CN109521418A - Ground-based radar angle-measuring method based on interference field - Google Patents
Ground-based radar angle-measuring method based on interference field Download PDFInfo
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Abstract
一种基于干涉场的地基雷达测角方法,主要解决在远场、窄带条件下对待估计目标方位角测量精度的提高问题。本发明实现的步骤如下:(1)构建两部地基雷达的测角模型;(2)设计地基雷达A和地基雷达B的发射信号;(3)通过设置两种不同初始相位的发射信号,得到在目标处的两种干涉波;(4)通过对两种干涉波信号在地基雷达A的和、差通道分别作取模处理,得到和信号和差信号;(5)利用得到的差和比值查表,得到目标的方位角。本发明通过基于干涉的地基雷达测角方法,能够利用周期性变化的鉴角曲线测得待估计目标精确的方位角信息,显著地提高了地基雷达对于待估计目标的测角精度。
A ground-based radar angle measurement method based on interference field mainly solves the problem of improving the azimuth angle measurement accuracy of the target to be estimated under far-field and narrow-band conditions. The steps that the present invention realizes are as follows: (1) construct the angle measurement model of two ground-based radars; (2) design the transmission signal of ground-based radar A and ground-based radar B; (3) by arranging two kinds of transmission signals of different initial phases, obtain Two kinds of interference waves at the target; (4) by taking modulus processing on the sum and difference channels of the two kinds of interference wave signals in the ground-based radar A respectively, and obtaining the sum signal and the difference signal; (5) using the obtained difference and ratio Check the table to get the aurament of the target. The invention can measure the accurate azimuth angle information of the target to be estimated by using the periodically changing angle discrimination curve through the method of measuring the angle of the ground-based radar based on interference, thereby significantly improving the angle-measuring precision of the target to be estimated by the ground-based radar.
Description
技术领域technical field
本发明属于雷达技术领域,更进一步涉及雷达测角技术领域中的一种基于干涉的雷达测角方法。本发明可用于在窄带条件下对远距离的待估计静止点目标进行方位角的测量。The invention belongs to the technical field of radar, and further relates to a radar angle measurement method based on interference in the technical field of radar angle measurement. The invention can be used to measure the azimuth angle of the long-distance static point target to be estimated under the condition of narrow band.
背景技术Background technique
雷达测角的主要任务是,探测目标所处的空间位置。随着人们对雷达测角领域的不断深入认识,目标角度的跟踪在该领域得到了广泛应用和发展,目前已经存在大量的角度估计算法来实现目标的角度估计。但是,由于雷达系统应用的不断深入,实际跟踪需求对目标角度的探测能力越来越高。从常规的滑窗测角技术到幅度单脉冲测角技术,甚至是相位单脉冲测角技术,虽然滑窗测角技术、幅度单脉冲测角技术和相位单脉冲测角技术对于单脉冲测角的测角精度都有提高,但是对于测角精度提升的程度不高。The main task of radar angle measurement is to detect the spatial position of the target. With the deepening understanding of the field of radar angle measurement, the tracking of target angle has been widely used and developed in this field, and there are already a large number of angle estimation algorithms to realize the angle estimation of the target. However, due to the continuous deepening of the application of radar systems, the actual tracking requirements have higher and higher detection capabilities for target angles. From conventional sliding window angle measurement technology to amplitude single pulse angle measurement technology, even phase single pulse angle measurement technology, although sliding window angle measurement technology, amplitude single pulse angle measurement technology and phase single pulse angle measurement technology The angle measurement accuracy has been improved, but the degree of improvement in angle measurement accuracy is not high.
