CN116086252A - Rolling missile rolling angle measurement error estimation method containing line deviation measurement noise - Google Patents

Rolling missile rolling angle measurement error estimation method containing line deviation measurement noise Download PDF

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CN116086252A
CN116086252A CN202211528804.XA CN202211528804A CN116086252A CN 116086252 A CN116086252 A CN 116086252A CN 202211528804 A CN202211528804 A CN 202211528804A CN 116086252 A CN116086252 A CN 116086252A
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missile
angle measurement
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extended state
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CN116086252B (en
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于剑桥
周洪淼
赵新运
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Beijing Institute of Technology BIT
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    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H17/00Networks using digital techniques
    • H03H17/02Frequency selective networks
    • H03H17/0248Filters characterised by a particular frequency response or filtering method
    • H03H17/026Averaging filters
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F42AMMUNITION; BLASTING
    • F42BEXPLOSIVE CHARGES, e.g. FOR BLASTING, FIREWORKS, AMMUNITION
    • F42B15/00Self-propelled projectiles or missiles, e.g. rockets; Guided missiles
    • F42B15/01Arrangements thereon for guidance or control
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01CMEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
    • G01C1/00Measuring angles
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H17/00Networks using digital techniques
    • H03H17/02Frequency selective networks
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Abstract

The invention aims to provide a rolling missile rolling angle measurement error estimation method with line deviation measurement noise, which is characterized in that a missile is regarded as a second-order low-pass filter and a nonlinear extended state observer of a particle construction system, sampled line deviation data are brought into the filter and the state observer to obtain rolling angle measurement errors, and in order to enable a result to be more accurate, the calculated average value of the obtained rolling angle measurement errors is used for obtaining the rolling angle measurement error value.

Description

一种含线偏差测量噪声的滚转导弹滚转角测量误差估计方法A method for estimating the roll angle measurement error of a rolling missile with linear deviation measurement noise

技术领域Technical Field

本发明涉及一种含线偏差测量噪声的滚转导弹滚转角测量误差估计方法,属于激光驾束制导滚转导弹制导控制技术领域。The invention relates to a rolling missile rolling angle measurement error estimation method containing linear deviation measurement noise, and belongs to the technical field of laser beam-riding guided rolling missile guidance control.

背景技术Background Art

激光驾束制导导弹根据与激光驾束中心的位置线偏差形成制导指令。激光驾束制导滚转导弹使用陀螺仪敏感弹体空间姿态,但由于陀螺仪对重力方向的标定存在误差,进而导致测得的滚转角存在误差。滚转角测量误差的存在会导致理论控制力方向与实际控制力方向存在偏差,致使导弹在俯仰和偏航通道的控制存在耦合,弹道出现螺旋运动。滚转角测量误差的估计对提升激光驾束制导滚转导弹命中精度具有重要意义。滚转角测量误差的估计需使用线偏差数据,但是由导弹敏感到的线偏差数据不可避免会存在测量噪声,对含有噪声的测量数据进行求导会进一步放大噪声,最终难以获得滚转角测量误差。Laser beam-riding guided missiles form guidance instructions based on the position line deviation from the center of the laser beam. Laser beam-riding guided rolling missiles use gyroscopes to sense the spatial attitude of the missile body, but due to the error in the calibration of the gyroscope for the direction of gravity, the measured roll angle has an error. The existence of roll angle measurement error will lead to a deviation between the theoretical control force direction and the actual control force direction, resulting in coupling between the missile's pitch and yaw channel control and spiral motion in the trajectory. Estimation of roll angle measurement error is of great significance to improving the hit accuracy of laser beam-riding guided rolling missiles. Estimation of roll angle measurement error requires the use of line deviation data, but the line deviation data sensed by the missile will inevitably have measurement noise. Derivation of the noisy measurement data will further amplify the noise, and it is ultimately difficult to obtain the roll angle measurement error.

目前针对导弹滚转角测量误差补偿多采用太阳方位角测量法、加速度计法和磁探测法。但是上述方法不可避免会在弹体中引入额外的传感器,增加弹体重量。对于一般用作反坦克及低空防御的激光驾束制导导弹而言,引入高昂的高精度传感器会降低其低成本的优势。At present, the sun azimuth angle measurement method, accelerometer method and magnetic detection method are mostly used to compensate for the missile roll angle measurement error. However, the above methods will inevitably introduce additional sensors into the missile body, increasing the weight of the missile body. For laser beam-riding guided missiles, which are generally used for anti-tank and low-altitude defense, the introduction of expensive high-precision sensors will reduce their low-cost advantages.

