CN108169732A - A kind of transform domain Beamforming Method based on extension aperture sonar - Google Patents

A kind of transform domain Beamforming Method based on extension aperture sonar Download PDF

Info

Publication number
CN108169732A
CN108169732A CN201810165058.XA CN201810165058A CN108169732A CN 108169732 A CN108169732 A CN 108169732A CN 201810165058 A CN201810165058 A CN 201810165058A CN 108169732 A CN108169732 A CN 108169732A
Authority
CN
China
Prior art keywords
transmitting
array
signal
domain
different
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201810165058.XA
Other languages
Chinese (zh)
Other versions
CN108169732B (en
Inventor
朴胜春
闫路
郭微
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Harbin Engineering University
Original Assignee
Harbin Engineering University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Harbin Engineering University filed Critical Harbin Engineering University
Priority to CN201810165058.XA priority Critical patent/CN108169732B/en
Publication of CN108169732A publication Critical patent/CN108169732A/en
Application granted granted Critical
Publication of CN108169732B publication Critical patent/CN108169732B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • 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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/52Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00
    • G01S7/539Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Abstract

The invention discloses a kind of transform domain Beamforming Methods based on extension aperture sonar, belong to field of underwater acoustic signal processing.The present invention includes:According to sonar system index request, according to the equivalent array element phase center principle of extension aperture sonar, i.e. one transmitting array element receives array element with one and forms a module, and the phase center of this module is located at the geometric center of two array element, reasonable Arrangement transmitting battle array, the position for receiving battle array;Formation is received according to the transmitting of arrangement, at transmitting basic matrix end, transmitting battle array emits mutually orthogonal waveform simultaneously;Receive the reflection signal that battle array receives target, i.e. echo-signal;It carries out reception Wave beam forming processing respectively in transform domain to echo-signal, carries out transform domain filtering and receive Wave beam forming;The signal after Wave beam forming processing is received to transform domain, to different transmitting formation into delay inequality compensated with Wave beam forming, and then obtain the distance of extension aperture sonar to angle to sound spectrogram.