四川九洲空管科技有限责任公司在其申请的专利文献“一种单脉冲高精度测角系统及其测角方法”(专利申请号201410053339.8,公开号CN103792532A)中公开了一种单脉冲高精度测角方法。该方法实现的具体步骤是,(1)利用同步PN码对基带数字信号进行解调,恢复出原始的有用信号,使噪声、干扰信号被抑制;(2)对恢复出的原始的有用信号进行幅度检测;(3)利用和、差通道的幅度进行相位判断,解算出和、差幅度信息和相位判断结果;(4)根据解算出的和、差幅度信息和相位判断结果获取OBA值函数并进行目标方位计算。该方法存在的不足之处是,在利用同步伪随机码对基带数字信号进行解调,并从噪声和干扰信号中恢复原始信号的过程中,现有技术不能使得有用信号与干扰信号和噪声完全分离,即有用信号中可能混有噪声和干扰信号,导致后续得到的单脉冲测角结果的会出现误差,使得测角的精度不高。Sichuan Jiuzhou Air Traffic Control Technology Co., Ltd. disclosed a single-pulse high-precision angle measurement system and its method in its patent application (patent application number 201410053339.8, publication number CN103792532A). angle measurement method. The concrete steps that this method realizes are, (1) utilize the synchronous PN code to demodulate the baseband digital signal, restore the original useful signal, noise, interference signal are suppressed; Amplitude detection; (3) use the amplitude of the sum and difference channels to perform phase judgment, and calculate the sum and difference amplitude information and phase judgment results; (4) obtain the OBA value function according to the calculated sum and difference amplitude information and phase judgment results and Perform target bearing calculations. The disadvantage of this method is that in the process of using synchronous pseudo-random codes to demodulate the baseband digital signal and restore the original signal from the noise and interference signal, the existing technology cannot make the useful signal and the interference signal and noise completely Separation, that is, useful signals may be mixed with noise and interference signals, resulting in errors in the subsequent single-pulse angle measurement results, making the angle measurement accuracy not high.
西安电子科技大学在其申请的专利文献“机扫米波雷达在多目标情况下的测角方法”(专利申请号CN201410018152.4,公开号CN103744077A)中公开了一种机扫米波雷达在多目标情况下的测角方法。该方法实现的具体步骤是,(1)将天线均分为两个子阵,每个子阵下接一个接收机形成左、右两路通道;(2)由左右两路接收通道分别接收雷达发射的脉冲信号;(3)对接收的回波信号数据进行杂波目标对消处理;(4)将杂波对消后的两路数据相干积累;(5)由积累后的两路数据得到和波束与差波束;(6)利用传统单脉冲方法测出期望目标的偏轴角,并将偏轴角与基准角相加,得到期望目标的准确角度;(7)重复步骤(3)-(6)依次得到所有目标的准确角度。该方法存在的不足之处是,在对两个天线子阵形成的左、右通道接收的回波数据进行杂波目标对消处理时,不能很好对消回波与杂波,由此产生的对消结果会影响相干积累,进而影响测得期望目标偏轴角的精确性,最终得到的角度测量结果的精度仍显不足。Xidian University disclosed a kind of machine-scanned meter-wave radar in the patent document "Angle measurement method of machine-scanned meter-wave radar in the case of multiple targets" (patent application number CN201410018152.4, publication number CN103744077A). Angle measurement method in the target case. The concrete steps that this method realizes are: (1) the antenna is divided into two sub-arrays, and each sub-array is connected with a receiver to form left and right two-way channels; pulse signal; (3) perform clutter target cancellation processing on the received echo signal data; (4) coherently accumulate the two-way data after clutter cancellation; (5) obtain the sum beam from the accumulated two-way data and the difference beam; (6) Use the traditional monopulse method to measure the off-axis angle of the desired target, and add the off-axis angle to the reference angle to obtain the exact angle of the desired target; (7) Repeat steps (3)-(6 ) to obtain the accurate angles of all targets in turn. The disadvantage of this method is that when the clutter target cancellation processing is performed on the echo data received by the left and right channels formed by the two antenna sub-arrays, the echo and clutter cannot be canceled well, resulting in The cancellation results will affect the coherent accumulation, and then affect the accuracy of the measured off-axis angle of the desired target, and the accuracy of the final angle measurement results is still insufficient.
发明内容SUMMARY OF THE INVENTION
本发明的目的是针对上述现有技术的不足,提出一种基于干涉场的地基雷达测角方法,以实现对待估计静止点目标的方位角进行高精度测量。The object of the present invention is to address the deficiencies of the above-mentioned prior art, and propose a ground-based radar angle measurement method based on interference field, so as to realize high-precision measurement of the azimuth angle of the static point target to be estimated.