发明内容Summary of the invention

本发明提出了一种含线偏差测量噪声的滚转导弹滚转角测量误差估计方法,能够在线偏差含有测量噪声的情况下,较为精准地将导弹滚转角测量误差估计出来,用于控制系统的修正和补偿。The present invention proposes a method for estimating the roll angle measurement error of a rolling missile containing line deviation measurement noise. When the line deviation contains measurement noise, the missile roll angle measurement error can be estimated more accurately for correction and compensation of the control system.

一种含线偏差测量噪声的滚转导弹滚转角测量误差估计方法,包括如下步骤:A method for estimating the roll angle measurement error of a rolling missile containing linear deviation measurement noise comprises the following steps:

步骤一,导弹上激光接收装置处理接收到的激光信号,获取弹目之间的线偏差Δx、Δy,导弹上的控制器根据导弹控制力获得分控制力Fx2、Fy2Step 1: The laser receiving device on the missile processes the received laser signal to obtain the linear deviations Δx and Δy between the missile and the target, and the controller on the missile obtains the sub-control forces F x2 and F y2 according to the missile control force;

步骤二,将线偏差输入二阶低通滤波器后再输入非线性扩张状态观测器,获得扩张状态观测器算出的

Figure BDA0003973861650000021
Step 2: Input the line deviation into the second-order low-pass filter and then into the nonlinear extended state observer to obtain the
Figure BDA0003973861650000021

步骤三,基于所述分控制力Fx2、Fy2、导弹质量m和所述扩张状态观测器算出的

Figure BDA0003973861650000022
计算滚转角测量误差δ;Step 3: Based on the control forces F x2 , F y2 , the missile mass m and the extended state observer,
Figure BDA0003973861650000022
Calculate the roll angle measurement error δ;

步骤四,重复步骤一至四共N次,对获得的结果进行平均值滤波,获得最终的滚转角测量误差估计值

Figure BDA0003973861650000023
Step 4: Repeat steps 1 to 4 N times, perform average filtering on the obtained results, and obtain the final roll angle measurement error estimate.
Figure BDA0003973861650000023

进一步地,本发明所述二阶低通滤波器的传递函数为:Furthermore, the transfer function of the second-order low-pass filter of the present invention is:

Figure BDA0003973861650000024
Figure BDA0003973861650000024

其中,Y(s)为滤波之后的信号在频域表达式,S为复参变量,ω为截止频率,R(s)为输入滤波器的信号进行拉氏变换后在频域表达式。Among them, Y(s) is the frequency domain expression of the signal after filtering, S is a complex parameter, ω is the cutoff frequency, and R(s) is the frequency domain expression of the signal input to the filter after Laplace transform.

进一步地,本发明所述非线性扩张状态观测器:Furthermore, the nonlinear extended state observer of the present invention:

e=z1-ye=z 1 -y

Figure BDA0003973861650000025
Figure BDA0003973861650000025

Figure BDA0003973861650000026
Figure BDA0003973861650000026

Figure BDA0003973861650000027
Figure BDA0003973861650000027

其中,β1,β2,β3,δ1,α1,α2为设定值,饱和函数fal(e,α11)的表示为:Among them, β 1 , β 2 , β 3 , δ 1 , α 1 , α 2 are set values, and the saturation function fal(e,α 11 ) is expressed as:

Figure BDA0003973861650000028
Figure BDA0003973861650000028

饱和函数fal(e,α21)的表示为:The saturation function fal(e,α 21 ) is expressed as:

Figure BDA0003973861650000031
Figure BDA0003973861650000031

其中,sgn(e)为符号函数,输出e的正负号。Among them, sgn(e) is the sign function, which outputs the positive or negative sign of e.

