelerometer is calibrated beforehand, δK A and δA are not considered, then the velocity error equation of the projectile is:
    Figure PCTCN2019121491-appb-100041
    Figure PCTCN2019121491-appb-100041
    根据上述式(11)所述转换关系,得弹体姿态变换矩阵有:According to the conversion relationship described in the above formula (11), the obtained body attitude transformation matrix is:
    Figure PCTCN2019121491-appb-100042
    Figure PCTCN2019121491-appb-100042
    因此,姿态变换矩阵的计算误差
    Figure PCTCN2019121491-appb-100043
    为:
    Therefore, the calculation error of the attitude transformation matrix
    Figure PCTCN2019121491-appb-100043
    for:
    Figure PCTCN2019121491-appb-100044
    Figure PCTCN2019121491-appb-100044
    如前所述,
    Figure PCTCN2019121491-appb-100045
    代入上式(16)得到
    Figure PCTCN2019121491-appb-100046
    As mentioned before,
    Figure PCTCN2019121491-appb-100045
    Substitute into the above formula (16) to get
    Figure PCTCN2019121491-appb-100046
    Figure PCTCN2019121491-appb-100047
    Figure PCTCN2019121491-appb-100047
    又由于
    Figure PCTCN2019121491-appb-100048
    Figure PCTCN2019121491-appb-100049
    简化为:
    Again
    Figure PCTCN2019121491-appb-100048
    then
    Figure PCTCN2019121491-appb-100049
    Simplified to:
    Figure PCTCN2019121491-appb-100050
    Figure PCTCN2019121491-appb-100050
    Figure PCTCN2019121491-appb-100051
    Figure PCTCN2019121491-appb-100052
    是非线性的,其中
    Figure PCTCN2019121491-appb-100053
    的计算公式为:
    Figure PCTCN2019121491-appb-100051
    Correct
    Figure PCTCN2019121491-appb-100052
    Is nonlinear, where
    Figure PCTCN2019121491-appb-100053
    The calculation formula is:
    Figure PCTCN2019121491-appb-100054
    Figure PCTCN2019121491-appb-100054
    由上述的推导关系可知,速度误差方程体现出是一个非线性的误差方程,其中
    Figure PCTCN2019121491-appb-100055
    项即为其非线性部分,若假设速度误差方程(14)中非线性部分为f 1(x,t):
    From the above derivation, we can see that the velocity error equation is a nonlinear error equation, where
    Figure PCTCN2019121491-appb-100055
    The term is its nonlinear part. If the nonlinear part in the velocity error equation (14) is assumed to be f 1 (x, t):
    Figure PCTCN2019121491-appb-100056
    Figure PCTCN2019121491-appb-100056
    在对非线性的速度误差方程进行线性化处理时,f 1(x,t)对
    Figure PCTCN2019121491-appb-100057
    的雅克比矩阵公式为:
    When linearizing the nonlinear velocity error equation, f 1 (x, t) is
    Figure PCTCN2019121491-appb-100057
    The formula of the Jacobian matrix is:
    Figure PCTCN2019121491-appb-100058
    Figure PCTCN2019121491-appb-100058
    上式δu i(i=1,2,3,4)表示
    Figure PCTCN2019121491-appb-100059
    的第i行,其中,
    Figure PCTCN2019121491-appb-100060
    Figure PCTCN2019121491-appb-100061
    分别定义为:
    The above formula δu i (i=1, 2, 3, 4) represents
    Figure PCTCN2019121491-appb-100059
    The i-th line, where,
    Figure PCTCN2019121491-appb-100060
    with
    Figure PCTCN2019121491-appb-100061
    They are defined as:
    Figure PCTCN2019121491-appb-100062
    Figure PCTCN2019121491-appb-100062
    综合方程(14)和(18)为适用于大误差角状态下的弹体速度误差模型;The integrated equations (14) and (18) are the velocity error models of the projectile that are suitable for the large error angle state;
    2.3、位置误差方程2.3. Position error equation
    弹体位置误差方程为:The body position error equation is:
    Figure PCTCN2019121491-appb-100063
    Figure PCTCN2019121491-appb-100063
    式(24)中,V E、V N、V U分别为弹体沿东、北、天方向的速度;R M和R N分别为弹体所在点子午圈和卯酉圈的曲率半径;L为弹体所在点纬度,λ为弹体所在点经度,h为弹体所在点的高度;δV E,δV N,δV U为旋转弹速度误差参数,δh,δλ和δL为位置误差参数; In equation (24), V E , V N , and V U are the velocity of the projectile in the east, north, and sky directions; R M and R N are the radius of curvature of the meridian circle and the unitary circle where the projectile is located; L Is the latitude of the point where the projectile is located, λ is the longitude of the point where the projectile is located, h is the height of the point where the projectile is located; δV E , δV N , δV U are the parameters of the velocity error of the rotating projectile, δh, δλ and δL are the position error parameters;
    (3)、弹体姿态高阶非线性滤波模型(3) High-order nonlinear filtering model of projectile attitude
    选取旋转弹姿态四元数误差δQ、速度误差δ V和位置误差δp以及陀螺漂移ε b、加速度计零偏作为系统的状态变量
    Figure PCTCN2019121491-appb-100064
    其表示为
    Figure PCTCN2019121491-appb-100065
    The quaternion error δQ, velocity error δ V , position error δp, gyro drift ε b and accelerometer bias of the rotating projectile are selected as the state variables of the system
    Figure PCTCN2019121491-appb-100064
    Which is expressed as
    Figure PCTCN2019121491-appb-100065