Description

A kind of transform domain Beamforming Method based on extension aperture sonar
Technical field
The invention belongs to field of underwater acoustic signal processing, and in particular to a kind of transform domain wave beam shape based on extension aperture sonar Into method.
Background technology
In recent years, multi-beam image sonar technology is in seafloor topography mapping, oil pipeline detection and submarine target Field of detecting is widely used, in order to obtain high-definition sonar image, need to improve simultaneously sonar image away from Descriscent resolution ratio and angle are to resolution ratio.
In wideband signaling system, distance resolution is usually determined by the effective bandwidth of reception signal, and angular resolution Usually determined by the effective aperture of receiving array and reception signal frequency.In practical applications, image sonar is specifically being applied In field, changing its specific operating frequency range will cause its detection performance to decline, and therefore, usually select and expand sonar system Improve angular resolution in the effective receiving array aperture of system.
In order not to increase array sizes, the hardware cost of transducer array is reduced, virtual extended aperture sonar may be used Angle is improved to resolution ratio, operation principle is that orthogonal waveforms are penetrated in different transmitting paroxysm, receiving terminal by matched filtering into Row transmitting Signal separator, then does reception and launching beam is formed, and achievees the purpose that the practical receiving array aperture of extension.But in work In Cheng Yingyong, completely orthogonal signal is not present, then distance will be led to side by emitting the high cross correlation between signal Valve is raised, and reduces the distance of sonar image to clarity.
Invention content
The invention is realized in this way:
A kind of transform domain Beamforming Method based on extension aperture sonar, which is characterized in that comprise the steps of:
Step 1 is according to sonar system index request, according to the equivalent array element phase center principle of extension aperture sonar, i.e., One transmitting array element receives array element with one and forms a module, and the phase center of this module is located in the geometry of two array element The heart, reasonable Arrangement transmitting battle array, the position for receiving battle array;If sonar receiving array is one-dimensional array, two transmitting battle array cloth are placed on Receive the both ends of battle array, if sonar receiving array is two-dimensional planar array, orientation and pitching to being required for extending, then receive it is flat Four transmitting battle arrays are laid around the array of face;If a uniform rectilinear receiving array, adjacent array element spacing be half-wavelength, element number of array For M, two transmitting battle arrays are arranged at array both ends, then the angle for extending aperture sonar is expressed as to beam angle
In formula, BW be angle to beam angle, unit is radian, and λ is transmitting signal wavelength, and d is adjacent reception array element Spacing,For wave beam offset angle, setting
If a uniform two dimensional surface receiving array, adjacent array element spacing be half-wavelength, horizontal direction element number of array be L, pitching It is Q to element number of array, four emission arrays are arranged in four angles of receiving plane battle array, then horizontal direction beam angle and pitching are to wave beam Width is:
Wherein, BWθFor horizontal direction beam angle,It is pitching to beam angle, dθFor the adjacent array element spacing of horizontal direction,It is pitching to adjacent array element spacing;
Step 2 receives formation according to the transmitting of arrangement, and at transmitting basic matrix end, transmitting battle array emits mutually orthogonal waveform simultaneously, In practice there is no completely orthogonal signal, design emits the signal different signal of feature in the transform domain as illustrated, with one-dimensional reception battle array Example, two transmitting battle arrays, the sinusoidal signal of two different frequencies of transmitting are classified as, and the frequency response curve -3dB of two signals is without weight Folded, i.e., frequency is without intersection, then the frequecy characteristic of this two transmitting signals is different;For another example believe in the positive negative frequency modulation of different center frequency Number, then two transmitting signals have different characteristics in STFT time-frequency domains, you can it is orthogonal letter to think that two transmitting paroxysms are penetrated Number;
s1(t)=cos (2 π f1t+K1πt2)
s2(t)=cos (2 π f2t+K2πt2)
In formula, s1(t), s2(t) orthogonal signalling penetrated for the transmitting paroxysm at both ends, the transmission center frequency values of a transmitting battle array For f1, frequency change rate K1, t is time point, and the transmission center frequency values of another transmitting battle array are f2, frequency change rate K2, The centre frequency of two signals is different, and frequency change rate is different;
Step 3 receives the reflection signal that battle array receives target, i.e. echo-signal, contains multiple Orthogonal injections in echo-signal The superposition of the target echo of signal, it is right with reference to transmitting orthogonal signalling in the different feature of transform domain to realize waveform separation Echo-signal carries out receiving Wave beam forming processing in transform domain respectively, carries out transform domain filtering and receives Wave beam forming;
If receiving array is one dimensional linear array, two transmitting signal transmitting different frequency signals, two signals are in the spy of frequency domain Sign is different, then carries out reception Wave beam forming in different frequency respectively;If the frequency modulation up and down of two transmitting signal transmitting different frequencies Signal since two class signals have different characteristics in not same order Fourier Transform of Fractional Order domain, becomes according to fractional order Fourier Change with extraction multi -components chirp signal parameters ability, then using respectively different rank Fourier Transform of Fractional Order domain into Row receives Wave beam forming processing;