实现本发明目的的思路是,构建两部地基雷达的测角模型;设计地基雷达A和地基雷达B的发射信号,使两部地基雷达发射的单载频信号同时到达待估计静止点目标;改变两部地基雷达发射信号的初始相位,在等距离环处生成两种干涉场信号;两种干涉场信号被地基雷达A接收,对两种回波信号在地基雷达A的和通道和差通道内进行处理,生成和信号和差信号;利用差和比值查表,得到待估计静止点目标的方位角。The train of thought of realizing the object of the present invention is to construct the angle-measuring models of two ground-based radars; design the transmission signals of ground-based radar A and ground-based radar B, so that the single carrier frequency signals emitted by the two ground-based radars arrive at the stationary point target to be estimated simultaneously; change The initial phase of the transmitted signals of the two ground-based radars generates two kinds of interference field signals at the equidistant ring; the two kinds of interference field signals are received by the ground-based radar A, and the two echo signals are in the sum channel and difference channel of the ground-based radar A Perform processing to generate a sum signal and a difference signal; use the difference and ratio look-up table to obtain the azimuth angle of the static point target to be estimated.
本发明的具体步骤如下:Concrete steps of the present invention are as follows:
(1)构建两部地基雷达的测角模型:(1) Construct the angle measurement model of two ground-based radars:
(1a)以地基雷达A为坐标原点,地基雷达A的正东方向为X轴,地基雷达A的正北方向为Y轴,建立直角坐标系;(1a) With the ground-based radar A as the coordinate origin, the due east direction of the ground-based radar A is the X-axis, and the due north direction of the ground-based radar A is the Y-axis, and a rectangular coordinate system is established;
(1b)在X轴上与地基雷达A间距为L的位置设置地基雷达B,得到两部地基雷达的测角模型,60m≤L≤100m;(1b) Set the ground-based radar B at the distance L from the ground-based radar A on the X axis, and obtain the angle measurement models of the two ground-based radars, 60m≤L≤100m;
(2)地基雷达A和地基雷达B发射单载频信号:(2) Ground-based radar A and ground-based radar B transmit single carrier frequency signals:
(2a)利用余弦公式,计算地基雷达A和地基雷达B与待估计静止点目标的距离差;(2a) Using the cosine formula, calculate the distance difference between ground-based radar A and ground-based radar B and the stationary point target to be estimated;
(2b)用距离差除以真空中电磁波的传播速度,得到两部地基雷达发射信号的时延Δτ;(2b) Divide the distance difference by the propagation speed of electromagnetic waves in vacuum to obtain the time delay Δτ of the transmitted signals of the two ground-based radars;
(2c)地基雷达A发射单载频信号,在地基雷达A的发射时间时延Δτ之后,地基雷达B发射相同频率的单载频信号;(2c) Ground-based radar A transmits a single-carrier frequency signal, and ground-based radar B transmits a single-carrier frequency signal of the same frequency after the transmission time delay Δτ of ground-based radar A;
(3)生成两种干涉场信号:(3) Generate two kinds of interference field signals:
(3a)将地基雷达A和地基雷达B的初始相位均设置为0,将两个地基雷达发射的电磁波在等距离环内干涉,得到第一种干涉场信号;(3a) The initial phases of ground-based radar A and ground-based radar B are both set to 0, and the electromagnetic waves emitted by the two ground-based radars are interfered in an equidistant ring to obtain the first type of interference field signal;
(3b)将地基雷达A的初始相位设置为0,地基雷达B的初始相位设置为π,将两个地基雷达发射的电磁波在等距离环内干涉,得到第二种干涉场信号;(3b) Set the initial phase of ground-based radar A to 0, and the initial phase of ground-based radar B to π, and interfere the electromagnetic waves emitted by the two ground-based radars in an equidistant ring to obtain the second interference field signal;
(4)生成和信号和差信号:(4) Generate sum signal and difference signal:
(4a)地基雷达A接收两种干涉场信号的回波,得到两种回波信号;(4a) The ground-based radar A receives the echoes of two kinds of interference field signals, and obtains two kinds of echo signals;
(4b)将第一种回波信号与第二种回波信号在地基雷达A的和通道内取模相加,得到和信号;(4b) The first echo signal and the second echo signal are modulo-added in the sum channel of the ground-based radar A to obtain the sum signal;
(4c)将第一种回波信号与第二种回波信号在地基雷达A的差通道内取模相减,得到差信号;(4c) taking the modulo subtraction of the first echo signal and the second echo signal in the difference channel of the ground-based radar A to obtain the difference signal;
(5)获取待估计静止点目标的方位角:(5) Obtain the azimuth angle of the static point target to be estimated:
(5a)将差信号除以和信号,得到差和比值;(5a) dividing the difference signal by the sum signal to obtain the difference and ratio;
(5b)从鉴角曲线表中查找该差和比值对应的待估计静止点目标相对于地基雷达A的方位角。(5b) Look up the azimuth angle of the static point target to be estimated relative to the ground-based radar A corresponding to the difference and the ratio from the angle discrimination curve table.
