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CN111220942B - Near-field calibration method for amplitude-phase consistency of receiving transducer array - Google Patents

Near-field calibration method for amplitude-phase consistency of receiving transducer array Download PDF

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CN111220942B
CN111220942B CN201911257833.5A CN201911257833A CN111220942B CN 111220942 B CN111220942 B CN 111220942B CN 201911257833 A CN201911257833 A CN 201911257833A CN 111220942 B CN111220942 B CN 111220942B
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CN111220942A (en
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周天
袁伟家
朱建军
魏波
李海森
刘伟陆
杜伟东
陈宝伟
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Harbin Engineering University
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    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S3/00Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
    • G01S3/80Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using ultrasonic, sonic or infrasonic waves
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Abstract

The invention provides a near-field calibration method for amplitude-phase consistency of a receiving transducer array. Firstly, incident signals collected in different directions by a receiving array on a rotary table are subjected to focused beam forming processing to obtain a series of direction-of-arrival estimates; then, establishing a covariance matrix of the received signals in a frequency domain, and establishing an amplitude-phase consistency error estimation model; selecting small-angle incident angle signals, respectively assuming the neighborhood angles as ideal incident angles, and estimating error estimation results corresponding to angles in the neighborhood according to an amplitude-phase consistency error estimation model; and finally, compensating the array according to the error result, selecting data of two known angle intervals according to preset parameters of a test, evaluating the estimated deviation of the angle intervals, determining the amplitude-phase consistency error according to the minimum value of the deviation, and finishing calibration. The invention can improve the amplitude-phase consistency and direction-finding performance of the array without an auxiliary information source.

Description

一种接收换能器阵列幅相一致性近场校准方法A Near Field Calibration Method for Amplitude and Phase Consistency of Receive Transducer Array

技术领域technical field

本发明涉及的是一种阵列天线的校准和测量方法,具体地说是一种接收换能器阵列幅相一致性近场校准方法。The invention relates to a method for calibrating and measuring an array antenna, in particular to a near-field calibration method for receiving transducer array amplitude and phase consistency.

背景技术Background technique

信号波达方向估计中需要采用波束形成方法对来波方位进行扫描,而一些波束形成算法的测向性能极大依赖于阵元间的幅度相位信息,接收换能器阵列由于长时间使用,阵元加工工艺差异,以及环境变化等会不可避免引发水声换能器阵元间幅度相位的不一致性问题,进一步导致测向精度下降、波束图旁瓣级升高。In signal direction of arrival estimation, it is necessary to use the beamforming method to scan the incoming wave azimuth, and the direction finding performance of some beamforming algorithms greatly depends on the amplitude and phase information between the array elements. Due to the long-term use of the receiving transducer array, the array The difference in element processing technology and environmental changes will inevitably lead to the inconsistency of the amplitude and phase between the array elements of the underwater acoustic transducer, which will further lead to the decrease of the direction finding accuracy and the increase of the side lobe level of the beam pattern.

现有的接收换能器阵列幅相一致性校准方法通常需要借助辅助信源获得方位信息,并且大多采用平面波假设模型。然而借助辅助信源的被动校准方法更易引入误差,并且平面波的假设模型仅适用于远场,一旦被校准对象孔径较大且阵元数较多,若继续采用平面波模型,则校准方法对校准场地尺寸有着较高的要求,而这通常是难以满足的。此外,由于一个周期内时域信号的采样点数目较多,在涉及协方差矩阵运算时,现有校准方法多在时域进行,运算量较大。The existing calibration methods for the amplitude-phase consistency of receiving transducer arrays usually need to obtain azimuth information with the help of auxiliary sources, and most of them use a plane wave assumption model. However, the passive calibration method with the help of auxiliary sources is more likely to introduce errors, and the hypothetical model of the plane wave is only applicable to the far field. Dimensions have high requirements, which are often difficult to meet. In addition, due to the large number of sampling points of the time-domain signal in one period, when it comes to covariance matrix calculations, the existing calibration methods are mostly performed in the time domain, and the amount of calculation is relatively large.