    选取上述推导所得弹体飞行姿态误差方程(12)、速度误差方程(14)和位置误差方程(24)共同构成了滤波器状态方程组,将其简化为如下一般形式:The flight attitude error equation (12), velocity error equation (14) and position error equation (24) obtained by the above derivation form the filter state equation group, which is simplified to the following general form:
    Figure PCTCN2019121491-appb-100066
    Figure PCTCN2019121491-appb-100066
    上式中f[X(t),t]是关于自变量X(t)的非线性函数,系统过程白噪声w(t)满足E[w(t)]=0和E[w(t),w T(τ)]=Q(t)δ(t-τ); In the above formula, f[X(t), t] is a nonlinear function about the independent variable X(t), and the system process white noise w(t) satisfies E[w(t)]=0 and E[w(t) , W T (τ)] = Q(t)δ(t-τ);
    选取卫星导航系统测量输出的位置和速度与惯导相应解算的位置和速度相减结果作为组合滤波系统的观测变量Z(t),其表示为:The subtraction result of the position and velocity measured by the satellite navigation system and the corresponding position and velocity calculated by the inertial navigation system is selected as the observation variable Z(t) of the combined filter system, which is expressed as:
    Figure PCTCN2019121491-appb-100067
    Figure PCTCN2019121491-appb-100067
    上式中L GPS,λ GPS,h GPS和v i,GPS(i=N,E,U)分别表示为卫星导航系统测量输出的位置和速度信息,下标为INS变量表示为惯导解算的位置和速度信息;量测噪声v(t)满足E[v(t)]=0和E[v(t),v T(τ)]=R(t)δ(t-τ); In the above formula, L GPS , λ GPS , h GPS and v i, GPS (i=N, E, U) represent the position and speed information measured and output by the satellite navigation system, respectively, and the subscript is the INS variable, which represents the inertial navigation solution. Position and velocity information; measurement noise v(t) satisfies E[v(t)]=0 and E[v(t), v T (τ)]=R(t)δ(t-τ);
    综合上述状态方程(25)和量测方程(26)共同构成适用于大误差角状态下的弹体姿态高阶非线性滤波模型;Combining the above equations of state (25) and measurement equations (26) together constitute a high-order nonlinear filtering model of the body attitude suitable for large error angle states;
    (4)、弹体姿态高精度实时滤波算法(4) High-precision real-time filtering algorithm for projectile attitude
    基于修正系数的SRUKF滤波算法流程如下:The SRUKF filtering algorithm process based on the correction coefficient is as follows:
    4.1、滤波初始化:4.1, filter initialization:
    Figure PCTCN2019121491-appb-100068
    Figure PCTCN2019121491-appb-100068
    对于任一时段UKF滤波算法计算一个循环的具体步骤:For any period of time, the UKF filter algorithm calculates the specific steps of a cycle:
    4.2、对于给定的
    Figure PCTCN2019121491-appb-100069
    和P k-1(k=0,2,...n),首先计算状态一步预测
    Figure PCTCN2019121491-appb-100070
    及一步预报误差协方差阵P k,k-1,包括sigma点计算及其传播过程:
    4.2. For a given
    Figure PCTCN2019121491-appb-100069
    And P k-1 (k = 0, 2, ... n), first calculate the state and predict one step
    Figure PCTCN2019121491-appb-100070
    And one-step forecast error covariance matrix P k,k-1 , including sigma point calculation and its propagation process:
    4.2.1、计算sigma点
    Figure PCTCN2019121491-appb-100071
    即为:
    4.2.1. Calculate sigma points
    Figure PCTCN2019121491-appb-100071
    That is:
    Figure PCTCN2019121491-appb-100072
    Figure PCTCN2019121491-appb-100072
    4.2.2、计算
    Figure PCTCN2019121491-appb-100073
    通过状态方程f(·)传播的sigma点,即为:
    4.2.2, calculation
    Figure PCTCN2019121491-appb-100073
    The sigma point propagating through the state equation f(·) is:
    Figure PCTCN2019121491-appb-100074
    Figure PCTCN2019121491-appb-100074
    上式中qr{·}表示对其矩阵进行矩阵的正交三角分解,而
    Figure PCTCN2019121491-appb-100075
    表为其QR分解后的返回值R;公式S′=cholupdate{S,u,±v}是等价于SS T=P,S′=chol{P±vuu T};
    In the above formula, qr{·} means orthogonal triangulation of the matrix of the matrix, and
    Figure PCTCN2019121491-appb-100075
    The table is the return value R after QR decomposition; the formula S′=cholupdate{S,u,±v} is equivalent to SS T =P, S′=chol{P±vuu T };
    4.3、利用UT变换,求sigma点
    Figure PCTCN2019121491-appb-100076
    和P k,k-1通过量测方程的传播,包括如下两更新计算过程:
    4.3. Use UT transform to find sigma points
    Figure PCTCN2019121491-appb-100076
    Propagation of P k,k-1 through the measurement equation includes the following two update calculation processes:
    4.3.1、首先,计算sigma点
    Figure PCTCN2019121491-appb-100077
    和P k,k-1通过量测方程h(·)的对X k的传播:
    4.3.1. First, calculate the sigma point
    Figure PCTCN2019121491-appb-100077
    And P k,k-1 by measuring the propagation of equation h(·) to X k :
    Figure PCTCN2019121491-appb-100078
    Figure PCTCN2019121491-appb-100078
    4.3.2、然后,计算输出的一步提前预测值:4.3.2 Then, calculate the output one-step forecast value in advance:
    Figure PCTCN2019121491-appb-100079
    Figure PCTCN2019121491-appb-100079
    4.4、最后,利用得到的新的量测值,进行滤波更新过程:4.4. Finally, use the new measured values to perform the filter update process:
    Figure PCTCN2019121491-appb-100080
    Figure PCTCN2019121491-appb-100080
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