本发明与现有的技术相比具有以下优点:Compared with the prior art, the present invention has the following advantages:
第一,由于本发明利用两部地基雷达发射电磁波的叠加得到两种干涉波,利用周期变化的干涉波来精确的表征待估计静止点目标的方位角信息,克服了现有技术中地基雷达回波信号波形变化单一导致的对待估计静止点目标的空间方位角信息描述不精确的问题,使得本发明能够更加精确的估计静止点目标的方位角。First, because the present invention uses the superposition of electromagnetic waves emitted by two ground-based radars to obtain two kinds of interference waves, and uses periodically changing interference waves to accurately characterize the azimuth information of the static point target to be estimated, which overcomes the ground-based radar echo in the prior art The problem of inaccurate description of the space azimuth angle information of the static point target to be estimated caused by the single wave signal waveform change enables the present invention to estimate the azimuth angle of the static point target more accurately.
第二,由于本发明对两种回波信号在地基雷达A的和差通道进行了取模操作,先将两种回波信号在地基雷达A的和通道内取模相加得到和信号,再将两种回波信号在地基雷达A的差通道内取模相减得到差信号,克服了现有技术当待估计静止点目标处于噪声和干扰的复杂环境时,回波与杂波对消不彻底,导致得不到正确的和信号和差信号的问题,使得本发明能够准确的得到待估计静止点目标的和信号和差信号,增强了静止点目标方位角估计的准确性和可靠性。The second, because the present invention has carried out modulo-taking operation to two kinds of echo signals in the sum difference channel of ground-based radar A, first two kinds of echo signals are taken modulo-adding in the sum channel of ground-based radar A to obtain the sum signal, and then The two echo signals are modulo-subtracted in the difference channel of the ground-based radar A to obtain the difference signal, which overcomes the inability of echo and clutter cancellation in the prior art when the static point target to be estimated is in a complex environment of noise and interference. Thoroughly, it leads to the problem that the correct sum signal and difference signal cannot be obtained, so that the present invention can accurately obtain the sum signal and difference signal of the static point target to be estimated, and enhance the accuracy and reliability of the static point target azimuth estimation.
附图说明Description of drawings
图1为本发明的流程图;Fig. 1 is a flowchart of the present invention;
图2为本发明建立的地基雷达测角模型示意图;Fig. 2 is the schematic diagram of the ground-based radar angle measurement model established by the present invention;
图3为传统单脉冲测角方法得到的鉴角曲线;Fig. 3 is the angle discrimination curve that traditional monopulse angle measurement method obtains;
图4为本发明的仿真结果图。Fig. 4 is a simulation result diagram of the present invention.
具体实施方式Detailed ways
下面结合附图对本发明做进一步的描述。The present invention will be further described below in conjunction with the accompanying drawings.
结合附图1中,对本发明的具体步骤进一步的描述。In conjunction with accompanying drawing 1, the specific steps of the present invention are further described.
步骤1,构建两部地基雷达的测角模型。Step 1. Construct angle measurement models of two ground-based radars.
以地基雷达A为坐标原点,地基雷达A的正东方向为X轴,地基雷达A的正北方向为Y轴,建立直角坐标系。With the ground-based radar A as the coordinate origin, the due east direction of the ground-based radar A is the X-axis, and the due north direction of the ground-based radar A is the Y-axis, and a rectangular coordinate system is established.