近场聚焦波束形成基于球面波假设能够对声源位置聚焦,相对于平面波假设模型,它可以保证距离发射声源较近时依然具有精确的测向结果,为测量条件提供了便利。尤其是在对孔径较大且阵元数较多的换能器阵列进行校准时,相比于传统校准方法具有天然的优势。Near-field focused beamforming is based on the spherical wave assumption and can focus on the position of the sound source. Compared with the plane wave assumption model, it can ensure accurate direction finding results when the distance from the emitting sound source is relatively close, which provides convenience for measurement conditions. Especially when calibrating a transducer array with a large aperture and a large number of elements, it has natural advantages over traditional calibration methods.

发明内容Contents of the invention

本发明的目的在于提供一种在校准场地尺寸有限且无辅助信源的情况下能够提高接收换能器阵列幅相一致性的接收换能器阵列幅相一致性近场校准方法。The purpose of the present invention is to provide a near-field calibration method for the amplitude-phase consistency of the receiving transducer array that can improve the amplitude-phase consistency of the receiving transducer array under the condition of limited calibration site size and no auxiliary signal source.

本发明的目的是这样实现的:The purpose of the present invention is achieved like this:

(1)建立近场聚焦波束形成模型,处于回转台上的接收阵在不同方向采集的入射信号经过聚焦波束形成处理得到一系列的波达方向估计;(1) Establish a near-field focused beamforming model. The incident signals collected by the receiving array on the rotary platform in different directions are processed by focused beamforming to obtain a series of direction-of-arrival estimates;

(2)在频域建立接收信号协方差矩阵,并建立幅相一致性误差估计模型;(2) Establish the received signal covariance matrix in the frequency domain, and establish the amplitude-phase consistency error estimation model;

(3)选取小角度入射角信号,将其邻域角度分别设为理想入射角,根据幅相一致性误差估计模型估计对应邻域内角度的幅相误差;(3) Select the small-angle incident angle signal, set its neighborhood angles as ideal incident angles, and estimate the amplitude-phase error corresponding to the angle in the neighborhood according to the amplitude-phase consistency error estimation model;

(4)根据误差结果补偿阵列,根据预设参数选择两已知角度间隔的数据,评估对于角度间隔估计的偏差,根据偏差极小值确定幅相一致性误差,完成校准。(4) Compensate the array according to the error result, select the data of two known angular intervals according to the preset parameters, evaluate the deviation of the estimated angular interval, determine the amplitude and phase consistency error according to the minimum value of the deviation, and complete the calibration.

本发明还可以包括:The present invention may also include:

1.所述的近场聚焦模型为:1. The near-field focusing model described is:

Figure BDA0002310787940000021
Figure BDA0002310787940000021

其中,V(θ)为对应于入射方向θ的波束输出,M为待估计阵列的阵元数,xm为第m个阵元接收到的信号,

Figure BDA00023107879400000211
为在第n个采样时刻下,接收信号在阵元m与参考阵元之间的相位差。Among them, V(θ) is the beam output corresponding to the incident direction θ, M is the number of array elements to be estimated, x m is the signal received by the mth array element,
Figure BDA00023107879400000211
is the phase difference of the received signal between element m and the reference element at the nth sampling moment.

2.步骤(2)具体包括:2. Step (2) specifically includes:

建立幅相一致性误差估计模型,Γ和Φ分别作为阵列的幅度相位向量有:Establish the magnitude-phase consistency error estimation model, Γ and Φ are respectively used as the magnitude and phase vectors of the array:

Γ=diag[ρ12,…,ρM]Γ=diag[ρ 12 ,…,ρ M ]

Figure BDA0002310787940000022
Figure BDA0002310787940000022

其中ρm

Figure BDA0002310787940000023
分别为第m个阵元的幅度和相位向量,并且ρ1=1,
Figure BDA0002310787940000024
where ρ m and
Figure BDA0002310787940000023
are the magnitude and phase vectors of the mth array element respectively, and ρ 1 =1,
Figure BDA0002310787940000024

则理想接收信号以及存在误差的接收信号表示为:Then the ideal received signal and the received signal with errors are expressed as:

X0(t)=AS(t)+N(t)X 0 (t)=AS(t)+N(t)

X(t)=ΓΦ(AS(t)+N(t))X(t)=ΓΦ(AS(t)+N(t))

Figure BDA0002310787940000025
Figure BDA0002310787940000025

S(t)=[s1(t),s2(t),…,sM(t)]T(s1(t)=s2(t),…,=sM(t))S(t)=[s 1 (t),s 2 (t),…,s M (t)] T (s 1 (t)=s 2 (t),…,=s M (t))