The docking collection of letters number carries out a Fourier Transform of Fractional Order for not same order respectively, i.e.,
In formula, x (t) is the target echo received,For p1The Fourier Transform of Fractional Order kernel function of rank,For the corresponding p of x (t)1The Fourier Transform of Fractional Order domain function of rank,For p2The Fourier Transform of Fractional Order of rank Kernel function,For the corresponding p of x (t)2The Fourier Transform of Fractional Order domain function of rank;
Step 4 inverse transform domain converts, and launching beam is formed;The signal after Wave beam forming processing is received to transform domain, into Row inverse transform domain converts, and transforms to Beam Domain time-domain signal, according to the delay inequality that different transmitting battle arrays reflects to form target, Time domain carry out launching beam formation processing, i.e., to it is different transmitting formation into delay inequality compensated with Wave beam forming, and then obtain expand The distance of aperture sonar is opened up to angle to sound spectrogram.
Compared with prior art, the beneficial effects of the present invention are:
1st, proposition method of the invention can reduce the influence that transmitted waveform high correlation is adjusted the distance to high secondary lobe, realize and expand The sound spectrogram distance of aperture sonar is opened up to high-resolution map.
2nd, proposition method of the invention can select to realize in multiple transform domains, realize that flow is simple, it is easy to accomplish.
Description of the drawings
Fig. 1 is one-dimensional array extension aperture principle schematic of the present invention;
Fig. 2 is two-dimensional planar array extension aperture sonar transducer array arrangement schematic diagram of the present invention;
Fig. 3 is invention implementing procedure block diagram;
Fig. 4 is that receiving array aperture beams figure of the present invention compares.
Specific embodiment
Invention is described in more detail below in conjunction with the accompanying drawings:
The present invention relates to a kind of transform domain Beamforming Method based on extension aperture sonar, due to virtual extended aperture sound It receives in system, emits the incomplete orthogonal of signal, reduce the distance of sonar image to clarity, which is connect using transform domain Receiving Beamforming Method realizes the distance of virtual extended aperture sonar to fine definition.The inventive method is first according to virtual extended Aperture is theoretical, reasonable Arrangement emission array receiving array, and then each transmitting basic matrix transmitting orthogonal waveforms, reception basic matrix receive more The target echo signal of a orthogonal waveforms superposition, it is different in transform domain feature according to different orthogonal waveform, it is directed in transform domain Multigroup orthogonal waveforms do reception array beamforming, and do inverse transform domain transformation respectively, finally carry out transmitting array beam in time domain It is formed.This method do not need to using matched filtering carry out orthogonal waveforms Signal separator, using orthogonal signalling transform domain feature Difference receives Wave beam forming using transform domain, solves in practical application distance caused by orthogonal time-domain waveform high correlation to height Secondary lobe, obtained while angular resolution is improved distance to fine definition, integrally improve sonar image quality.
Specific embodiment one:
In this example, systematic parameter:Receiving array is one dimensional linear array, and angle is 1.5 ° to beam angle, receives basic matrix Working frequency be 60kHz, velocity of sound 1500m/s, operating distance 50m, signal sampling rate 300kHz.
1. calculating process:
Assuming that receiving array is a uniform linear array, adjacent array element spacing is the half-wavelength of receiving array working frequency, In order to meet system perspective to beam angle requirement, can be obtained according to formula,
It then can be calculated, the element number of array in practical receiving array is designed as 36, and the both ends for receiving basic matrix lay two Emit basic matrix.
According to the receiving array parameter calculated, emulated by Fig. 4 it is found that the beam angle for extending system after aperture is approximately The 0.55 of practical receiving array system beam angle, improves angle to resolution ratio.
Two transmitting basic matrixs, emit mutually orthogonal signal, and signal waveform is respectively that centre frequency is 55kHz positive frequency modulation signals It is 85kHz negative frequency modulation signals with centre frequency, transmitted signal bandwidth is 3kHz, and pulsewidth is 10ms.
Receiving array receives target echo signal, and analysis is it is found that the two emits signal in not same order fractional order Fourier Transform domain has a different characteristics, and echo-signal carries out-1.539 rank Fourier Transform of Fractional Order first, it is known that, transmitting signal 1- In 1.539 rank transform domains there is strong component, and carry out received wave beam and formed to obtain transform-domain signals y1While echo-signal (u), Carry out 1.539 rank Fourier Transform of Fractional Order, it is known that, transmitting signal 2 has strong component, and carry out in 1.539 rank transform domains It receives Wave beam forming and obtains transform-domain signals y2(u), it avoids and waveform separation is carried out using correlation function, lead to distance by height Valve.
Then to transform-domain signals y1(u) and transform-domain signals y2(u) inverse transform domain transformation is carried out, transforms to time-domain signal Respectively y1(t) and transform-domain signals y2(t), delay compensation progress launching beam is carried out again later to be formed.