在X轴上与地基雷达A间距为L的位置设置地基雷达B,得到两部地基雷达的测角模型,如图2所示,A和B表示两部地基雷达在X轴上的位置,L表示地基雷达A与地基雷达B间的基线长度,θ表示所观测方位维的角度范围,θ0表示待估计静止点目标相对于地基雷达A的方位角,R0表示待估计静止点目标与地基雷达A的距离,P0表示待估计静止点目标所在的位置,P1表示地基雷达A发射信号的3dB波束宽度相对于中心的最大偏角所对应的位置,两个灰色扇形区域为两部地基雷达发射信号3dB波束的覆盖范围,透明环表示待估计静止点目标所在的等距离环,60m≤L≤100m。Set ground-based radar B at a distance L from ground-based radar A on the X-axis, and obtain the angle measurement models of the two ground-based radars, as shown in Figure 2, A and B represent the positions of the two ground-based radars on the X-axis, L Indicates the baseline length between ground-based radar A and ground-based radar B, θ indicates the angle range of the observed azimuth dimension, θ 0 indicates the azimuth angle of the stationary point target to be estimated relative to ground-based radar A, and R 0 indicates the distance between the stationary point target to be estimated and the ground-based radar. The distance of radar A, P 0 represents the position of the static point target to be estimated, P 1 represents the position corresponding to the maximum deflection angle of the 3dB beam width of the signal transmitted by ground-based radar A relative to the center, and the two gray fan-shaped areas are two ground-based The coverage of the 3dB beam of the radar transmission signal, the transparent ring indicates the equidistant ring where the static point target to be estimated is located, 60m≤L≤100m.
其中,地基雷达A既发射又接收单载频信号,地基雷达B只发射单载频信号。Among them, ground-based radar A both transmits and receives single-carrier frequency signals, and ground-based radar B only transmits single-carrier frequency signals.
步骤2,地基雷达A和地基雷达B发射单载频信号。Step 2, ground-based radar A and ground-based radar B transmit single carrier frequency signals.
利用余弦公式,计算地基雷达A和地基雷达B与待估计静止点目标的距离差。Using the cosine formula, calculate the distance difference between ground-based radar A and ground-based radar B and the static point target to be estimated.
所述的余弦公式如下:The described cosine formula is as follows:
其中,ΔR表示地基雷达A与待估计静止点目标的距离以及地基雷达B与待估计静止点目标的距离之差,R0表示地基雷达A与待估计静止点目标的距离,表示求平方根操作,L表示地基雷达A与地基雷达B之间的距离,cos表示余弦函数,θ0表示待估计静止点目标相对于地基雷达A的方位角,c表示真空中电磁波的传播速度。Among them, ΔR represents the difference between the distance between ground-based radar A and the static point target to be estimated and the distance between ground-based radar B and the static point target to be estimated, R0 represents the distance between ground-based radar A and the static point target to be estimated, represents the square root operation, L represents the distance between ground-based radar A and ground-based radar B, cos represents the cosine function, θ 0 represents the azimuth angle of the static point target to be estimated relative to ground-based radar A, and c represents the propagation velocity of electromagnetic waves in vacuum.
用距离差除以真空中电磁波的传播速度,得到两部地基雷达发射信号的时延Δτ。Divide the distance difference by the propagation speed of electromagnetic waves in vacuum to obtain the time delay Δτ of the two ground-based radars' transmitted signals.
为了使两部地基雷达发射的单载频信号能够在静止点目标所在的等距离环处形成稳定的干涉效应,需使得两部地基雷达发射的单载频信号能够同时到达待估计静止点目标所在的等距离区域。地基雷达A发射单载频信号,在地基雷达A的发射时间时延Δτ之后,地基雷达B发射相同频率的单载频信号。In order to make the single-carrier frequency signals transmitted by the two ground-based radars form a stable interference effect at the equidistant ring where the stationary point target is located, it is necessary to make the single-carrier frequency signals transmitted by the two ground-based radars reach the location of the static point target to be estimated at the same time equidistant area. Ground-based radar A transmits a single carrier frequency signal, and ground-based radar B transmits a single carrier frequency signal of the same frequency after ground-based radar A transmits a time delay Δτ.