N(t)=[n1(t),n2(t),…,nM(t)]T N(t)=[n 1 (t),n 2 (t),...,n M (t)] T

其中,X0(t)和X(t)为以理想接收信号和实际接收信号矩阵;S(t)为信源发射信号组成的发射信号矩阵,N(t)为各阵元接收的噪声组成的噪声矩阵,其中噪声设为高斯白噪声;Among them, X 0 (t) and X(t) are the ideal received signal and the actual received signal matrix; S(t) is the transmitted signal matrix composed of the source transmitted signal, and N(t) is the noise composition received by each array element The noise matrix of , where the noise is set to Gaussian white noise;

将各阵元接收的理想信号X0(t)和实际信号X(t)经过傅里叶变换至频域得到X0 fre(f)和Xfre(f),分别提取距离零频最近频谱峰值X0 P和XPThe ideal signal X 0 (t) and the actual signal X(t) received by each array element are transformed into the frequency domain by Fourier transform to obtain X 0 fre (f) and X fre (f), and the spectrum peaks closest to zero frequency are extracted respectively X 0 P and X P :

Figure BDA0002310787940000026
Figure BDA0002310787940000026

Xfre(f)=[x1(f),x2(f),…,xM(f)]T X fre (f)=[x 1 (f), x 2 (f),…, x M (f)] T

Figure BDA0002310787940000027
Figure BDA0002310787940000027

XP=[P1,P2,…,PM]T X P =[P 1 ,P 2 ,…,P M ] T

并构建理想协方差矩阵和实际协方差矩阵

Figure BDA0002310787940000028
和RX:And construct the ideal covariance matrix and the actual covariance matrix
Figure BDA0002310787940000028
and R x :

Figure BDA0002310787940000029
Figure BDA0002310787940000029

Figure BDA00023107879400000210
Figure BDA00023107879400000210

幅相一致性误差矩阵Ω和各阵元幅相一致性误差ρ和

Figure BDA0002310787940000031
为:The amplitude-phase consistency error matrix Ω and the amplitude-phase consistency error ρ of each array element and
Figure BDA0002310787940000031
for:

Figure BDA0002310787940000032
Figure BDA0002310787940000032

Figure BDA0002310787940000033
Figure BDA0002310787940000033

Figure BDA0002310787940000034
Figure BDA0002310787940000034

3.步骤(3)中,选择小角度的入射角为θ0的接收信号,在角度范围为ε的邻域中对邻域内K个角度遍历,使得理想角度θs满足θs(k)∈(θ0-ε,θ0+ε),计算对应邻域内各个角度的幅相一致性误差Ω(k)。3. In step (3), select the received signal with a small incident angle of θ 0 , and traverse K angles in the neighborhood in the neighborhood with an angle range of ε, so that the ideal angle θ s satisfies θ s (k)∈ (θ 0 -ε,θ 0 +ε), calculate the amplitude-phase consistency error Ω(k) of each angle in the corresponding neighborhood.

4.步骤(4)具体为:4. Step (4) is specifically:

对k组各通道幅度误差ρm(k)和相位误差

Figure BDA0002310787940000035
分别补偿阵列,选择两入射角间隔为Δθ的接收信号,其中参数Δθ0根据回转台获得,分别估计这两组信号的波达方向并计算其角度间隔Δθ(k),考察对角度间隔估计的偏差e(k)=|Δθ0-Δθ(k)|,若在角度邻域(θ0-ε,θ0+ε)内存在唯一极小值,则
Figure BDA0002310787940000036
理想角度为
Figure BDA0002310787940000037
换能器阵列各阵元的幅相误差为
Figure BDA0002310787940000038
Figure BDA0002310787940000039
For each channel amplitude error ρ m (k) and phase error of group k
Figure BDA0002310787940000035
Compensate the array separately, select two received signals whose incident angle interval is Δθ, and the parameter Δθ 0 is obtained according to the turntable, estimate the direction of arrival of these two groups of signals and calculate their angular interval Δθ(k), and investigate the estimation of the angular interval Deviation e(k)=|Δθ 0 -Δθ(k)|, if there is a unique minimum value in the angle neighborhood (θ 0 -ε,θ 0 +ε), then
Figure BDA0002310787940000036
The ideal angle is
Figure BDA0002310787940000037
The amplitude and phase errors of each element of the transducer array are
Figure BDA0002310787940000038
and
Figure BDA0002310787940000039