The final distance that obtains is to fine definition and angle to high-definition picture.
Specific embodiment two:
1. first according to sonar system index request, according to the equivalent array element phase center principle of extension aperture sonar, i.e., One transmitting array element receives array element with one and forms a module, and the phase center of this module is located in the geometry of two array element The heart, reasonable Arrangement transmitting battle array, the position for receiving battle array.If sonar receiving array is one-dimensional array, two transmitting battle array cloth are placed on Receive the both ends of battle array, if sonar receiving array is two-dimensional planar array, orientation and pitching to being required for extending, then receive it is flat Four transmitting battle arrays are laid around the array of face, respectively as depicted in figs. 1 and 2.Assuming that a uniform rectilinear receiving array, adjacent array element Spacing is half-wavelength, element number of array M, and two transmitting battle arrays are arranged at array both ends, then the angle for extending aperture sonar is wide to wave beam Degree is expressed as
In formula, BW be angle to beam angle, unit is radian, and λ is transmitting signal wavelength, and d is adjacent reception array element Spacing,For wave beam offset angle, the method, settingIt is found that the beam angle of extension aperture sonar is approximately practical reception The 0.55 of array aperture, then angle about doubled to resolution ratio.
Assuming that a uniform two dimensional surface receiving array, adjacent array element spacing is half-wavelength, and horizontal direction element number of array is L, is bowed It is Q to face upward to element number of array, and four emission arrays are arranged in four angles of receiving plane battle array, then horizontal direction beam angle and pitching are to wave Beam width is
Wherein, BWθFor horizontal direction beam angle,It is pitching to beam angle, dθFor the adjacent array element spacing of horizontal direction,It is pitching to adjacent array element spacing.
It is found that after planar array extension, horizontal direction beam angle and pitching are practical reception battle array respectively to beam angle To the 0.55 of beam angle, i.e. horizontal direction and pitching improves one to angular resolution for the horizontal direction beam angle of row and pitching Times.
Wherein, Fig. 2 orbicular spots lay reception array element, and four corner black array elements of plane are laid to emit battle array.
2. the transmitting according to arrangement receives formation, at transmitting basic matrix end, transmitting battle array emits mutually orthogonal waveform simultaneously, practical In there is no completely orthogonal signal, the design transmitting signal different signal of feature in the transform domain as illustrated, using one-dimensional receiving array as Example, two transmitting battle arrays, the sinusoidal signal of two different frequencies of transmitting, and the frequency response curve -3dB of two signals is non-overlapping, I.e. frequency is without intersection, then the frequecy characteristic of this two transmitting signals is different;For another example in the positive and negative FM signal of different center frequency, Then two transmitting signals have different characteristics in STFT time-frequency domains, you can it is orthogonal signalling to think that two transmitting paroxysms are penetrated.
s1(t)=cos (2 π f1t+K1πt2)
s2(t)=cos (2 π f2t+K2πt2)
In formula, s1(t), s2(t) orthogonal signalling penetrated for the transmitting paroxysm at both ends, the transmission center frequency values of a transmitting battle array For f1, frequency change rate K1, t is time point, and the transmission center frequency values of another transmitting battle array are f2, frequency change rate K2, The centre frequency of two signals is different, and frequency change rate is different.
3. receiving the reflection signal that battle array receives target, i.e. echo-signal, contain multiple Orthogonal injection signals in echo-signal Target echo superposition, in order to realize that waveform detaches, with reference to transmitting orthogonal signalling in the different feature of transform domain, to returning Wave signal carries out receiving Wave beam forming processing in transform domain respectively, carries out transform domain filtering and receives Wave beam forming.
Assuming that receiving array is one dimensional linear array, two transmitting signal transmitting different frequency signals, two signals are in frequency domain Feature is different, then carries out reception Wave beam forming in different frequency respectively;If the upper downward of two transmitting signal transmitting different frequencies Frequency signal, since two class signals have different characteristics in not same order Fourier Transform of Fractional Order domain, according to fractional order Fourier Ability of the variation with extraction multi -components chirp signal parameters, then use respectively in different rank Fourier Transform of Fractional Order domain It carries out receiving Wave beam forming processing.
The docking collection of letters number carries out a Fourier Transform of Fractional Order for not same order respectively, i.e.,
In formula, x (t) is the target echo received,For p1The Fourier Transform of Fractional Order kernel function of rank,For the corresponding p of x (t)1The Fourier Transform of Fractional Order domain function of rank,For p2The Fourier Transform of Fractional Order of rank Kernel function,For the corresponding p of x (t)2The Fourier Transform of Fractional Order domain function of rank.
4. inverse transform domain converts, launching beam is formed.The signal after Wave beam forming processing is received to transform domain, is carried out inverse Transform domain converts, and Beam Domain time-domain signal is transformed to, according to the delay inequality that different transmitting battle arrays reflects to form target, in time domain Carry out launching beam formation processing, i.e., to it is different transmitting formation into delay inequality compensated with Wave beam forming, and then obtain extending bore The distance of diameter sonar is to angle to sound spectrogram.
