CN115639556A - Optimizing method of imaging zone in non-track-curved imaging mode of spaceborne SAR - Google Patents
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Abstract
本发明提出了一种星载SAR非沿迹弯曲成像模式成像带优化方法,能够解决星载SAR非沿迹弯曲成像模式中存在波束机动约束时多目标观测成像带设计难、目标点偏差大的问题,实现多目标观测成像带优化。本发明先对非沿迹分布的目标点进行观测顺序规划,随后首次给出了波束姿态角及其高阶导数的解析表达式,在此基础提出了波足循迹算法与偏差点最小准则以设计生成符合波束机动约束的最优非沿迹成像带,解决星载SAR非沿迹弯曲成像模式中存在波束机动约束时多目标观测成像带设计难、目标点偏差大的问题,同时避免了通过仿真计算姿态角产生的计算资源大量损耗,实现星载SAR非沿迹弯曲成像模式多目标观测成像带优化。
The present invention proposes a method for optimizing the imaging zone of the spaceborne SAR non-track-curving imaging mode, which can solve the problems of difficult design of multi-target observation imaging zone and large target point deviation when there are beam maneuver constraints in the space-borne SAR non-track-curving imaging mode. To solve the problem, realize the optimization of multi-objective observation imaging zone. The invention firstly plans the observation order of the target points not distributed along the track, and then gives the analytical expression of the beam attitude angle and its high-order derivative for the first time, and proposes the wave foot tracking algorithm and the minimum deviation point criterion on this basis. Design and generate the optimal non-along-track imaging zone that conforms to the beam maneuvering constraints, and solve the problems of difficult design of multi-target observation imaging zone and large target point deviation when there are beam maneuvering constraints in the spaceborne SAR non-along-track bending imaging mode. A large amount of computing resources are consumed by the simulation calculation of the attitude angle, and the optimization of the multi-target observation imaging zone of the spaceborne SAR non-along-track bending imaging mode is realized.
Description
技术领域technical field
本发明涉及合成孔径雷达(Synthetic Aperture Radar,简称SAR)技术领域,具体涉及一种星载SAR非沿迹弯曲成像模式成像带优化方法。The invention relates to the technical field of Synthetic Aperture Radar (SAR for short), in particular to a method for optimizing an imaging zone of a spaceborne SAR non-along-track curved imaging mode.
背景技术Background technique
非沿迹成像模式是星载SAR的一种特有的工作模式。相对于传统星载SAR,星载非沿迹SAR通过连续调整俯仰维、方位维波束指向,直接生成沿目标地形的测绘带,而不是传统的沿卫星轨道生成测绘带,这使得其在对某些“非沿卫星航迹场景”如地震带、海岸线成像时从根本上减少了回波数据冗余度,显著提高星载SAR对狭长场景的观测效率,具有独特的优势。The non-track imaging mode is a unique working mode of spaceborne SAR. Compared with the traditional space-borne SAR, the space-borne off-track SAR can directly generate the mapping strip along the target terrain by continuously adjusting the beam pointing in the elevation dimension and the azimuth dimension, instead of the traditional generation of the mapping strip along the satellite orbit, which makes it useful for certain Some "non-satellite track scenarios" such as seismic belts and coastline imaging fundamentally reduce the redundancy of echo data, and significantly improve the observation efficiency of spaceborne SAR for narrow and long scenes, which has unique advantages.
在数据获取期间,卫星一般通过控制波束姿态角进行观测。由于“斜向场景”走向大多是不规则的,这导致数据获取期间需要同时对波束姿态角及其高阶导数进行设计以生成不规则的测绘带。同时,卫星载荷也会对波束姿态角及其高阶导数提出约束以保证卫星安全、稳定的运行。因此,如何在给定的波束姿态角及其高阶导数约束下实现沿场景的测绘带规划成为了非沿迹成像模式需要解决的重要问题。而传统方法均由于缺乏理论指导与相关算法支撑,普遍在设计中不对波束机动加以考虑,而是在设计完成后再判断是否符合约束,由此产生成像带规划难、目标点偏差大等问题。During data acquisition, satellites generally make observations by controlling the beam attitude angle. Since the direction of the "oblique scene" is mostly irregular, it is necessary to simultaneously design the beam attitude angle and its higher-order derivatives during data acquisition to generate irregular swaths. At the same time, the satellite load will also impose constraints on the beam attitude angle and its high-order derivatives to ensure the safe and stable operation of the satellite. Therefore, how to realize the swath planning along the scene under the given beam attitude angle and its higher-order derivative constraints has become an important problem to be solved in the non-track imaging mode. However, due to the lack of theoretical guidance and related algorithm support, the traditional methods generally do not consider beam maneuvering in the design, but judge whether the constraints are met after the design is completed, resulting in problems such as difficult imaging zone planning and large deviation of target points.