与现有技术相比,本发明的有益效果是:无需辅助信源而采用回转台提供的角度间隔信息进行校准,试验简便且更易实际操作。相比于平面波假设模型,采用基于球面波假设的近场聚焦波束形成处理方法估计结果更精确,能够克服传统校准方法对于校准场地的尺寸难以满足的问题,通用性强。此外,本发明的校准方法在频域中的一次快拍即可完成协方差矩阵的构建,有效减少了计算量,并且频域处理使得信号在解调频后无需低通滤波环节就能提取有效信息。Compared with the prior art, the invention has the beneficial effects of using the angle interval information provided by the turntable for calibration without the need of an auxiliary signal source, and the test is simple and practical. Compared with the plane wave assumption model, the near-field focused beamforming processing method based on the spherical wave assumption is more accurate in estimation results, which can overcome the problem that the traditional calibration method is difficult to meet the size of the calibration site, and has strong versatility. In addition, the calibration method of the present invention can complete the construction of the covariance matrix in a snapshot in the frequency domain, which effectively reduces the amount of calculation, and the frequency domain processing enables the signal to extract effective information without low-pass filtering after demodulation .

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为角度间隔估计偏差示意图;Fig. 2 is a schematic diagram of angular interval estimation deviation;

图3a为阵元间幅度校准前后示意图;Figure 3a is a schematic diagram before and after amplitude calibration between array elements;

图3b为阵元间相位校准前后示意图;Figure 3b is a schematic diagram before and after phase calibration between array elements;

图4为幅相一致性误差校准前后的波束形成图。Fig. 4 is the beamforming diagram before and after calibration of the amplitude-phase consistency error.

具体实施方式detailed description

下面举例对本发明做更详细的描述。The following examples describe the present invention in more detail.

结合图1至图4,本发明的接收换能器阵列幅相一致性近场校准方法主要包括以下几个步骤:1 to 4, the receiving transducer array amplitude-phase consistency near-field calibration method of the present invention mainly includes the following steps:

(1)处于回转台上的接收阵在不同方向采集的入射信号经过聚焦波束形成处理得到一系列的波达方向估计;(1) The incident signals collected by the receiving array on the turntable in different directions are processed by focused beamforming to obtain a series of direction-of-arrival estimates;

(2)在频域建立接收信号协方差矩阵,并建立幅相一致性误差估计模型;(2) Establish the received signal covariance matrix in the frequency domain, and establish the amplitude-phase consistency error estimation model;

(3)选取小角度入射角信号,将其邻域角度分别假设为理想入射角,根据幅相一致性误差估计模型估计对应邻域内角度的幅相误差;(3) Select the small-angle incident angle signal, assume its neighborhood angles as ideal incident angles, and estimate the amplitude-phase error corresponding to the angle in the neighborhood according to the amplitude-phase consistency error estimation model;

(4)根据误差结果补偿阵列,根据试验预设参数选择两已知角度间隔的数据,评估对于角度间隔估计的偏差,根据偏差极小值确定幅相一致性误差,完成校准。(4) Compensate the array according to the error result, select the data of two known angular intervals according to the test preset parameters, evaluate the deviation of the estimated angular interval, determine the amplitude-phase consistency error according to the minimum value of the deviation, and complete the calibration.

回转台作为待校准接收阵的载体能够采集不同方向上入射的信号,能够获得任意两组采样数据的入射角度间隔,通过聚焦波束形成估计多组数据的波达方向,选择具有小角度入射的数据遍历其角度邻域,采用协方差矩阵算法计算幅相误差,考察补偿后的阵列对具有两已知入射角间隔的数据的估计偏差,通过偏差极小值存在情况,调节邻域范围,最终确定幅相一致性误差,校准的流程如图1所示。As the carrier of the receiving array to be calibrated, the turntable can collect signals incident in different directions, obtain the incident angle interval of any two sets of sampling data, estimate the direction of arrival of multiple sets of data through focused beamforming, and select the data with small incident angles Traversing its angular neighborhood, using the covariance matrix algorithm to calculate the amplitude and phase errors, investigating the estimated deviation of the compensated array for data with two known incident angle intervals, adjusting the neighborhood range through the existence of the deviation minimum, and finally determining Amplitude-phase consistency error, the calibration process is shown in Figure 1.