The concrete operation method of the present invention is as follows:
1. first according to sonar system index request, according to the equivalent array element phase center principle of extension aperture sonar, i.e., One transmitting array element receives array element with one and forms a module, and the phase center of this module is located in the geometry of two array element The heart, reasonable Arrangement transmitting battle array, the position for receiving battle array.If sonar receiving array is one-dimensional array, two transmitting battle array cloth are placed on Receive the both ends of battle array, if sonar receiving array is two-dimensional planar array, orientation and pitching to being required for extending, then receive it is flat Four transmitting battle arrays are laid around the array of face, respectively as depicted in figs. 1 and 2.Assuming that a uniform rectilinear receiving array, adjacent array element Spacing is half-wavelength, element number of array M, and two transmitting battle arrays are arranged at array both ends, then the angle for extending aperture sonar is wide to wave beam Degree is expressed as
In formula, BW be angle to beam angle, unit is radian, and λ is transmitting signal wavelength, and d is adjacent reception array element Spacing,For wave beam offset angle, the method, settingIt is found that the beam angle of extension aperture sonar is approximately practical reception The 0.55 of array aperture, then angle about doubled to resolution ratio.
Assuming that a uniform two dimensional surface receiving array, adjacent array element spacing is half-wavelength, and horizontal direction element number of array is L, is bowed It is Q to face upward to element number of array, and four emission arrays are arranged in four angles of receiving plane battle array, then horizontal direction beam angle and pitching are to wave Beam width is
It is found that after planar array extension, horizontal direction beam angle and pitching are practical reception battle array respectively to beam angle To the 0.55 of beam angle, i.e. horizontal direction and pitching improves one to angular resolution for the horizontal direction beam angle of row and pitching Times.
Wherein, Fig. 2 orbicular spots lay reception array element, and four corner black array elements of plane are laid to emit battle array.
2. the transmitting according to arrangement receives formation, at transmitting basic matrix end, transmitting battle array emits mutually orthogonal waveform simultaneously, practical In there is no completely orthogonal signal, the design transmitting signal different signal of feature in the transform domain as illustrated, using one-dimensional receiving array as Example, two transmitting battle arrays, the sinusoidal signal of two different frequencies of transmitting, and the frequency response curve -3dB of two signals is non-overlapping, I.e. frequency is without intersection, then the frequecy characteristic of this two transmitting signals is different;For another example in the positive and negative FM signal of different center frequency, Then two transmitting signals have different characteristics in STFT time-frequency domains, you can it is orthogonal signalling to think that two transmitting paroxysms are penetrated.
s1(t)=cos (2 π f1t+K1πt2)
s2(t)=cos (2 π f2t+K2πt2)
In formula, s1(t), s2(t) orthogonal signalling penetrated for the transmitting paroxysm at both ends, the transmission center frequency values of a transmitting battle array For f1, frequency change rate K1, t is time point, and the transmission center frequency values of another transmitting battle array are f2, frequency change rate K2, The centre frequency of two signals is different, and frequency change rate is different.
3. receiving the reflection signal that battle array receives target, i.e. echo-signal, contain multiple Orthogonal injection signals in echo-signal Target echo superposition, in order to realize that waveform detaches, with reference to transmitting orthogonal signalling in the different feature of transform domain, to returning Wave signal carries out receiving Wave beam forming processing in transform domain respectively, carries out transform domain filtering and receives Wave beam forming.
Assuming that receiving array is one dimensional linear array, two transmitting signal transmitting different frequency signals, two signals are in frequency domain Feature is different, then carries out reception Wave beam forming in different frequency respectively;If the upper downward of two transmitting signal transmitting different frequencies Frequency signal, since two class signals have different characteristics in not same order Fourier Transform of Fractional Order domain, according to fractional order Fourier Ability of the variation with extraction multi -components chirp signal parameters, then use respectively in different rank Fourier Transform of Fractional Order domain It carries out receiving Wave beam forming processing.
The docking collection of letters number carries out a Fourier Transform of Fractional Order for not same order respectively, i.e.,
In formula, x (t) is the target echo received,For p1The Fourier Transform of Fractional Order kernel function of rank,For the corresponding p of x (t)1The Fourier Transform of Fractional Order domain function of rank,For p2The Fourier Transform of Fractional Order of rank Kernel function,For the corresponding p of x (t)2The Fourier Transform of Fractional Order domain function of rank.
4. pair transform domain receives the signal after Wave beam forming processing, inverse transform domain transformation is carried out, when transforming to Beam Domain According to the delay inequality that transmitting battle array reflects to form target, transmitting terminal Wave beam forming processing is carried out, and then obtain in time domain for domain signal The distance of aperture sonar is extended to angle to sound spectrogram.