进一步地,所述将线偏差输入二阶低通滤波器后再输入非线性扩张状态观测器,获得扩张状态观测器算出的

Figure BDA0003973861650000032
包括如下内容:Furthermore, the line deviation is input into a second-order low-pass filter and then into a nonlinear extended state observer to obtain the
Figure BDA0003973861650000032
It includes the following:

将线偏差Δx、Δy进行拉氏变换后作为R(s)输入二阶低通滤波器,获得输出Y(s)分别记为Y1(s)、Y2(s),对Y1(s)、Y2(s)进行反拉氏变换后分别带入扩张状态观测器中的变量y,解得其中的z3分别记为

Figure BDA0003973861650000033
The line deviations Δx and Δy are Laplace transformed and input into the second-order low-pass filter as R(s), and the output Y(s) is recorded as Y 1 (s) and Y 2 (s) respectively. After Y 1 (s) and Y 2 (s) are inversely Laplace transformed, they are respectively brought into the variable y in the extended state observer, and the z 3 is solved and recorded as
Figure BDA0003973861650000033

进一步地,所述基于所述分量Fx2、Fy2、导弹质量m和所述扩张状态观测器算出的

Figure BDA0003973861650000034
计算滚转角测量误差δ,包括如下内容,基于所述分量Fx2、Fy2、导弹质量m和所述扩张状态观测器算出的
Figure BDA0003973861650000035
联立求解得滚转角测量误差δ:Furthermore, the component F x2 , F y2 , the missile mass m and the extended state observer calculated
Figure BDA0003973861650000034
Calculating the roll angle measurement error δ includes the following: based on the components F x2 , F y2 , the missile mass m and the extended state observer
Figure BDA0003973861650000035
The roll angle measurement error δ is obtained by simultaneous solution:

Figure BDA0003973861650000036
Figure BDA0003973861650000036

有益效果:Beneficial effects:

第一、本方法计算过程中使用到的计算量,不需要在原有弹体上添加额外的传感器仅依靠导弹上原有的激光接收装置和控制器即可采集完毕,避免了出现像传统方法中的太阳方位角测量法、加速度计法和磁探测法一样加入传感器后增加弹体重量和制造成本。First, the amount of calculation used in the calculation process of this method does not require the addition of additional sensors to the original missile body, and can be collected only by relying on the original laser receiving device and controller on the missile, avoiding the increase in missile body weight and manufacturing cost after adding sensors like the traditional methods of solar azimuth measurement, accelerometer method and magnetic detection method.

第二、本方法计算过程中,为了消除线偏差信号中的测量噪声,构造了二阶低通滤波器,且非线性扩张状态观测器中加入饱和函数fal(e,α1,δ)能够一直信号抖振,系统的精准性更高。Second, in the calculation process of this method, in order to eliminate the measurement noise in the line deviation signal, a second-order low-pass filter is constructed, and the addition of a saturation function fal(e,α 1 ,δ) in the nonlinear extended state observer can suppress signal jitter, and the system has higher accuracy.

第三、由于线偏差测量噪声的存在,步骤三求得的滚转角测量误差会在一定范围内振荡,为了进一步获得准确的滚转角测量误差,对步骤三得到的结果进行平均值滤波,有效消除震荡,计算精准度更高。Third, due to the existence of line deviation measurement noise, the roll angle measurement error obtained in step three will oscillate within a certain range. In order to further obtain an accurate roll angle measurement error, the result obtained in step three is averaged and filtered to effectively eliminate oscillation and achieve higher calculation accuracy.

附图说明BRIEF DESCRIPTION OF THE DRAWINGS

为了更清楚地说明本发明实施例的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其它的附图。In order to more clearly illustrate the technical solutions of the embodiments of the present invention, the drawings required for use in the embodiments will be briefly introduced below. Obviously, the drawings described below are only some embodiments of the present invention. For ordinary technicians in this field, other drawings can be obtained based on these drawings without creative work.

图1为坐标系示意图。Figure 1 is a schematic diagram of the coordinate system.

图2为滚转角测量误差估计流程图。FIG2 is a flow chart of the roll angle measurement error estimation.

具体实施方式DETAILED DESCRIPTION

下面结合附图对本发明实施例进行详细描述。The embodiments of the present invention are described in detail below with reference to the accompanying drawings.