步骤(1)中涉及的近场聚焦模型为:The near-field focusing model involved in step (1) is:

Figure BDA0002310787940000041
Figure BDA0002310787940000041

其中,V(θ)为对应于入射方向θ的波束输出,M为待估计阵列的阵元数,xm为第m个阵元接收到的信号,

Figure BDA0002310787940000042
为在第n个采样时刻下,接收信号在阵元m与参考阵元之间的相位差;Among them, V(θ) is the beam output corresponding to the incident direction θ, M is the number of array elements to be estimated, x m is the signal received by the mth array element,
Figure BDA0002310787940000042
is the phase difference of the received signal between element m and the reference element at the nth sampling moment;

上述建立的近场聚焦模型基于球面波假设,与平面波不同的是需要对接收信号的每一个采样时刻进行相位补偿以实现聚焦,

Figure BDA0002310787940000043
为:The near-field focusing model established above is based on the spherical wave assumption. Unlike the plane wave, it is necessary to perform phase compensation for each sampling moment of the received signal to achieve focusing.
Figure BDA0002310787940000043
for:

Figure BDA0002310787940000044
Figure BDA0002310787940000044

其中dm为第m个阵元相对于参考阵元的间距,λ为声波的波长,rn表示在第n个采样时刻下对应的聚焦距离。Where d m is the distance between the mth array element and the reference array element, λ is the wavelength of the sound wave, and r n is the corresponding focusing distance at the nth sampling moment.

步骤(2)建立幅相一致性误差估计模型,Γ和Φ分别作为阵列的幅度相位向量有:Step (2) Establish the amplitude-phase consistency error estimation model, Γ and Φ are used as the amplitude-phase vectors of the array respectively:

Γ=diag[ρ12,…,ρM]Γ=diag[ρ 12 ,…,ρ M ]

Figure BDA0002310787940000045
Figure BDA0002310787940000045

其中ρm

Figure BDA0002310787940000046
分别为第m个阵元的幅度和相位向量,并且有ρ1=1,
Figure BDA0002310787940000047
where ρ m and
Figure BDA0002310787940000046
are the magnitude and phase vectors of the mth array element respectively, and have ρ 1 =1,
Figure BDA0002310787940000047

则理想接收信号以及存在误差的接收信号可以表示为:Then the ideal received signal and the received signal with errors can be expressed as:

X0(t)=AS(t)+N(t)X 0 (t)=AS(t)+N(t)

X(t)=ΓΦ(AS(t)+N(t))X(t)=ΓΦ(AS(t)+N(t))

Figure BDA0002310787940000051
Figure BDA0002310787940000051

S(t)=[s1(t),s2(t),…,sM(t)]T(s1(t)=s2(t),…,=sM(t))S(t)=[s 1 (t),s 2 (t),…,s M (t)] T (s 1 (t)=s 2 (t),…,=s M (t))

N(t)=[n1(t),n2(t),…,nM(t)]T N(t)=[n 1 (t),n 2 (t),...,n M (t)] T

其中X0(t)和X(t)为以理想接收信号和实际接收信号矩阵。S(t)为信源发射信号组成的发射信号矩阵,N(t)为各阵元接收的噪声组成的噪声矩阵,其中噪声假设为高斯白噪声;Among them, X 0 (t) and X(t) are matrices based on the ideal received signal and the actual received signal. S(t) is the transmitted signal matrix composed of the signal transmitted by the source, and N(t) is the noise matrix composed of the noise received by each array element, where the noise is assumed to be Gaussian white noise;

将各阵元接收的理想信号X0(t)(各阵元幅相一致性误差一致)和实际信号X(t)经过傅里叶变换至频域得到X0 fre(f)和Xfre(f),分别提取距离零频最近频谱峰值X0 P和XPThe ideal signal X 0 (t) received by each array element (the amplitude and phase consistency error of each array element is consistent) and the actual signal X(t) are transformed into the frequency domain by Fourier transform to obtain X 0 fre (f) and X fre ( f), respectively extracting the spectrum peaks X 0 P and X P closest to the zero frequency:

Figure BDA0002310787940000052
Figure BDA0002310787940000052

Xfre(f)=[x1(f),x2(f),…,xM(f)]T X fre (f)=[x 1 (f), x 2 (f),…, x M (f)] T

Figure BDA0002310787940000053
Figure BDA0002310787940000053

XP=[P1,P2,…,PM]T X P =[P 1 ,P 2 ,…,P M ] T

并构建理想协方差矩阵和实际协方差矩阵

Figure BDA0002310787940000054
和RX:And construct the ideal covariance matrix and the actual covariance matrix
Figure BDA0002310787940000054
and R x :

Figure BDA0002310787940000055
Figure BDA0002310787940000055

Figure BDA0002310787940000056
Figure BDA0002310787940000056

幅相一致性误差矩阵Ω和各阵元幅相一致性误差ρ和

Figure BDA0002310787940000057
为:The amplitude-phase consistency error matrix Ω and the amplitude-phase consistency error ρ of each array element and
Figure BDA0002310787940000057
for:

Figure BDA0002310787940000058
Figure BDA0002310787940000058

Figure BDA0002310787940000059
Figure BDA0002310787940000059

Figure BDA00023107879400000510
Figure BDA00023107879400000510

步骤(3)中选择小角度的入射角为θ0的接收信号,在角度范围为ε的邻域中对邻域内K个角度遍历,使得理想角度θs满足θs(k)∈(θ0-ε,θ0+ε),计算对应邻域内各个角度的幅相一致性误差Ω(k)。In step (3), select the received signal with a small incident angle of θ 0 , and traverse K angles in the neighborhood in the neighborhood of angle range ε, so that the ideal angle θ s satisfies θ s (k)∈(θ 0 -ε,θ 0 +ε), calculate the amplitude-phase consistency error Ω(k) of each angle in the corresponding neighborhood.

步骤(4)对k组各通道幅度误差ρm(k)和相位误差

Figure BDA00023107879400000511
分别补偿阵列,选择两入射角间隔为Δθ的接收信号,其中参数Δθ0根据回转台获得,分别估计这两组信号的波达方向并计算其角度间隔Δθ(k),考察对角度间隔估计的偏差e(k)=|Δθ0-Δθ(k)|,若在角度邻域(θ0-ε,θ0+ε)内存在唯一极小值,则
Figure BDA00023107879400000512
理想角度为
Figure BDA00023107879400000513
换能器阵列各阵元的幅相误差为
Figure BDA0002310787940000061
Figure BDA0002310787940000062
Step (4) for each channel amplitude error ρ m (k) and phase error of group k
Figure BDA00023107879400000511
Compensate the array separately, select two received signals whose incident angle interval is Δθ, and the parameter Δθ 0 is obtained according to the turntable, estimate the direction of arrival of these two groups of signals and calculate their angular interval Δθ(k), and investigate the estimation of the angular interval Deviation e(k)=|Δθ 0 -Δθ(k)|, if there is a unique minimum value in the angle neighborhood (θ 0 -ε,θ 0 +ε), then
Figure BDA00023107879400000512
The ideal angle is
Figure BDA00023107879400000513
The amplitude and phase errors of each element of the transducer array are
Figure BDA0002310787940000061
and
Figure BDA0002310787940000062

对接收换能器阵列幅相一致性近场校准方法进行了仿真试验分析,待校准的阵列为一阵元数为M=100的均匀线列阵,阵元间距d=3.75mm,由于阵列安装在回转台上使得各数据间入射角度间隔为已知,回转台设定旋转范围为-90°~90°,回转速度为0.6°/s,信号源与接收阵距离为10m处于近场范围,发射高频窄带脉冲信号,其中发射信号中心频率为200kHz,脉冲宽度为0.1ms,信号发射的同时接收阵接收,周期均为1s,则共有300组接收信号,且每相邻两组数据的角度间隔为0.6°,其中以第150组数据的入射角度为理想的参考值,设为0.8°。引入幅度相位误差,各阵元幅度误差满足ρ~N(1,0.32),相位误差满足

Figure BDA0002310787940000063
存在幅相一致性误差情况下使得第150组数据的波束图的旁瓣级升高并导致波达方向估计偏差为0.9°。以0.9°对附近邻域进行搜索,由于设定的理想值为0.8°,则选择邻域为0.7°~0.9°进行遍历,每次遍历增量为0.01°,共21个角度,通过幅相一致性误差估计模型计算得到21组阵元间幅度相位误差,根据21组幅相误差对阵列补偿前,为结果更加明显应选择入射角较大的数据,适当选择两角度间隔为24°的两组数据,选择第100组数据和第140组数据,在每一组幅相误差补偿后,记录对两组数据的波达方向估计结果。经过处理,得到对应不同组数据的角度间隔估计误差。由图2可知,第11组幅相误差对阵列补偿后具有最佳的估计结果,对应的入射角度为0.8°与理想角度参考值一致,并且在邻域内具有唯一的极小值,因此阵列的幅度相位误差可以确定,幅相误差真实值与估计值的对比如图3a和图3b,阵列校准前后对第150组数据进行处理得到的波束图如图4。经过校准,阵列的测向精度得到了提高,波束图的旁瓣得到了抑制。The simulation test analysis of the near-field calibration method for the amplitude-phase consistency of the receiving transducer array is carried out. The array to be calibrated is a uniform linear array with the number of elements M=100, and the distance between elements d=3.75mm. Since the array is installed in The incident angle interval between each data is known on the turntable, the set rotation range of the turntable is -90°~90°, the rotation speed is 0.6°/s, the distance between the signal source and the receiving array is 10m in the near-field range, and the transmission High-frequency narrow-band pulse signal, in which the center frequency of the transmitted signal is 200kHz, and the pulse width is 0.1ms. The receiving array receives the signal at the same time as the signal is transmitted, and the cycle is 1s. There are 300 sets of received signals in total, and the angular interval between each adjacent two sets of data is 0.6°, where the incident angle of the 150th set of data is the ideal reference value and is set to 0.8°. Introducing amplitude and phase errors, the amplitude error of each array element satisfies ρ~N(1,0.3 2 ), and the phase error satisfies
Figure BDA0002310787940000063
In the case of amplitude-phase consistency error, the sidelobe level of the beam pattern of the 150th set of data increases and causes a deviation of 0.9° in the estimated direction of arrival. Search the nearby neighborhood at 0.9°. Since the ideal value set is 0.8°, select the neighborhood to traverse from 0.7° to 0.9°. Each traverse increment is 0.01°, a total of 21 angles, through the amplitude and phase The consistency error estimation model calculates the amplitude and phase errors between 21 groups of array elements. Before the array is compensated according to the 21 groups of amplitude and phase errors, the data with a larger incident angle should be selected for the result to be more obvious, and the two angles with an interval of 24° should be selected appropriately. Group data, select the 100th group of data and the 140th group of data, after each group of amplitude and phase error compensation, record the DOA estimation results of the two groups of data. After processing, angle interval estimation errors corresponding to different sets of data are obtained. It can be seen from Figure 2 that the 11th group of amplitude and phase errors has the best estimation result after array compensation, and the corresponding incident angle is 0.8°, which is consistent with the ideal angle reference value, and has a unique minimum value in the neighborhood, so the array’s The amplitude and phase error can be determined. The comparison between the real value and the estimated value of the amplitude and phase error is shown in Figure 3a and Figure 3b. The beam pattern obtained by processing the 150th set of data before and after array calibration is shown in Figure 4. After calibration, the direction finding accuracy of the array is improved and the side lobes of the beam pattern are suppressed.

综上,本发明提供了一种接收换能器阵列幅相一致性近场校准方法。无需辅助信源即可完成校准,尤其是在对孔径较大且阵元数较多的换能器阵列进行校准时,采用的基于近场球面波模型能够克服校准场地尺寸难以满足测量要求的现状。在频域中构造协方差矩阵简化了解调频步骤和计算复杂度,本发明提高了阵列的幅相一致性及测向性能,操作简便,适合工程应用。In summary, the present invention provides a near-field calibration method for amplitude-phase consistency of a receiving transducer array. Calibration can be completed without an auxiliary source, especially when calibrating a transducer array with a large aperture and a large number of elements, the near-field spherical wave model used can overcome the current situation that the size of the calibration site is difficult to meet the measurement requirements . Constructing a covariance matrix in the frequency domain simplifies the frequency modulation steps and calculation complexity, and the invention improves the amplitude-phase consistency and direction-finding performance of the array, is easy to operate, and is suitable for engineering applications.