Claims (1)

1. a kind of transform domain Beamforming Method based on extension aperture sonar, which is characterized in that comprise the steps of:
Step 1 is according to sonar system index request, according to the equivalent array element phase center principle of extension aperture sonar, i.e., one Emit array element and receive array element one module of composition with one, the phase center of this module is located at the geometric center of two array element, closes Removing the work puts transmitting battle array, the position for receiving battle array;If sonar receiving array is one-dimensional array, two transmitting battle array cloth are placed on reception battle array Both ends, if sonar receiving array is two-dimensional planar array, orientation and pitching to being required for extending, then in receiving plane array Around lay four transmitting battle arrays;If a uniform rectilinear receiving array, adjacent array element spacing be half-wavelength, element number of array M, battle array It arranges both ends and arranges two transmitting battle arrays, then the angle for extending aperture sonar is expressed as to beam angle
In formula, BW be angle to beam angle, unit is radian, and λ is transmitting signal wavelength, and d is adjacent reception array element spacing,For wave beam offset angle, setting
If a uniform two dimensional surface receiving array, adjacent array element spacing is half-wavelength, and horizontal direction element number of array is L, and pitching is to battle array First number is Q, and four emission arrays are arranged in four angles of receiving plane battle array, then horizontal direction beam angle and pitching are to beam angle For:
Wherein, BWθFor horizontal direction beam angle,It is pitching to beam angle, dθFor the adjacent array element spacing of horizontal direction,To bow It faces upward to adjacent array element spacing;
Step 2 receives formation according to the transmitting of arrangement, and at transmitting basic matrix end, transmitting battle array emits mutually orthogonal waveform simultaneously, practical In there is no completely orthogonal signal, the design transmitting signal different signal of feature in the transform domain as illustrated, using one-dimensional receiving array as Example, two transmitting battle arrays, the sinusoidal signal of two different frequencies of transmitting, and the frequency response curve -3dB of two signals is non-overlapping, I.e. frequency is without intersection, then the frequecy characteristic of this two transmitting signals is different;For another example in the positive and negative FM signal of different center frequency, Then two transmitting signals have different characteristics in STFT time-frequency domains, you can it is orthogonal signalling to think that two transmitting paroxysms are penetrated;
s1(t)=cos (2 π f1t+K1πt2)
s2(t)=cos (2 π f2t+K2πt2)
In formula, s1(t), s2(t) orthogonal signalling penetrated for the transmitting paroxysm at both ends, the transmission center frequency values of a transmitting battle array are f1, Frequency change rate is K1, t is time point, and the transmission center frequency values of another transmitting battle array are f2, frequency change rate K2, two The centre frequency of signal is different, and frequency change rate is different;
Step 3 receives the reflection signal that battle array receives target, i.e. echo-signal, contains multiple Orthogonal injection signals in echo-signal Target echo superposition, to realize waveform separation, with reference to transmitting orthogonal signalling in the different feature of transform domain, to echo Signal carries out receiving Wave beam forming processing in transform domain respectively, carries out transform domain filtering and receives Wave beam forming;
If receiving array be one dimensional linear array, two transmitting signals transmitting different frequency signals, two signals frequency domain feature not Together, then reception Wave beam forming is carried out in different frequency respectively;If the FM signal up and down of two transmitting signal transmitting different frequencies, Since two class signals have different characteristics in not same order Fourier Transform of Fractional Order domain, had according to fractional order Fourier variation The ability of multi -components chirp signal parameters is extracted, then uses and is received respectively in different rank Fourier Transform of Fractional Order domain Wave beam forming processing;
The docking collection of letters number carries out a Fourier Transform of Fractional Order for not same order respectively, i.e.,
In formula, x (t) is the target echo received,For p1The Fourier Transform of Fractional Order kernel function of rank, For the corresponding p of x (t)1The Fourier Transform of Fractional Order domain function of rank,For p2The Fourier Transform of Fractional Order core letter of rank Number,For the corresponding p of x (t)2The Fourier Transform of Fractional Order domain function of rank;
Step 4 inverse transform domain converts, and launching beam is formed;The signal after Wave beam forming processing is received to transform domain, is carried out inverse Transform domain converts, and Beam Domain time-domain signal is transformed to, according to the delay inequality that different transmitting battle arrays reflects to form target, in time domain Carry out launching beam formation processing, i.e., to it is different transmitting formation into delay inequality compensated with Wave beam forming, and then obtain extending bore The distance of diameter sonar is to angle to sound spectrogram.
CN201810165058.XA 2018-02-28 2018-02-28 Transform domain beam forming method based on extended aperture sonar Active CN108169732B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810165058.XA CN108169732B (en) 2018-02-28 2018-02-28 Transform domain beam forming method based on extended aperture sonar