发明内容Contents of the invention
有鉴于此,本发明提出了一种星载SAR非沿迹弯曲成像模式成像带优化方法,能够解决星载SAR非沿迹弯曲成像模式中存在波束机动约束时多目标观测成像带设计难的问题,实现多目标观测成像带优化。In view of this, the present invention proposes a method for optimizing the imaging zone of the spaceborne SAR non-curving along the track imaging mode, which can solve the problem of difficult design of the imaging zone for multi-object observation when there are beam maneuver constraints in the non-curving along the track imaging mode of the spaceborne SAR , to realize the optimization of multi-objective observation imaging band.
为实现上述目的,本发明的一种星载SAR非沿迹弯曲成像模式成像带优化方法,包括如下步骤:In order to achieve the above object, a method for optimizing the imaging zone of a spaceborne SAR non-along-track curved imaging mode of the present invention comprises the following steps:
步骤一、规划输入的目标点集合,生成若干目标点序列;
步骤二,建立坐标系,得到波束姿态角及其高阶导数的解析表达;
步骤三,输入目标点序列,依据波足循优算法流程求解符合波束姿态角约束下的可行波足轨迹;所述波足循优算法流程为:输入卫星开机时间以及步骤一中生成的目标点序列,从当前点开始计算下一时刻波足可选运动方向的位置、速度和加速度,根据步骤二得到的波束姿态角及其高阶导数的解析表达,计算各可选方向波足姿态角及其高阶导数,基于姿态约束筛选出下一时刻的波足运动方向,然后判断是否遍历所有目标点,若是则输出波足轨迹,否则判断是否切换循迹目标点,若是则将下一目标点设为循迹目标,然后返回重新计算下一时刻波足可选运动方向的位置、速度和加速度,否则直接返回重新计算下一时刻波足可选运动方向的位置、速度和加速度,直至遍历所有目标点,输出波足轨迹;Step 3: Input the sequence of target points, and solve the feasible wave foot trajectory that meets the constraints of the beam attitude angle according to the wave foot optimization algorithm flow; the wave foot optimization algorithm flow is: input the satellite startup time and the target points generated in step Sequence, starting from the current point to calculate the position, velocity and acceleration of the optional movement direction of the wave foot at the next moment, according to the analytical expression of the beam attitude angle and its high-order derivative obtained in
步骤四,改变循迹目标的切换判据中的判断阈值,对波足循优算法中相关参数进行迭代,根据目标点偏差最小准则选出最优波足轨迹。Step 4: Change the judgment threshold in the switching criterion of the tracking target, iterate the relevant parameters in the wave foot tracking optimization algorithm, and select the optimal wave foot trajectory according to the minimum deviation criterion of the target point.
其中,波束姿态角与观测构型特征角的解析关系如下:Among them, the analytical relationship between the beam attitude angle and the observation configuration characteristic angle is as follows:
其中β为下视角,β′为包含左右视信息的下视角,当右视时β′=β,左视时β′=-β;γ为斜视角在星下点所在的地球切面的投影;η为波束投影角,用来表征投影椭圆的旋转角度,可在观测期间自行设定以权衡幅宽、方位分辨率;β、γ、η统称为观测构型特征角;为滚转角,θ为俯仰角,ψ为偏航角,统称为波束姿态角;Wherein β is the downward angle of view, and β' is the downward angle of view that includes the information of the left and right views, when the right view is β'=β, and when the left view is β'=-β; η is the beam projection angle, which is used to represent the rotation angle of the projected ellipse, which can be set during the observation period to balance the width and azimuth resolution; β, γ, and η are collectively referred to as the observation configuration characteristic angle; is the roll angle, θ is the pitch angle, and ψ is the yaw angle, collectively referred to as the beam attitude angle;
对波束姿态角与观测构型特征角的解析关系式分别取一阶和二阶微分得到波束姿态角的高阶形式,分别为:The high-order form of the beam attitude angle is obtained by taking the first-order and second-order differentials of the analytical relational expressions of the beam attitude angle and the observation configuration characteristic angle, respectively:
其中,所述波足循优算法具体包括如下步骤:Wherein, the wave-foot-based optimization algorithm specifically includes the following steps:
首先输入步骤一中生成的目标点序列及卫星开机时间等参数,然后计算波足可选运动方向:First input the target point sequence generated in
其中Pfoot.f(i)为第i时刻波足地固系位置,pi为其单位向量;PT(j)为第j个循迹目标地固系位置,满足j∈[1,2,…,M],M为目标点个数;两向量所在的平面的法向量为nij;vij为地球表面上从Pfoot.f(i)到PT(j)的单位方向向量;||·||2为二范数算子;vi为第i时刻波足地固系速度的单位向量;kij为vij与vi的夹角;N为波足可选运动方向数量,n为可选运动方向序号,满足n∈[1,2,…,N],k(n)为第n个可选方向所对夹角;v′ij(n)表示第i时刻对地固系中第j个目标的第n个可选方向的单位向量,HY(θ)代表以Y轴正方向为轴,沿着右手定则的正方向将坐标轴旋转θ度;where P foot.f (i) is the fixed position of the wave foot at the i-th moment, and p i is its unit vector; P T (j) is the fixed position of the jth tracking target, satisfying j∈[1,2 ,...,M], M is the number of target points; the normal vector of the plane where the two vectors are located is n ij ; v ij is the unit direction vector from P foot.f (i) to P T (j) on the surface of the earth; ||·|| 2 is the two-norm operator; v i is the unit vector of the ground-solid velocity of the wave foot at the i-th moment; k ij is the angle between v ij and v i ; N is the number of optional motion directions of the wave foot , n is the serial number of the optional motion direction, satisfying n∈[1,2,…,N], k(n) is the angle opposite to the nth optional direction; v′ ij (n) represents the The unit vector of the n-th optional direction of the j-th target in the solid system, H Y (θ) represents the positive direction of the Y-axis as the axis, and rotates the coordinate axis by θ degrees along the positive direction of the right-hand rule;
V′ij(n)表示第i时刻对地固系中第j个目标的第n个可选方向的速度;a′ij(n)表示使用V′ij(n)后第i时刻对地固系中第j个目标的加速度;P′ij(n)表示使用V′ij(n)和a′ij(n)后第i+1时刻波足地固系坐标,Vfoot.f(i)为为第i时刻波足地固系速度,dt为时间微分;V' ij (n) represents the speed of the nth optional direction of the jth target in the ground-fixed system at the i -th moment; a' ij (n) represents the ground-fixed The acceleration of the jth target in the system; P′ ij (n) represents the ground-solid system coordinates of the wave foot at the i+1th moment after using V′ ij (n) and a′ ij (n), V foot.f (i) is the velocity of the wave-foot ground solid system at the i-th moment, and dt is the time differential;
将P′ij(n)、V′ij(n)、a′ij(n)带入步骤二得到的解析表达,直接求出各个可选方向的姿态角及其一、二阶导数,再依据选出符合卫星姿态角约束下的最优方向的序号ni,其中F(·)为姿态角约束,G(·)为姿态角变化速度约束,H(·)为姿态角变化加速度约束,进而确定第i时刻的加速度,第i+1时刻波足在地固系的位置、速度 Put P′ ij (n), V′ ij (n), a′ ij (n) into the analytical expression obtained in
其中,所述循迹目标的切换判据为:Wherein, the switching criterion of the tracking target is:
其中Pfoot.f(i)为第i时刻波足地固系位置,PT(j)为第j个循迹目标地固系位置,满足j∈[1,2,...,M],M为目标点个数;vij为地球表面上从Pfoot.f(i)到PT(j)的单位方向向量;||·||2为二范数算子;Rset为设置的长度阈值,其取值范围在一个距离幅宽内;vi为第i时刻波足地固系速度的单位向量,上标H表示转置。where P foot.f (i) is the fixed position of the wave foot at the i-th moment, and P T (j) is the fixed position of the jth tracking target, satisfying j∈[1,2,...,M] , M is the number of target points; v ij is the unit direction vector from P foot.f (i) to P T (j) on the earth's surface; ||·|| 2 is the two-norm operator; R set is the setting The length threshold of , and its value range is within a distance width; v i is the unit vector of the wave-foot ground-solid velocity at the i-th moment, and the superscript H represents transposition.
其中,目标点规划方法流程包括目标点聚类以及目标序列划分;其中,目标点聚类具体步骤为:Among them, the target point planning method process includes target point clustering and target sequence division; wherein, the specific steps of target point clustering are:
步骤11,对集合中所有点标号为1,2,...,M,并计算目标点集合中每个点到所有点的距离,并与聚类阈值比较,若小于该阈值则判为1,反之为0;将结果按目标点序号放入一个M×M的矩阵中,生成目标距离矩阵;Step 11, label all points in the set as 1, 2, ..., M, and calculate the distance from each point in the target point set to all points, and compare it with the clustering threshold, if it is less than the threshold, it will be judged as 1 , otherwise it is 0; put the result into an M×M matrix according to the target point number to generate the target distance matrix;
步骤12,从第一行开始,找到矩阵中数值为1的元素所对的列号i,j,k,...,记录该序号并将第i,j,k,...行和第i,j,k,...列的所有元素置为0;
步骤13,将步骤12重复M次,遍历目标距离矩阵的所有行,记录的所有序号即为被聚类的点;Step 13, repeating step 12 M times, traversing all the rows of the target distance matrix, and all the serial numbers recorded are the clustered points;
目标序列划分具体步骤为:The specific steps of target sequence division are as follows:
步骤21,对聚类后的所有目标点从低纬到高纬排序,设点集为T={T1,T2,...,TN};Step 21, sort all target points after clustering from low latitude to high latitude, set point set as T={T 1 , T 2 ,...,T N };
步骤22,令S1(1)=T1,i=1,j=2,依据如下判断条件:Step 22, set S 1 (1)=T 1 , i=1, j=2, according to the following judgment conditions:
若满足则令S1(i+1)=Tj,若不满足则令j=j+1,其中S1(i)为划分出的第一个序列的第i个目标点;重复上述操作直到j=N,即可得到所划分出的目标序列S1;If it is satisfied, set S 1 (i+1)=T j , if it is not satisfied, set j=j+1, where S 1 (i) is the i-th target point of the first sequence divided; repeat the above operations Until j=N, the divided target sequence S 1 can be obtained;
步骤23,设T1=T-S1,对T1执行步骤22得到S2和T2,重复步骤22直到则输出所划分出的k个目标序列。Step 23, set T 1 =TS 1 , perform step 22 on T 1 to obtain S 2 and T 2 , repeat step 22 until Then output the divided k target sequences.
其中,所述目标点偏差最小准则为:Wherein, the minimum criterion of the target point deviation is:
其中,L′foot.f(Rset)为拟合后的波足轨迹,为基于该准则得到的最佳阈值,inf(·)为求函数下确界.Among them, L′ foot.f (R set ) is the fitted wave foot trajectory, is the optimal threshold obtained based on this criterion, and inf( ) is the infimum of the function.
有益效果:Beneficial effect:
本发明先对非沿迹分布的目标点进行观测顺序规划,随后首次给出了波束姿态角及其高阶导数的解析表达式,在此基础提出了波足循迹算法与偏差点最小准则以设计生成符合波束机动约束的最优非沿迹成像带,解决星载SAR非沿迹弯曲成像模式中存在波束机动约束时多目标观测成像带设计难、目标点偏差大的问题,同时避免了通过仿真计算姿态角产生的计算资源大量损耗,实现星载SAR非沿迹弯曲成像模式多目标观测成像带优化。The invention firstly plans the observation order of the target points not distributed along the track, and then gives the analytical expression of the beam attitude angle and its high-order derivative for the first time, and on this basis, proposes the wave foot tracking algorithm and the minimum deviation point criterion to Design and generate the optimal non-along-track imaging zone that conforms to the beam maneuvering constraints, and solve the problems of difficult design of multi-target observation imaging zone and large target point deviation when there are beam maneuvering constraints in the spaceborne SAR non-along-track bending imaging mode. A large amount of computing resources are consumed by the simulation calculation of the attitude angle, and the optimization of the multi-target observation imaging zone of the spaceborne SAR non-along-track bending imaging mode is realized.
附图说明Description of drawings
图1是本发明所述星载SAR非沿迹弯曲成像模式多目标观测成像带优化方法的流程图。Fig. 1 is a flow chart of the method for optimizing the multi-target observation imaging zone in the spaceborne SAR non-along-track curved imaging mode of the present invention.
图2是本发明所述目标点规划方法流程图。Fig. 2 is a flow chart of the target point planning method of the present invention.
图3是本发明所述星载SAR非沿迹弯曲成像模式观测构型示意图。Fig. 3 is a schematic diagram of the observation configuration of the spaceborne SAR non-track-curving imaging mode according to the present invention.
图4是本发明所述波足循优算法流程图。Fig. 4 is a flow chart of wave foot optimization algorithm in the present invention.
图5是本发明实施例中采用本发明所述方法与传统方法的规划结果及目标覆盖情况。Fig. 5 shows the planning results and target coverage of the method of the present invention and the traditional method in the embodiment of the present invention.
图6是本发明实施例中本发明所述方法与传统方法的波束姿态角及其一、二阶导数对比图。Fig. 6 is a comparison diagram of the beam attitude angle and its first and second order derivatives between the method of the present invention and the traditional method in the embodiment of the present invention.
图7是本发明实施例中采用波束姿态角及其一、二阶导数解析表达式与代码仿真结果误差。Fig. 7 is the error of the analytical expression of the beam attitude angle and its first and second order derivatives and the code simulation results used in the embodiment of the present invention.
具体实施方式Detailed ways
下面结合附图并举实施例,对本发明进行详细描述。The present invention will be described in detail below with reference to the accompanying drawings and examples.
在星载SAR非沿迹弯曲成像模式中,传统的成像带设计方法在设计时不考虑波束机动约束,设计结果往往不满足实际波束机动约束导致无法使用;此外,其设计结果距目标点偏差较大,在数据获取时极易丢失目标。本发明所提方法首先对任务目标进行规划,随后基于所提的波足寻优算法得到满足波束机动约束的波足轨迹,再基于偏差点最小准则迭代给出最优的多目标观测成像带设计结果,解决了传统方法中设计实现难、目标点偏差大的问题。本发明所述星载SAR非沿迹弯曲成像模式多目标观测成像带优化方法的流程图如图1所示,本发明包括如下步骤:In the non-track-curving imaging mode of spaceborne SAR, the traditional imaging zone design method does not consider the beam maneuvering constraints in the design, and the design results often do not meet the actual beam maneuvering constraints and cannot be used; in addition, the design results are far from the target point. Large, it is easy to lose the target during data acquisition. The method proposed in the present invention first plans the mission target, then obtains the wave foot trajectory satisfying the beam maneuvering constraints based on the proposed wave foot optimization algorithm, and then iteratively gives the optimal multi-object observation imaging zone design based on the minimum deviation point criterion As a result, the problems of difficult design and realization and large deviation of target points in traditional methods are solved. The flow chart of the method for optimizing the multi-target observation imaging zone of the space-borne SAR non-along-track curved imaging mode described in the present invention is shown in Figure 1, and the present invention includes the following steps:
步骤一、规划输入的目标点集合,生成若干目标点序列;
目标点规划方法流程如图2所示,包括目标点聚类以及目标序列划分。其中,目标点聚类具体步骤为:The process flow of the target point planning method is shown in Figure 2, including target point clustering and target sequence division. Among them, the specific steps of target point clustering are:
步骤11,对集合中所有点标号为1,2,...,M(M为目标点总数)并计算目标点集合中每个点到所有点的距离,并与聚类阈值比较,若小于该阈值则判为1,反之为0。将结果按目标点序号放入一个M×M的矩阵中,生成目标距离矩阵;Step 11, label all points in the set as 1, 2, ..., M (M is the total number of target points) and calculate the distance from each point in the target point set to all points, and compare with the clustering threshold, if less than The threshold is judged as 1, otherwise it is 0. Put the result into an M×M matrix according to the target point number to generate a target distance matrix;
步骤12,从第一行开始,找到矩阵中数值为1的元素所对的列号i,j,k,...,记录该序号并将第i,j,k,...行和第i,j,k,...列的所有元素置为0;
步骤13,将步骤12重复M次,遍历目标距离矩阵的所有行,记录的所有序号即为被聚类的点。Step 13, repeating step 12 M times, traversing all the rows of the target distance matrix, and all the serial numbers recorded are the points to be clustered.
目标序列划分具体步骤为:The specific steps of target sequence division are as follows:
步骤21,对聚类后的所有目标点从低纬到高纬排序,设点集为T={T1,T2,...,TN}。Step 21, sort all target points after clustering from low latitude to high latitude, and set the point set as T={T 1 , T 2 , . . . , T N }.
步骤22,令S1(1)=T1,i=1,j=2,依据式(1)给出的判断条件,若满足则令S1(i+1)=Tj,若不满足则令j=j+1,其中S1(i)为划分出的第一个序列的第i个目标点。重复上述操作直到j=N,即可得到所划分出的目标序列S1。Step 22, set S 1 (1)=T 1 , i=1, j=2, according to the judgment condition given by formula (1), if it is satisfied, then set S 1 (i+1)=T j , if not Then let j=j+1, wherein S 1 (i) is the i-th target point of the first divided sequence. By repeating the above operations until j=N, the divided target sequence S 1 can be obtained.
步骤23,设T1=T-S1,对T1执行步骤22可得到S2和T2,重复步骤22直到则输出所划分出的k个目标序列。Step 23, set T 1 =TS 1 , execute step 22 on T 1 to obtain S 2 and T 2 , repeat step 22 until Then output the divided k target sequences.
步骤二、建立坐标系,得到波束姿态角及其高阶导数的解析表达,具体过程如下:
首先建立卫星轨道坐标系、SAR坐标系,其定义如下所示:卫星轨道坐标系中,X轴方向为卫星运动速度方向;Z轴矢量在卫星轨道平面内且指向地心;Y轴按照右手法则求解;SAR天线坐标系中,X轴正方向与卫星运动方向同向,XOZ面为天线沿方位向的剖面;Z轴为天线波束中心指向。First establish the satellite orbit coordinate system and the SAR coordinate system, which are defined as follows: in the satellite orbit coordinate system, the X-axis direction is the direction of the satellite motion velocity; the Z-axis vector is in the satellite orbit plane and points to the center of the earth; the Y-axis follows the right-hand rule Solution: In the SAR antenna coordinate system, the positive direction of the X-axis is in the same direction as the satellite motion direction, and the XOZ plane is the section of the antenna along the azimuth direction; the Z-axis is the center pointing of the antenna beam.
波束姿态角是偏航、俯仰、滚转角的总称,用来描述卫星波束指向对于卫星本体的相对关系,即描述从卫星轨道坐标系到SAR天线坐标系的转移矩阵。如式(2)所示,采取3-2-1转序(偏航-俯仰-滚转),其中为滚转角,θ(t)为俯仰角,ψ(t)为偏航角,HX(θ)代表以X轴正方向为轴,沿着右手定则的正方向将坐标轴旋转θ度,HY(θ)和HZ(θ)的定义与之类似。Beam attitude angle is a general term for yaw, pitch, and roll angles, which is used to describe the relative relationship between the satellite beam pointing to the satellite body, that is, to describe the transfer matrix from the satellite orbit coordinate system to the SAR antenna coordinate system. As shown in formula (2), a 3-2-1 rotation sequence (yaw-pitch-roll) is adopted, where is the roll angle, θ(t) is the pitch angle, ψ(t) is the yaw angle, H X (θ) represents the positive direction of the X-axis as the axis, and rotates the coordinate axis by θ degrees along the positive direction of the right-hand rule, H Y (θ) and H Z (θ) are defined similarly.
同样的,卫星轨道坐标系与SAR天线坐标系的相对关系可以由图3所示的星载SAR观测构型得到,其中卫星轨道坐标系为X-Y-Z、SAR天线坐标系为r1-r2-r3;天线距离向平面为r2-o-r3;天线方位向平面为r1-o-r3;β为下视角;γ为斜视角在星下点所在的地球切面(平行于X-O-Y面)的投影;η为Y轴与天线距离向平面和X-O-Z的交线形成夹角,称为波束投影角,用来表征投影椭圆的旋转角度;β、γ、η统称为观测构型特征角。波束姿态角与观测构型特征角的解析关系如式(3)所示,其中β′为包含左右视信息的下视角,当右视时β′=β,左视时β′=-β。Similarly, the relative relationship between the satellite orbit coordinate system and the SAR antenna coordinate system can be obtained from the spaceborne SAR observation configuration shown in Figure 3, where the satellite orbit coordinate system is XYZ, and the SAR antenna coordinate system is r 1 -r 2 -r 3 ; the antenna distance plane is r 2 -or 3 ; the antenna azimuth plane is r 1 -or 3 ; β is the downward angle of view; η is the angle formed by the Y-axis and the intersection line of the antenna distance plane and XOZ, which is called the beam projection angle, and is used to represent the rotation angle of the projected ellipse; β, γ, and η are collectively called the observation configuration characteristic angle. The analytical relationship between the beam attitude angle and the observation configuration characteristic angle is shown in formula (3), where β' is the downward viewing angle including the left and right view information, and β'=β for the right view, and β'=-β for the left view.
对式(3)分别取一阶、二阶微分可以得到波束姿态角的高阶形式,如式(4)、(5)所示。The high-order form of the beam attitude angle can be obtained by taking the first-order and second-order differentials of equation (3), as shown in equations (4) and (5).
式(3)中η可在观测期间自行设定以权衡幅宽、方位分辨率;β、γ解析表达式则由式(6)给出,其中k1,k2,k3为卫星轨道系的三个坐标轴在地惯系的单位列向量;L3为卫星到波足的位置向量。β、γ的一、二阶导数由式(7)、(8)给出。In Equation (3), η can be set during the observation period to balance the width and azimuth resolution; the analytical expressions of β and γ are given by Equation (6), where k 1 , k 2 , and k 3 are satellite orbit systems The unit column vector of the three coordinate axes in the geo-inertial system; L 3 is the position vector from the satellite to the wave foot. The first and second derivatives of β and γ are given by formulas (7) and (8).
式(7)、(8)中k1,k2,k3与L3的一、二阶导数如式(9)~(11)所示,其中ω为卫星轨道平均角速度;we为地球自转角速度;Pfoot(t)和Psat(t)分别为t时刻波足和卫星的地惯系位置坐标,asat(t)为波足地惯系加速度;||·||2为二范数算子;P⊥Z为XOY面投影矩阵;Pfoot.f(t)、Vfoot.f(t)、afoot.f(t)为地固系下波足位置;Hecef2eci(t)为t时刻地固系到地惯系转移矩阵。The first and second derivatives of k 1 , k 2 , k 3 and L 3 in formulas (7) and (8) are shown in formulas (9) to (11), where ω is the average angular velocity of the satellite orbit; w e is the earth’s Angular velocity of rotation; P foot (t) and P sat (t) are the position coordinates of the wave foot and the satellite’s inertial system at time t respectively, a sat (t) is the acceleration of the ground inertial system of the wave foot; ||·|| 2 is two Norm operator; P ⊥Z is the XOY plane projection matrix; P foot.f (t), V foot.f (t), a foot.f (t) are the wave foot positions under the ground-solid system; H ecef2eci (t ) is the transfer matrix from the fixed system to the inertial system at time t.
根据式(3)~(11)即可用某瞬时时刻地固系波足位置、速度、加速度直接求得该时刻下波束姿态角(偏航、俯仰、滚转)的值及其一、二阶导数,从而为测绘带规划提供支撑。According to formulas (3)-(11), the value of the beam attitude angle (yaw, pitch, roll) and its first and second orders can be obtained directly by using the position, velocity, and acceleration of the ground wave foot at a certain instant. Derivatives, thus providing support for swath planning.
步骤三、输入目标点序列,依据波足循优算法流程求解符合波束姿态角约束下的可行波足轨迹;Step 3: Input the target point sequence, and solve the feasible wave foot trajectory under the constraints of the beam attitude angle according to the wave foot follow-through algorithm process;
波足循优算法流程图如图4所示,具体包括如下步骤:The flow chart of wave foot optimization algorithm is shown in Figure 4, which specifically includes the following steps:
首先输入步骤一中生成的目标点序列及卫星开机时间等参数,然后计算波足可选运动方向,如式(12)~(14)所示。其中Pfoot.f(i)为第i时刻波足地固系位置,pi为其单位向量;PT(j)为第j个循迹目标地固系位置,满足j∈[1,2,...,M],M为目标点个数;两向量所在的平面的法向量为nij;vij为地球表面上从Pfoot.f(i)到PT(j)的单位方向向量;||·||2为二范数算子。First input the target point sequence generated in
vi为第i时刻波足地固系速度的单位向量;kij为vij与vi的夹角;N为波足可选运动方向数量,n为可选运动方向序号,满足n∈[1,2,...,N],k(n)为第n个可选方向所对夹角;v′ij(n)表示第i时刻对地固系中第j个目标的第n个可选方向的单位向量。v i is the unit vector of the ground-solid velocity of the wave foot at the i-th moment; k ij is the angle between v ij and v i ; N is the number of optional movement directions of the wave foot, and n is the number of the optional movement direction, satisfying n∈[ 1,2,...,N], k(n) is the angle opposite to the nth optional direction; v′ ij (n) represents the nth Unit vector for optional orientation.
V′ij(n)表示第i时刻对地固系中第j个目标的第n个可选方向的速度;a′ij(n)表示使用V′ij(n)后第i时刻对地固系中第j个目标的加速度;P′ij(n)表示使用V′ij(n)和a′ij(n)后第i+1时刻波足地固系坐标,Vfoot.f(i)为为第i时刻波足地固系速度。V' ij (n) represents the speed of the nth optional direction of the jth target in the ground-fixed system at the i -th moment; a' ij (n) represents the ground-fixed The acceleration of the jth target in the system; P′ ij (n) represents the ground-solid system coordinates of the wave foot at the i+1th moment after using V′ ij (n) and a′ ij (n), V foot.f (i) is the fixed velocity of wave feet at the i-th moment.
将式(15)中P′ij(n)、V′ij(n)、a′ij(n)带入步骤二可以直接求出各个可选方向的姿态角及其一、二阶导数,再依据式(16)选出符合卫星姿态角约束下的最优方向的序号ni,其中F(·)为姿态角约束,G(·)为姿态角变化速度约束,H(·)为姿态角变化加速度约束。进而确定了第i时刻的加速度,第i+1时刻波足在地固系的位置、速度,如式(17)所示。Bringing P′ ij (n), V′ ij (n), and a′ ij (n) in formula (15) into
循迹目标的切换判据如式(18)所示,满足该式的任一条件即可进行循迹目标的切换,其中Rset为设置的长度阈值,其取值范围在一个距离幅宽内。The switching criterion of the tracking target is shown in formula (18). The tracking target can be switched if any condition of the formula is satisfied, where R set is the set length threshold, and its value range is within a distance width .
步骤四、对波足循优算法中相关参数进行迭代,根据目标点偏差最小准则选出最优波足轨迹,具体如下:
设Lfoot.f(Rset)为采用式(18)中的长度阈值Rset循迹得到的波足轨迹。在实际应用中,需要对姿态角再进行多项式拟合以便于星上指令传输与控制,依据拟合出的姿态角可计算出拟合后的波足轨迹L′foot.f(Rset)。对Rset进行迭代,再依据式(19)中的目标点偏差最小准则即可选出最优波足轨迹其中为基于该准则得到的最佳阈值,inf(·)为求函数下确界。Let L foot.f (R set ) be the wave foot track obtained by using the length threshold R set in formula (18). In practical applications, it is necessary to perform polynomial fitting on the attitude angle to facilitate on-board command transmission and control, and the fitted wave foot trajectory L′ foot.f (R set ) can be calculated according to the fitted attitude angle. Iterate on R set , and then select the optimal wave foot trajectory according to the minimum criterion of the target point deviation in formula (19) in is the optimal threshold obtained based on this criterion, and inf(·) is the infimum of the function.
仿真实验:星载SAR非沿迹弯曲成像模式测绘带规划仿真参数如表1所示。Simulation experiment: Table 1 shows the simulation parameters of the surveying zone planning in the non-along-track curved imaging mode of spaceborne SAR.
表1星载SAR非沿迹弯曲成像模式测绘带规划仿真参数列表Table 1. Simulation parameter list of mapping zone planning in spaceborne SAR non-along-track curved imaging mode
首先,为验证星载SAR非沿迹弯曲成像模式多目标观测成像带优化方法在解决存在波束机动约束下沿场景多目标观测成像带设计难这一问题上的优势,在表1参数下使用传统成像带设计方法(即直接对点目标位置进行拟合的方法)对一组目标点(共29个)进行观测任务规划,其被划分为两个目标序列,如图5(a)所示。接下来我们以左侧的目标序列为例(即图5(b)中“*”所表示的21个目标点),对该组目标序列进行波足设计。本次仿真的卫星机动约束为:波束姿态角小于等于45deg,姿态角速度小于等于0.8deg/s,姿态角加速度小于等于0.08deg/s2。在图5(b)中分别给出采用传统方法(虚线)与本发明所提方法(实线)所规划的波足;图5(c)给出了21个目标点分别到上述两个测绘带波足中心的最短距离,其中“o”代表传统方法的,共有7个目标超出观测范围,“*”表示本发明所提方法的,仅有1个目标超出观测范围。两种方法的姿态角真值及其速度、加速度如图6所示,实线代表本发明所提算法生成结果,可以看到,上述两种算法均满足卫星机动约束,但本算法对机动约束要求更宽松,即做到覆盖目标更多且对波束机动要求更低,具有显著优势。此外,为验证波束姿态角及其一、二阶导数解析表达式的正确性。图7给出了采用本发明所提的波束姿态角及其一、二阶导数解析表达式与代码仿真所求的误差,可见波束姿态角误差在10-13度数量级,其一、二阶导数误差在10-4度数量级,远小于波束姿态角及其一、二阶导数的真值,验证了本发明所提解析表达式的正确性。First of all, in order to verify the advantages of the multi-target observation imaging zone optimization method of spaceborne SAR non-along-track curved imaging mode in solving the problem of difficult design of multi-target observation imaging zone along the scene under the constraint of beam maneuvering, the traditional The imaging zone design method (that is, the method of directly fitting the point target position) performs observation task planning on a set of target points (29 in total), which are divided into two target sequences, as shown in Fig. 5(a). Next, we take the target sequence on the left as an example (that is, the 21 target points represented by "*" in Figure 5(b)), and conduct wave foot design on this group of target sequences. The satellite maneuvering constraints for this simulation are: the beam attitude angle is less than or equal to 45deg, the attitude angular velocity is less than or equal to 0.8deg/s, and the attitude angular acceleration is less than or equal to 0.08deg/s 2 . In Fig. 5(b), the wave feet planned by the traditional method (dotted line) and the method proposed by the present invention (solid line) are shown respectively; Fig. 5(c) provides 21 target points respectively to the above two surveying and mapping The shortest distance with the center of the wave foot, where "o" represents that with the traditional method, a total of 7 targets are beyond the observation range, and "*" represents that with the method proposed by the present invention, only 1 target is beyond the observation range. The true value of the attitude angle and its velocity and acceleration of the two methods are shown in Figure 6. The solid line represents the results generated by the proposed algorithm of the present invention. It can be seen that the above two algorithms all meet the satellite maneuver constraints, but the algorithm does not require the maneuver constraints. The requirements are looser, that is, to cover more targets and have lower requirements for beam maneuvering, which has significant advantages. In addition, in order to verify the correctness of the analytical expressions of the beam attitude angle and its first and second derivatives. Fig. 7 has provided the error that adopts the beam attitude angle that the present invention proposes and its first, second order derivative analytical expression and code emulation seek, visible beam attitude angle error is on the order of magnitude of 10-13 degree, and its first, second order derivative The error is on the order of 10 -4 degrees, which is far smaller than the true value of the beam attitude angle and its first and second order derivatives, which verifies the correctness of the analytical expression proposed by the present invention.
综上所述,以上仅为本发明的较佳实施例而已,并非用于限定本发明的保护范围。凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。To sum up, the above are only preferred embodiments of the present invention, and are not intended to limit the protection scope of the present invention. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included within the protection scope of the present invention.
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