地基雷达A发射的信号为:The signal transmitted by ground-based radar A is:
地基雷达B发射的信号为:The signal transmitted by the ground-based radar B is:
其中,Tp表示脉冲重复周期,fc表示发射信号的载频,φ1、φ2分别表示地基雷达A和地基雷达B发射信号的初始相位。Among them, T p represents the pulse repetition period, f c represents the carrier frequency of the transmitted signal, φ 1 and φ 2 represent the initial phases of the transmitted signals of ground-based radar A and ground-based radar B, respectively.
步骤3,生成两种干涉场信号。Step 3, generating two kinds of interference field signals.
将地基雷达A和地基雷达B的初始相位均设置为0,将两个地基雷达发射的电磁波在等距离环内干涉,得到第一种干涉场信号。The initial phases of ground-based radar A and ground-based radar B are both set to 0, and the electromagnetic waves emitted by the two ground-based radars are interfered in an equidistant ring to obtain the first interference field signal.
将地基雷达A的初始相位设置为0,地基雷达B的初始相位设置为π,将两个地基雷达发射的电磁波在等距离环内干涉,得到第二种干涉场信号。The initial phase of ground-based radar A is set to 0, the initial phase of ground-based radar B is set to π, and the electromagnetic waves emitted by the two ground-based radars are interfered in an equidistant ring to obtain the second interference field signal.
两部地基雷达的发射信号到达等距离环上任一点的时延差为:The time delay difference between the transmitted signals of two ground-based radars arriving at any point on the equidistant ring is:
其中,Δτ(θ)表示等距离环上任一点处两部地基雷达发射信号的时延,Δτ(θ0)表示待估计静止点目标处两部地基雷达发射信号的时延。Among them, Δτ(θ) represents the time delay of the two ground-based radars transmitting signals at any point on the equidistant ring, and Δτ(θ 0 ) represents the time delay of the two ground-based radars transmitting signals at the static point target to be estimated.
在目标区域(θ-θ0)≤θ3dB内,两部地基雷达发射信号的到达时间差的最大值为:In the target area (θ-θ 0 )≤θ 3dB , the maximum value of the arrival time difference of the transmitted signals of the two ground-based radars is:
由于窄带条件下雷达天线3dB波束宽度通常较小,可以近似认为地基雷达A和地基雷达B的发射信号可以同时到达等距离环上的任意一点,所以地基雷达A和地基雷达B的发射信号可以在待估计静止点目标区域内形成稳定的干涉效应。Since the 3dB beamwidth of the radar antenna is usually small under narrow-band conditions, it can be approximated that the transmission signals of ground-based radar A and ground-based radar B can reach any point on the equidistant ring at the same time, so the transmission signals of ground-based radar A and ground-based radar B can be at A stable interference effect is formed in the target area of the stationary point to be estimated.
等距离环内的干涉场信号可以表示为:The interference field signal in the equidistant ring can be expressed as:
将地基雷达A的初始相位设置为0,地基雷达B的初始相位设置为π,得到的第一种干涉波可以表示为:Set the initial phase of ground-based radar A to 0, and the initial phase of ground-based radar B to π, the obtained first interference wave can be expressed as:
将地基雷达A的初始相位设置为0,地基雷达B的初始相位设置为π,得到的第一种干涉波可以表示为:Set the initial phase of ground-based radar A to 0, and the initial phase of ground-based radar B to π, the obtained first interference wave can be expressed as:
步骤4,生成和信号和差信号。Step 4, generating a sum signal and a difference signal.
地基雷达A接收两种干涉场信号的回波,得到两种回波信号。The ground-based radar A receives the echoes of two kinds of interference field signals and obtains two kinds of echo signals.
将第一种回波信号与第二种回波信号在地基雷达A的和通道内取模相加,得到和信号。The first type of echo signal and the second type of echo signal are modulo-added in the sum channel of the ground-based radar A to obtain the sum signal.
将第一种回波信号与第二种回波信号在地基雷达A的差通道内取模相减,得到差信号。The first type of echo signal and the second type of echo signal are modulo subtracted in the difference channel of the ground-based radar A to obtain the difference signal.
地基雷达A接收到的第一种回波信号可以表示为:The first echo signal received by ground-based radar A can be expressed as:
地基雷达A接收到的第二种回波信号可以表示为:The second echo signal received by ground-based radar A can be expressed as:
地基雷达A内合通道的和信号可以表示为:The sum signal of the integrated channel of ground-based radar A can be expressed as:
地基雷达A内合通道的和信号可以表示为:The sum signal of the integrated channel of ground-based radar A can be expressed as:
步骤5,获取待估计静止点目标的方位角。Step 5, obtain the azimuth angle of the static point target to be estimated.
按照下式,将待估计目标处的差信号除以和信号,得到差和比值:According to the following formula, the difference signal at the target to be estimated is divided by the sum signal to obtain the difference sum ratio:
其中,表示待估计目标的差和比值。in, Indicates the difference and ratio of the target to be estimated.
将等距离环内的差信号除以和信号,得到如下的随方位角变化的差和比函数:Divide the difference signal in the equidistant ring by the sum signal to obtain the following difference and ratio function as a function of azimuth:
以等距离环相对于地基雷达A的角度范围为横坐标,以差和比为纵坐标,由该角度范围对应的差和比值绘制出该角度范围的鉴角曲线表,如图3所示。Taking the angle range of the equidistant ring relative to the ground-based radar A as the abscissa, and the difference and ratio as the ordinate, the angle discrimination curve table of the angle range is drawn from the difference and ratio corresponding to the angle range, as shown in Figure 3.
从图3鉴角曲线表中查找差和比值对应的待估计静止点目标相对于地基雷达A的方位角。Find the azimuth angle of the static point target to be estimated relative to the ground-based radar A corresponding to the difference and the ratio from the angle discrimination curve table in Fig. 3 .
下面结合仿真实验对本发明的效果做进一步说明。The effects of the present invention will be further described below in combination with simulation experiments.
1.仿真实验条件:1. Simulation experimental conditions:
本发明仿真实验的硬件测试平台是:处理器为CPU intel Core i5-6500,主频为3.2GHz,内存4GB;软件平台为:Windows 7旗舰版,64位操作系统,MATLAB R2012b。The hardware test platform of the simulation experiment of the present invention is: processor is CPU intel Core i5-6500, main frequency is 3.2GHz, internal memory 4GB; Software platform is: Windows 7 ultimate edition, 64 operating systems, MATLAB R2012b.
2.仿真内容仿真结果分析:2. Simulation content Simulation result analysis:
本发明仿真实验有两个,第一个仿真是使用现有技术的单脉冲测角方法,对待估计静止点目标的方位角测量进行仿真,第二个仿真是使用本发明所述的角度测量方法,对待估计静止点目标的方位角测量进行仿真。There are two simulation experiments of the present invention, the first simulation is to use the monopulse angle measurement method of the prior art to simulate the azimuth measurement of the static point target to be estimated, and the second simulation is to use the angle measurement method of the present invention , to simulate the azimuth measurement of the stationary point target to be estimated.
仿真1,使用现有单脉冲测角技术对待估计静止点目标的方位角测量进行仿真,得到如图3所示的鉴角曲线,鉴角曲线是以待估计静止点目标相对于地基雷达的角度范围为横坐标,横坐标的单位是弧度,以差和比为纵坐标,纵坐标的单位是1。分析仿真结果可知,在以待估计静止点目标相对于地基雷达的角度范围内,现有技术得到的鉴角曲线只单调的变化一次,测角的精度不高。Simulation 1, use the existing monopulse angle measurement technology to simulate the azimuth measurement of the stationary point target to be estimated, and obtain the angle detection curve shown in Figure 3. The angle detection curve is the angle of the stationary point target to be estimated relative to the ground-based radar The range is the abscissa, and the unit of the abscissa is radian, and the difference and ratio are the ordinate, and the unit of the ordinate is 1. Analysis of the simulation results shows that within the angle range of the stationary point target to be estimated relative to the ground-based radar, the angle detection curve obtained by the prior art only changes monotonously once, and the angle measurement accuracy is not high.
仿真2,使用本发明所述的角度测量方法,对待估计静止点目标的方位角测量进行仿真,本发明的仿真实验中使用的仿真参数如表1所示:Simulation 2, using the angle measurement method of the present invention, simulates the azimuth measurement of the stationary point target to be estimated, and the simulation parameters used in the simulation experiment of the present invention are as shown in table 1:
表1仿真参数一览表Table 1 list of simulation parameters
使用本发明方法仿真得到如图4所示的鉴角曲线,鉴角曲线是以等距离环相对于地基雷达A的角度范围为横坐标,横坐标的单位是角度,以差和比为纵坐标。Use the simulation method of the present invention to obtain the angle detection curve as shown in Figure 4, the angle detection curve is based on the angle range of the equidistant ring relative to the ground-based radar A as the abscissa, the unit of the abscissa is the angle, and the difference and ratio is the ordinate .
对比图3和图4分析仿真结果可知,本发明仿真的鉴角曲线是周期性变化的,变化的周期受到发射信号载频和双基地雷达间基线长度的制约。通过改变地基雷达发射信号的载频和地基雷达间的基线长度,可以改变变化周期的大小,进而改变方位角的测量精度。所以,本发明所用的基于干涉的地基雷达测角技术的精度,远远高于现有单脉冲测角方法的测角精度。Comparing the simulation results of Fig. 3 and Fig. 4, it can be seen that the angle detection curve of the simulation of the present invention changes periodically, and the period of change is restricted by the carrier frequency of the transmitted signal and the baseline length between the bistatic radars. By changing the carrier frequency of the signal transmitted by the ground-based radar and the baseline length between the ground-based radar, the size of the change period can be changed, thereby changing the measurement accuracy of the azimuth angle. Therefore, the accuracy of the interference-based ground-based radar angle measurement technology used in the present invention is far higher than the angle measurement accuracy of the existing single-pulse angle measurement method.
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111220954A (en) * | 2019-12-05 | 2020-06-02 | 上海无线电设备研究所 | Radar angle error correction method based on self-correcting amplitude normalization |
CN113406615A (en) * | 2021-05-25 | 2021-09-17 | 森思泰克河北科技有限公司 | Target tracking method and device of binary phase modulation array radar |
WO2022104666A1 (en) * | 2020-11-19 | 2022-05-27 | 深圳市大疆创新科技有限公司 | Radar system, movable platform, control method, obstacle avoidance method, and storage medium |
CN119335520A (en) * | 2024-12-20 | 2025-01-21 | 中国电子科技集团公司第五十四研究所 | A radar interferometry angle measurement method based on coherent MIMO signal processing |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH11202046A (en) * | 1998-01-20 | 1999-07-30 | Toshiba Corp | Radar angle measurement method and device |
CN104914415A (en) * | 2015-05-21 | 2015-09-16 | 中国人民解放军63892部队 | Single-pulse radar coherent jamming method based on target range profile template matching |
CN105974389A (en) * | 2016-06-30 | 2016-09-28 | 西安电子科技大学 | Mechanic scan meter-wave radar monopulse angle measuring method based on iterative processing |
-
2018
- 2018-12-28 CN CN201811617549.XA patent/CN109521418B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH11202046A (en) * | 1998-01-20 | 1999-07-30 | Toshiba Corp | Radar angle measurement method and device |
CN104914415A (en) * | 2015-05-21 | 2015-09-16 | 中国人民解放军63892部队 | Single-pulse radar coherent jamming method based on target range profile template matching |
CN105974389A (en) * | 2016-06-30 | 2016-09-28 | 西安电子科技大学 | Mechanic scan meter-wave radar monopulse angle measuring method based on iterative processing |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111220954A (en) * | 2019-12-05 | 2020-06-02 | 上海无线电设备研究所 | Radar angle error correction method based on self-correcting amplitude normalization |
CN111220954B (en) * | 2019-12-05 | 2022-07-22 | 上海无线电设备研究所 | Radar angle error correction method based on self-correcting amplitude normalization |
WO2022104666A1 (en) * | 2020-11-19 | 2022-05-27 | 深圳市大疆创新科技有限公司 | Radar system, movable platform, control method, obstacle avoidance method, and storage medium |
CN113406615A (en) * | 2021-05-25 | 2021-09-17 | 森思泰克河北科技有限公司 | Target tracking method and device of binary phase modulation array radar |
CN119335520A (en) * | 2024-12-20 | 2025-01-21 | 中国电子科技集团公司第五十四研究所 | A radar interferometry angle measurement method based on coherent MIMO signal processing |
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