Claims (4)

1. A near field calibration method for receiving the amplitude-phase consistency of a transducer array is characterized by comprising the following steps:
(1) Establishing a near-field focusing beam forming model, and carrying out focusing beam forming processing on incident signals acquired by a receiving array on a rotary table in different directions to obtain a series of direction-of-arrival estimations;
(2) Establishing a covariance matrix of a received signal in a frequency domain, and establishing an amplitude-phase consistency error estimation model;
establishing an amplitude-phase consistency error estimation model, wherein gamma and phi respectively serve as amplitude-phase vectors of the array and comprise:
Γ=diag[ρ 12 ,…,ρ M ]
Figure FDA0003876762660000011
where ρ is m And
Figure FDA0003876762660000012
amplitude and phase vectors of the m-th array element, respectively, and p 1 =1,
Figure FDA0003876762660000013
The ideal received signal and the received signal with errors are expressed as:
X 0 (t)=AS(t)+N(t)
X(t)=ΓΦ(AS(t)+N(t))
Figure FDA0003876762660000014
S(t)=[s 1 (t),s 2 (t),…,s M (t)] T (s 1 (t)=s 2 (t),…,=s M (t))
N(t)=[n 1 (t),n 2 (t),…,n M (t)] T
wherein, X 0 (t) and X (t) are matrices of ideal received signals and actual received signals; s (t) is a transmitting signal matrix formed by transmitting signals by an information source, N (t) is a noise matrix formed by noise received by each array element, wherein the noise is Gaussian white noise;
ideal signal X received by each array element 0 (t) Fourier transforming the actual signal X (t) to a frequency domain to obtain X 0 fre (f) And X fre (f) Respectively extracting the nearest frequency spectrum peak value X from the zero frequency 0 P And X P
Figure FDA0003876762660000015
X fre (f)=[x 1 (f),x 2 (f),…,x M (f)] T
Figure FDA0003876762660000016
X P =[P 1 ,P 2 ,…,P M ] T
And constructing an ideal covariance matrix and an actual covariance matrix
Figure FDA0003876762660000017
And R X
Figure FDA0003876762660000018
Figure FDA0003876762660000019
Amplitude-phase consistency error matrix omega and amplitude-phase consistency errors rho and
Figure FDA00038767626600000110
comprises the following steps:
Figure FDA0003876762660000021
(3) Selecting small-angle incident angle signals, setting the neighborhood angles of the small-angle incident angle signals as ideal incident angles, and estimating the amplitude-phase error corresponding to the angles in the neighborhood according to an amplitude-phase consistency error estimation model;
(4) And according to the error result compensation array, selecting data of two known angle intervals according to preset parameters, evaluating the deviation estimated for the angle intervals, determining amplitude-phase consistency errors according to the minimum deviation value, and finishing calibration.
2. The method of claim 1, wherein the near field focused beam forming model comprises:
Figure FDA0003876762660000022
wherein V (theta) is the beam output corresponding to the incident direction theta, M is the array element number of the array to be estimated, and x m For the signal received by the m-th array element,
Figure FDA0003876762660000023
is the phase difference of the received signal between the array element m and the reference array element at the nth sampling time.
3. The method of claim 2 wherein in step (3) the angle of incidence is selected to be a small angle θ 0 Traversing K angles in the neighborhood with the angle range of epsilon to ensure that the ideal angle theta s Satisfies theta s (k)∈(θ 0 -ε,θ 0 + epsilon), the amplitude-phase consistency error omega (k) for each angle in the neighborhood is calculated.
4. The method of claim 3, wherein the step (4) is specifically as follows:
for k groups of channel amplitude errors rho m (k) And phase error
Figure FDA0003876762660000024
Respectively compensating the arrays, selecting two incidence angles with a delta theta interval 0 In which the parameter delta theta 0 Obtained from the rotary table, the directions of arrival of the two sets of signals are estimated, the angular interval delta theta (k) is calculated, and the deviation e (k) = | delta theta (k) of the angular interval estimation is considered 0 - Δ θ (k) | if in angular neighborhood (θ) 0 -ε,θ 0 + ε) has a unique minimum value, then
Figure FDA0003876762660000025
The ideal angle is
Figure FDA0003876762660000026
The amplitude-phase error of each array element of the transducer array is
Figure FDA0003876762660000027
And
Figure FDA0003876762660000028
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