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810165058.XA CN108169732B (en) 2018-02-28 2018-02-28 Transform domain beam forming method based on extended aperture sonar

Publications (2)

Publication Number Publication Date
CN108169732A true CN108169732A (en) 2018-06-15
CN108169732B CN108169732B (en) 2021-08-20

Family

ID=62510700

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810165058.XA Active CN108169732B (en) 2018-02-28 2018-02-28 Transform domain beam forming method based on extended aperture sonar

Country Status (1)

Country Link
CN (1) CN108169732B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108761433A (en) * 2018-08-02 2018-11-06 西北工业大学 A kind of high-resolution imaging method handled using MIMO sonar difference combined arrays
CN113702978A (en) * 2021-08-04 2021-11-26 中国科学院声学研究所 Submarine pipeline detection positioning method and system based on forward-looking sonar

Citations (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5612929A (en) * 1995-12-27 1997-03-18 The United States Of America As Represented By The Secretary Of The Navy Spectral processor and range display unit
US5923617A (en) * 1997-02-05 1999-07-13 The United States Of America As Represented By The Secretary Of The Navy Frequency-steered acoustic beam forming system and process
US6879543B1 (en) * 2003-08-07 2005-04-12 The United States Of America As Represented By The Secretary Of The Navy Acoustic processing for estimating size of small targets
JP2006234478A (en) * 2005-02-23 2006-09-07 Japan Agengy For Marine-Earth Science & Technology Method of correcting platform oscillation in synthetic aperture processing system
US20070159376A1 (en) * 2006-01-11 2007-07-12 Raytheon Company Interrupt SAR implementation for range migration (RMA) processing
CN101470195A (en) * 2007-12-26 2009-07-01 中国科学院声学研究所 Non-parameter type high-resolution beam forming method and apparatus
CN101609150A (en) * 2009-07-07 2009-12-23 哈尔滨工程大学 A kind of fast beam formation method that improves array resolution and gain
CN101702027A (en) * 2009-12-02 2010-05-05 电子科技大学 Nonuniform frequency spectrum reconfiguration method of orientation multi-beam synthetic aperture radar
CN101813772A (en) * 2009-12-31 2010-08-25 中国科学院声学研究所 Array beamforming method by quickly expanding and dragging broadband frequency domain
CN101825709A (en) * 2009-12-08 2010-09-08 中国科学院声学研究所 Underwater high-resolution side-looking acoustic imaging system and method thereof
CN103576156A (en) * 2012-07-18 2014-02-12 中国科学院声学研究所 Synthetic aperture sonar imaging method and system based on frequency division MIMO
CN103616693A (en) * 2013-11-22 2014-03-05 江苏科技大学 Fish finding sonar and sonar echo signal processing method
CN103675819A (en) * 2012-09-06 2014-03-26 中国科学院声学研究所 Target detection method and system capable of being used for passive synthetic aperture array yawing
US20140321235A1 (en) * 2013-04-24 2014-10-30 Ofodike A. Ezekoye Acoustic sonar imaging and detection system for firefighting applications
CN104656073A (en) * 2013-11-21 2015-05-27 中国科学院声学研究所 Three-dimensional imaging sonar wave beam forming method and implementation method on multi-core processor
CN104811867A (en) * 2015-04-29 2015-07-29 西安电子科技大学 Spatial filtering method for microphone array based on virtual array extension
CN105319543A (en) * 2015-06-26 2016-02-10 中国科学院声学研究所 Wave beam forming method based on constant horizontal resolution
CN106291516A (en) * 2016-07-27 2017-01-04 河海大学 A kind of elimination method of sonar response formula interference
CN106991708A (en) * 2017-04-27 2017-07-28 飞依诺科技(苏州)有限公司 The processing method and processing system of ultrasonic Doppler blood flow imaging
CN107505604A (en) * 2017-09-02 2017-12-22 中国人民解放军91388部队 A kind of echo simulation method for considering sending and receiving directivity

Patent Citations (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5612929A (en) * 1995-12-27 1997-03-18 The United States Of America As Represented By The Secretary Of The Navy Spectral processor and range display unit
US5923617A (en) * 1997-02-05 1999-07-13 The United States Of America As Represented By The Secretary Of The Navy Frequency-steered acoustic beam forming system and process
US6879543B1 (en) * 2003-08-07 2005-04-12 The United States Of America As Represented By The Secretary Of The Navy Acoustic processing for estimating size of small targets
JP2006234478A (en) * 2005-02-23 2006-09-07 Japan Agengy For Marine-Earth Science & Technology Method of correcting platform oscillation in synthetic aperture processing system
US20070159376A1 (en) * 2006-01-11 2007-07-12 Raytheon Company Interrupt SAR implementation for range migration (RMA) processing
CN101470195A (en) * 2007-12-26 2009-07-01 中国科学院声学研究所 Non-parameter type high-resolution beam forming method and apparatus
CN101609150A (en) * 2009-07-07 2009-12-23 哈尔滨工程大学 A kind of fast beam formation method that improves array resolution and gain
CN101702027A (en) * 2009-12-02 2010-05-05 电子科技大学 Nonuniform frequency spectrum reconfiguration method of orientation multi-beam synthetic aperture radar
CN101825709A (en) * 2009-12-08 2010-09-08 中国科学院声学研究所 Underwater high-resolution side-looking acoustic imaging system and method thereof
CN101813772A (en) * 2009-12-31 2010-08-25 中国科学院声学研究所 Array beamforming method by quickly expanding and dragging broadband frequency domain
CN103576156A (en) * 2012-07-18 2014-02-12 中国科学院声学研究所 Synthetic aperture sonar imaging method and system based on frequency division MIMO
CN103675819A (en) * 2012-09-06 2014-03-26 中国科学院声学研究所 Target detection method and system capable of being used for passive synthetic aperture array yawing
US20140321235A1 (en) * 2013-04-24 2014-10-30 Ofodike A. Ezekoye Acoustic sonar imaging and detection system for firefighting applications
CN104656073A (en) * 2013-11-21 2015-05-27 中国科学院声学研究所 Three-dimensional imaging sonar wave beam forming method and implementation method on multi-core processor
CN103616693A (en) * 2013-11-22 2014-03-05 江苏科技大学 Fish finding sonar and sonar echo signal processing method
CN104811867A (en) * 2015-04-29 2015-07-29 西安电子科技大学 Spatial filtering method for microphone array based on virtual array extension
CN105319543A (en) * 2015-06-26 2016-02-10 中国科学院声学研究所 Wave beam forming method based on constant horizontal resolution
CN106291516A (en) * 2016-07-27 2017-01-04 河海大学 A kind of elimination method of sonar response formula interference
CN106991708A (en) * 2017-04-27 2017-07-28 飞依诺科技(苏州)有限公司 The processing method and processing system of ultrasonic Doppler blood flow imaging
CN107505604A (en) * 2017-09-02 2017-12-22 中国人民解放军91388部队 A kind of echo simulation method for considering sending and receiving directivity