本申请实施例提出了一种含线偏差测量噪声的激光驾束制导滚转导弹滚转角测量误差估计方法,能够在线偏差含有测量噪声的情况下,较为精准地将导弹滚转角测量误差估计出来,用于控制系统的修正和补偿。The embodiment of the present application proposes a method for estimating the roll angle measurement error of a laser beam-riding guided rolling missile containing line deviation measurement noise. The method can more accurately estimate the missile roll angle measurement error when the line deviation contains measurement noise, which is used for correction and compensation of the control system.

一种含线偏差测量噪声的滚转导弹滚转角测量误差估计方法,包括如下步骤(如附图2所示):A method for estimating the roll angle measurement error of a rolling missile containing linear deviation measurement noise comprises the following steps (as shown in FIG. 2 ):

步骤一,导弹上激光接收装置处理接收到的激光信号,不断获取弹目之间的距离偏差Δx、Δy,导弹上的控制器根据导弹控制力获得分控制力Fx2、Fy2Step 1: The laser receiving device on the missile processes the received laser signal and continuously obtains the distance deviations Δx and Δy between the missile and the target. The controller on the missile obtains the sub-control forces F x2 and F y2 according to the missile control force;

本实施例中计算的过程中,其中的距离偏差和分控制力的计算,相当于设定标准坐标系Ox1y1,将导弹M视为质点,质量为m,T为目标点,以导弹质心为原点,其x1、y1轴位于激光波束轴向的垂直平面内,x1轴指向水平方向,y1轴指向重力在该平面的分力相反方向;设定动坐标系Ox2y2为:以导弹质心为原点,动坐标系与标准坐标系之间的夹角为滚转角测量误差δ,Ox1逆时针转到Ox2为正;Fx2、Fy2分别是导弹控制力作用在动坐标系下x2、y2方向上的分控制力,导弹M的坐标为(xM、yM),导弹T的坐标为(xT、yT),在标准坐标系下的导弹和目标之间的位置线偏差为:In the calculation process of this embodiment, the calculation of the distance deviation and the component control force is equivalent to setting the standard coordinate system Ox1y1 , taking the missile M as a mass point with a mass of m, T as the target point, and taking the missile mass center as the origin. Its x1 and y1 axes are located in the vertical plane of the laser beam axis, the x1 axis points to the horizontal direction, and the y1 axis points to the opposite direction of the component force of gravity in the plane; setting the moving coordinate system Ox2y2 as follows : taking the missile mass center as the origin, the angle between the moving coordinate system and the standard coordinate system is the roll angle measurement error δ, and Ox1 is positive when it rotates counterclockwise to Ox2 ; Fx2 and Fy2 are the component control forces of the missile control force acting on the moving coordinate system in the x2 and y2 directions, respectively. The coordinates of the missile M are ( xM , yM ), and the coordinates of the missile T are ( xT , yT ). The position line deviation between the missile and the target in the standard coordinate system is:

Figure BDA0003973861650000051
Figure BDA0003973861650000051

导弹运动学和动力学在标准坐标系下被描述为:The missile kinematics and dynamics are described in standard coordinates as:

Figure BDA0003973861650000052
Figure BDA0003973861650000052

其中VMx、VMy是导弹的在x和y方向上的速度值。Where V Mx and V My are the velocity values of the missile in the x and y directions.

步骤二,构建系统二阶低通滤波器和非线性扩张状态观测器,将线偏差输入二阶低通滤波器后再输入非线性扩张状态观测器,获得扩张状态观测器算出的

Figure BDA0003973861650000053
Step 2: Construct a second-order low-pass filter and a nonlinear extended state observer for the system. Input the line deviation into the second-order low-pass filter and then into the nonlinear extended state observer to obtain the
Figure BDA0003973861650000053

若目标加速度aT=0或满足导弹加速度远大于目标加速度即aT<<aM,在标准坐标系下x方向上,令x1=Δx,

Figure BDA0003973861650000054
建立系统状态方程,其中输出y1为在x1方向的线偏差:If the target acceleration a T = 0 or the missile acceleration is much greater than the target acceleration, that is, a T << a M , in the x direction of the standard coordinate system, let x 1 = Δx,
Figure BDA0003973861650000054
The system state equation is established, where the output y 1 is the line deviation in the x 1 direction:

Figure BDA0003973861650000055
Figure BDA0003973861650000055

Figure BDA0003973861650000056
Figure BDA0003973861650000056

Figure BDA0003973861650000057
Figure BDA0003973861650000057

在标准坐标系下y方向上,令x3=Δy,

Figure BDA0003973861650000058
建立系统状态方程,其中输出y2为在y1方向的线偏差:In the y direction of the standard coordinate system, let x 3 = Δy,
Figure BDA0003973861650000058
The system state equation is established, where the output y2 is the line deviation in the y1 direction:

Figure BDA0003973861650000061
Figure BDA0003973861650000061

Figure BDA0003973861650000062
Figure BDA0003973861650000062

Figure BDA0003973861650000063
Figure BDA0003973861650000063

上述系统状态方程中,f由于未知项δ的存在而成为未知部分。In the above system state equation, f becomes the unknown part due to the existence of the unknown term δ.

将线偏差数据y1、y2进行拉氏变换后作为R(s)输入二阶低通滤波器,构造二阶低通滤波器,其传递函数为:The line deviation data y 1 and y 2 are Laplace transformed and input into a second-order low-pass filter as R(s) to construct a second-order low-pass filter, whose transfer function is:

Figure BDA0003973861650000064
Figure BDA0003973861650000064

其中,Y(s)为滤波之后的信号在频域表达式,ω为截止频率,其取值小于噪声信号频率时,滤波效果较好,通过上述传递函数可获得输出Y(s)分别记为Y1(s)、Y2(s),进行反拉氏变换后分别获得新的y1、y2Among them, Y(s) is the frequency domain expression of the signal after filtering, ω is the cutoff frequency. When its value is less than the frequency of the noise signal, the filtering effect is better. Through the above transfer function, the output Y(s) can be obtained and recorded as Y 1 (s) and Y 2 (s), and the new y 1 and y 2 are obtained after inverse Laplace transform.

然后构建非线性扩张状态观测器:Then construct the nonlinear extended state observer:

e=z1-ye=z 1 -y

Figure BDA0003973861650000065
Figure BDA0003973861650000065

Figure BDA0003973861650000066
Figure BDA0003973861650000066

Figure BDA0003973861650000067
Figure BDA0003973861650000067

其中,本实施例中设定β1=100,β2=300,β3=1000,δ1=0.01,α1=0.5,α2=0.25,饱和函数fal(e,α1,δ)的作用为抑制信号抖振,表示为:In this embodiment, β 1 =100, β 2 =300, β 3 =1000, δ 1 =0.01, α 1 =0.5, α 2 =0.25 are set, and the saturation function fal(e, α 1 , δ) is used to suppress signal jitter, which is expressed as:

Figure BDA0003973861650000068
Figure BDA0003973861650000068

则有z1(t)→x1(t),z2(t)→x2(t),z3(t)→f。Then z 1 (t)→x 1 (t), z 2 (t)→x 2 (t), z 3 (t)→f.

将经过滤波后的线偏差数据y1、y2分别带入扩张状态观测器中的变量y,解得到扩张状态观测器算出的z3,记为

Figure BDA0003973861650000069
有Substitute the filtered line deviation data y 1 and y 2 into the variable y in the extended state observer, and solve for z 3 calculated by the extended state observer, which is recorded as
Figure BDA0003973861650000069
have

Figure BDA0003973861650000071
Figure BDA0003973861650000071

步骤三,基于所述分量Fx2、Fy2和所述扩张状态观测器算出的

Figure BDA0003973861650000075
计算δ,联立求解得滚转角测量误差δ:Step 3: Based on the components F x2 , F y2 and the extended state observer,
Figure BDA0003973861650000075
Calculate δ and solve the roll angle measurement error δ:

Figure BDA0003973861650000072
Figure BDA0003973861650000072

步骤四,重复步骤一至步骤三共N次,对获得的结果进行平均值滤波,获得最终的滚转角测量误差估计值

Figure BDA0003973861650000073
由于线偏差测量噪声的存在,求得的滚转角测量误差会在一定范围内振荡,为了进一步获得准确的滚转角测量误差,需要得到的结果进行平均值滤波,所述平均值滤波计算过程如下:Step 4: Repeat steps 1 to 3 for a total of N times, perform average filtering on the obtained results, and obtain the final roll angle measurement error estimate.
Figure BDA0003973861650000073
Due to the existence of line deviation measurement noise, the roll angle measurement error obtained will oscillate within a certain range. In order to further obtain an accurate roll angle measurement error, the result needs to be averaged and filtered. The average filtering calculation process is as follows:

Figure BDA0003973861650000074
Figure BDA0003973861650000074

其中N为重复次数,δn为第n次过程计算得到的滚转角测量误差,

Figure BDA0003973861650000076
为最终求得的滚转角测量误差估计值。Where N is the number of repetitions, δn is the roll angle measurement error calculated in the nth process,
Figure BDA0003973861650000076
is the final estimated value of the roll angle measurement error.

对于本发明中提到的重力、重力补偿和控制力应作广义理解,当激光束非水平时,上述作用力应理解为实际作用力在垂直于激光束平面内的分量。The gravity, gravity compensation and control force mentioned in the present invention should be understood in a broad sense. When the laser beam is non-horizontal, the above-mentioned force should be understood as the component of the actual force in the plane perpendicular to the laser beam.

以上所述,仅为本发明的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,可轻易想到的变化或替换,都应涵盖在本发明的保护范围之内。因此,本发明的保护范围应以权利要求的保护范围为准。The above is only a specific embodiment of the present invention, but the protection scope of the present invention is not limited thereto. Any changes or substitutions that can be easily thought of by a person skilled in the art within the technical scope disclosed by the present invention should be included in the protection scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the claims.

Claims (5)

1. A rolling missile rolling angle measurement error estimation method containing line deviation measurement noise is characterized by comprising the following steps:
step one, a laser receiving device on the missile processes the received laser signals to obtain line deviations delta x and delta y between missile targets, and a controller on the missile obtains a sub-control force F according to the missile control force x2 、F y2
Inputting the line deviation into a second-order low-pass filter and then into a nonlinear extended state observer to obtain the calculated extended state observer
Figure FDA0003973861640000011
Step three, based on the sub-control force F x2 、F y2 Missile mass m and calculated by the extended state observer
Figure FDA0003973861640000012
Calculating a roll angle measurement error delta;
repeating the steps for one to four times for N times, and carrying out average value filtering on the obtained result to obtain a final roll angle measurement error estimated value
Figure FDA0003973861640000013
2. The method of claim 1, wherein the transfer function of the second order low pass filter is:
Figure FDA0003973861640000014
wherein Y (S) is the expression of the filtered signal in the frequency domain, S is the complex parameter, ω is the cut-off frequency, and R (S) is the expression of the filtered signal in the frequency domain after Law transformation.
3. The method of claim 1, wherein the nonlinear extended state observer:
e=z 1 -y
Figure FDA0003973861640000015
Figure FDA0003973861640000016
Figure FDA0003973861640000017
wherein beta is 1 ,β 2 ,β 3 ,δ 1 ,α 1 ,α 2 For the set value, the saturation function fal (e, alpha 11 ) Is expressed as:
Figure FDA0003973861640000018
saturation function fal (e, alpha 21 ) Is expressed as:
Figure FDA0003973861640000021
where sgn (e) is a sign function, outputting the sign of e.
4. A method according to claims 1-3, wherein the linear deviation is input into a second order low pass filter and then into a nonlinear extended state observer to obtain the calculated extended state observer
Figure FDA0003973861640000022
The method comprises the following steps:
the line deviations Deltax and Deltay are input into a second-order low-pass filter as R(s) after being subjected to Law transformation, and the obtained outputs Y(s) are respectively marked as Y 1 (s)、Y 2 (s) for Y 1 (s)、Y 2 (s) carrying out inverse Laplace transformation and then respectively taking the inverse Laplace transformation into the variable y in the extended state observer to obtain z 3 Respectively marked as
Figure FDA0003973861640000023
5. The method of claim 1, wherein the component F based x2 、F y2 Missile mass m and calculated by the extended state observer
Figure FDA0003973861640000024
Calculating a roll angle measurement error delta, including based on the component F x2 、F y2 Missile mass m and +.>
Figure FDA0003973861640000025
Figure FDA0003973861640000026
Simultaneous solution to obtain roll angle measurement error delta:
Figure FDA0003973861640000027
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