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
张小飞,汪飞,徐大专: "《阵列信号处理的理论和应用》", 30 November 2010, 国防工业出版社 *
段江涛,黄勇,刘纪元: "多维波形编码合成孔径声呐技术研究", 《声学学报》 *

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108761433A (en) * 2018-08-02 2018-11-06 西北工业大学 A kind of high-resolution imaging method handled using MIMO sonar difference combined arrays
CN108761433B (en) * 2018-08-02 2022-04-08 西北工业大学 High-resolution imaging method using MIMO sonar difference array processing
CN113702978A (en) * 2021-08-04 2021-11-26 中国科学院声学研究所 Submarine pipeline detection positioning method and system based on forward-looking sonar
CN113702978B (en) * 2021-08-04 2023-07-18 中国科学院声学研究所 Submarine pipeline detection positioning method and system based on forward-looking sonar

Also Published As

Publication number Publication date
CN108169732B (en) 2021-08-20

Similar Documents

Publication Publication Date Title
CN112505710B (en) Multi-beam synthetic aperture sonar three-dimensional imaging algorithm
US20090048789A1 (en) Optimized Embedded Ultrasonics Structural Radar System With Piezoelectric Wafer Active Sensor Phased Arrays For In-Situ Wide-Area Damage Detection
CN109765562A (en) A kind of three-dimensional looking forward sound sonar system and method
CN112269164A (en) Weak target positioning method based on interference structure matching processing under deep sea reliable acoustic path
CN106125078B (en) A kind of underwater multidimensional acoustic imaging system and method
CN103245943A (en) Method for MIMO array scanning imagery using chirp signals
CN108169732A (en) A kind of transform domain Beamforming Method based on extension aperture sonar
CN110412587A (en) A kind of lower view synthetic aperture three-D imaging method and system based on deconvolution
CN104062663B (en) A kind of multi-beam seabed subbottom profile probing equipment
CN106872572B (en) The vertical acoustical reflection factor measurement method of ice sheet rough surface
CN108181626A (en) A kind of high-resolution three-dimensional acoustics imaging system
CN101504458B (en) Phase filtering based beam forming method
CN110907938A (en) Near-field rapid downward-looking synthetic aperture three-dimensional imaging method
CN108508446A (en) Fan-shaped transform method based on cold seepage imaging data
CN103926586B (en) A kind of MIMO array depth detecting method using transmitting submatrix
CN103901422A (en) Underwater target echo geometric bright spot structure characteristic extracting method
CN206546434U (en) A kind of multidimensional acoustic imaging system under water
CN108761433B (en) High-resolution imaging method using MIMO sonar difference array processing
JP5497302B2 (en) Synthetic aperture sonar
CN103984007A (en) Optimization design method for time delay parameters of directional seismic waves
CN108845298B (en) Adaptive beam forming method based on clutter mapping
CN105652272A (en) Distance dimension high-resolution imaging method utilizing signal discrete frequency component
CN109557541B (en) Holographic penetration imaging radar polar coordinate data processing method
CN103995262B (en) MIMO sparse array ultrasonic measurement methods and system for fluctuation interface
CN109407102B (en) Two-dimensional underwater environment detection method based on transducer receiving phase

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant