CN113900088A - Long-time coherent accumulation method and system for uniform acceleration maneuvering target - Google Patents

Long-time coherent accumulation method and system for uniform acceleration maneuvering target Download PDF

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CN113900088A
CN113900088A CN202111092763.XA CN202111092763A CN113900088A CN 113900088 A CN113900088 A CN 113900088A CN 202111092763 A CN202111092763 A CN 202111092763A CN 113900088 A CN113900088 A CN 113900088A
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target
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coherent accumulation
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杨杰芳
张云华
秘运鹏
石晓进
李东
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National Space Science Center of CAS
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    • 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
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/02Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
    • G01S13/50Systems of measurement based on relative movement of target
    • G01S13/58Velocity or trajectory determination systems; Sense-of-movement determination systems
    • G01S13/583Velocity or trajectory determination systems; Sense-of-movement determination systems using transmission of continuous unmodulated waves, amplitude-, frequency-, or phase-modulated waves and based upon the Doppler effect resulting from movement of targets
    • G01S13/584Velocity or trajectory determination systems; Sense-of-movement determination systems using transmission of continuous unmodulated waves, amplitude-, frequency-, or phase-modulated waves and based upon the Doppler effect resulting from movement of targets adapted for simultaneous range and velocity measurements
    • 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
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/28Details of pulse systems
    • G01S7/285Receivers
    • G01S7/292Extracting wanted echo-signals
    • G01S7/2923Extracting wanted echo-signals based on data belonging to a number of consecutive radar periods
    • 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
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/41Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section
    • G01S7/415Identification of targets based on measurements of movement associated with the target

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Abstract

The invention belongs to the technical field of radar signal processing, and particularly relates to a long-time coherent accumulation method and a long-time coherent accumulation system for a uniform acceleration maneuvering target, wherein the method comprises the following steps: performing pulse compression processing on the target echo signal to obtain a pulse-compressed signal; performing second-order Keystone conversion on the pulse-compressed signal to obtain a second-order Keystone converted signal; determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation on the signal after the second-order Keystone conversion in the search distance-search speed domain to obtain coherent accumulation results of all targets; and carrying out target detection on the coherent accumulation result, and carrying out motion parameter estimation on the detected target.

Description

Long-time coherent accumulation method and system for uniform acceleration maneuvering target
Technical Field
The invention belongs to the technical field of radar signal processing and radar maneuvering target detection, and particularly relates to a long-time coherent accumulation method and system for a uniform acceleration maneuvering target.
Background
With the continuous development of aerospace technology and the increasingly mature modern stealth technology, how to accurately and effectively realize the detection of weak maneuvering targets becomes a difficult problem in the field of radar signal processing. On the premise of not changing radar hardware and basic parameters as much as possible, long-time coherent accumulation is a technology capable of effectively improving radar weak target detection. Even acceleration motion is a common motion pattern for maneuvering targets. When the maneuvering target in the uniform acceleration motion state is observed by the radar for a long time, the speed of the maneuvering target can cause the first-order range migration of the echo, and the acceleration of the maneuvering target can cause the second-order range migration and Doppler spread of the echo. When the coherent accumulation is carried out on the radar echo of the maneuvering target, the main lobe is widened and the accumulated peak value is reduced, so that the detection performance of the radar on the maneuvering target is influenced. Therefore, range and doppler shifts must be eliminated before radar coherent accumulation detection.
For resolving first order range migration caused by the velocity of a maneuvering target, the Keystone transform and Radon-Fourier transform are typical algorithms. Keystone transformation generally adopts interpolation operation to realize scale transformation of a two-dimensional data plane, so as to effectively correct first-order distance migration (reference [1 ]: R.P. Perry, et al, "SAR imaging of moving targets," IEEE Transactions on Aerospace and Electronic Systems, vol.35, No.1, pp.188-200,1999). Radon-Fourier Transform (reference [2 ]: J.Xu, et al, "Radon-Fourier Transform for Radar Target Detection, I: Generalized Doppler Filter Bank," IEEE Transactions on Aerospace and Electronic Systems, vol.47, No.2, pp.1186-1202,2011) performs coherent accumulation of maneuvering Target energy by two-dimensional joint search of distance and velocity. The two methods can only correct first-order range walk, and when a maneuvering target does uniform acceleration movement and second-order range migration and Doppler walk occur, the coherent accumulation effect is obviously poor.
Aiming at the problems of second-order range migration and Doppler spread of uniform acceleration Maneuvering Target echoes, a Generalized Radon-Fourier Transform (reference [3 ]: J.xu, et al, "Radon Maneuvering Target Motion estimated on Generalized Radon-Fourier Transform," IEEE Transactions on Signal Processing, vol.60, No.12, pp.6190-6201,2012 ") is proposed by the application and the like, is a Generalized definition of the existing Radon-Fourier Transform, and performs coherent accumulation on Maneuvering Target energy through three-dimensional combined search of distance, speed and acceleration. In addition, RFRFT, RLVD, RLCT, etc. algorithms are successively proposed to solve the above problems (reference [4 ]: X.L.Chen, et al, ' Manual Target Detection radio-frame transfer-Based Long-Time coding introduction, ' IEEE Transactions on Signal Processing, vol.62, No.4, pp.939-953,2014, reference [5 ]: X.L.Li, et al, ' human Integration for Manual Target Detection radio-transmission-L's Distribution, ' IEEE Signal Processing Letters, vol.22, No.9, pp.1467-1471,2015, reference [6 ]: X.L.Chen, chemistry, ' parameter of radio-transmission, and [5] ' IEEE 1] noise-sensor, see [5 ]. Microreceiver, volume, see [5 ]. 3, see [6 ]. X.L.Chen, R, RLVD, RLCT, etc.). However, the existing methods jointly search in three dimensions of distance, speed and acceleration, and finally accumulate the energy of the maneuvering target in a three-dimensional or even four-dimensional space, so that target detection needs to be performed in the three-dimensional or even four-dimensional space, which causes higher computational complexity and affects the real-time performance of radar signal processing. The existing method has the problem of high computational complexity.
Disclosure of Invention
In order to overcome the defects in the prior art, the invention provides a long-time coherent accumulation method for a uniform acceleration maneuvering target, and particularly relates to a convenient long-time coherent accumulation method with low calculation complexity.
The invention provides a long-time coherent accumulation method for a uniform acceleration maneuvering target, which comprises the following steps:
the radar adopts a linear frequency modulation signal as a transmitting signal, a radar receiver receives a target echo signal, and pulse compression processing is carried out on the target echo signal to obtain a signal after pulse compression;
performing second-order Keystone conversion on the pulse-compressed signal to obtain a second-order Keystone converted signal;
determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation on the signal after the second-order Keystone conversion in the search distance-search speed domain to obtain a coherent accumulation result;
and carrying out target detection on the coherent accumulation result, and carrying out motion parameter estimation on the detected target.
As one improvement of the above technical solution, the radar uses a chirp signal as a transmission signal, and the radar receiver receives a target echo signal and performs pulse compression processing on the target echo signal to obtain a pulse-compressed signal; the specific implementation process is as follows:
the radar adopts a linear frequency modulation signal as a transmitting signal, and the radar receiver receives a target echo signal sraw(tr,tm):
Figure BDA0003267956260000031
Wherein A isrIs the amplitude of the echo signal; t is trThe time is fast;
Figure BDA0003267956260000032
represents the unit imaginary number; c is the speed of light; exp (·) represents an exponential function based on the natural logarithm e; f. ofcIs the center frequency of the transmitted signal; t ispIs the duration of the transmitted signal; krA frequency modulation rate for transmitting a chirp signal; t is tmIs a slow time, tm=mTr(ii) a Wherein M is 0,1,2,. M; t isrFor the pulse repetition interval, M represents the coherent accumulated total number of pulses;
Rt(tm) For the target and radar at tmInstantaneous distance of time:
Figure BDA0003267956260000033
wherein R is0Is the initial distance of the target relative to the radar; a isrRepresents the acceleration of the target; v. ofrRepresents the radial velocity of the target relative to the radar:
vr=vb+Mamb·vprf (3)
wherein v isbTo search for base-band unambiguous velocity, vb∈[-vprf/2,vprf/2];MambSearching fuzzy speed multiple; v. ofprfλ × PRF/2 is the blur speed; wherein PRF is pulse repetition frequency of radar, and PRF is 1/Tr(ii) a λ is the wavelength of the transmitted signal, λ is c/fc
For target echo signal sraw(tr,tm) Performing pulse compression to obtain a pulse-compressed signal src(tr,tm):
Figure BDA0003267956260000034
Wherein A isrcThe amplitude of the signal after pulse compression; b isrFor transmitting signal bandwidth, Br=KrTp
As one improvement of the above technical solution, the second-order Keystone transform is performed on the pulse-compressed signal to obtain a second-order Keystone-transformed signal; the specific implementation process is as follows:
for the pulse-compressed signal src(tr,tm) Fast edge time trFourier transform is carried out to obtain a fast time frequency-slow time domain signal Srm(fr,tm):
Figure BDA0003267956260000041
Wherein f isrIs a fast time trCorresponding fast time frequency, ArmIs the signal amplitude;
to Srm(fr,tm) T in (1)mThe following variable substitutions were made:
Figure BDA0003267956260000042
wherein, tnA new slow time variable after variable substitution;
after the variable substitution, the signal becomes:
Figure BDA0003267956260000043
to Srm(fr,tn) Fast edge time trPerforming inverse Fourier transform, and making r equal to ctrAnd/2, obtaining a second-order Keystone converted signal ssokt(r,tn):
Figure BDA0003267956260000044
Wherein v isr1=vhb+Mambvprf(ii) a Wherein the content of the first and second substances,
Figure BDA0003267956260000045
vhb∈[-vprf/4,vprf/4]。
as one improvement of the above technical solution, the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter are determined according to the range of the preset search parameter, the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter is traversed, and two-dimensional search and coherent accumulation are performed in the search distance-search speed domain according to the obtained second-order Keystone transformed signal to obtain a coherent accumulation result; the specific implementation process is as follows:
suppose a search distance rscSearching for base band unambiguous velocity vhb_scAnd searching for a fuzzy velocity multiple mamb_sc
Setting a search distance rscHas a search range of [ rmin,rmax]If the corresponding search step is Δ r, the number of search distances is determined
Figure BDA0003267956260000051
Further obtaining:
rsc=nrΔr+rmin (9)
wherein n isr=0,1,2,…,Nr-1,nrNumber of search distance; r isminFor searching for a distance rscMinimum value of (d); r ismaxFor searching for a distance rscMaximum value of (d);
setting search speed vsc
vsc=vhb_sc+mamb_scvprf
It should be noted that v isscCorresponds to vr1Rather than the true velocity v of the targetr
Wherein v ishb_scFor searching the base-band unambiguous velocity, the search range is [ -v ]prf/4,vprf/4]If the corresponding search step is Δ v, the base band unambiguous velocity search number is Nv
Figure BDA0003267956260000052
Further obtaining:
Figure BDA0003267956260000053
mamb_scfor searching fuzzy speed multiple, its search range is [ Mamb_min,Mamb_max]And the corresponding search step length is 1, and then:
mamb_sc=Mamb_min,Mamb_min+1,Mamb_min+2,…,Mamb_max-1,Mamb_max
wherein M isamb_minSearching the minimum value of the fuzzy speed multiple; mamb_maxSearching the maximum value of the fuzzy speed multiple;
according to the set search distance rscAnd a search velocity vscExtracting a signal s after second-order Keystone transformationsokt(r,tn) Signal s insokt(rsc+vsctn,tn) Discrete chirp-Fourier transform is carried out, and then the quadratic term coefficient is estimated to be a according to the peak position of the obtained transform resultr_est
According to ar_estAnd vhb_scConstructing phase compensation equation Hv_a(tn):
Figure BDA0003267956260000054
Equation of phase compensation H to be constructedv_a(tn) Substituting the following Radon-Fourier transform algorithm formula into the search distance-search speed domain (r)sc,vsc) Carrying out phase-coherent accumulation to obtain a phase-coherent accumulation result Rrv(rsc,vsc):
Figure BDA0003267956260000061
Wherein, TCPIThe coherent accumulation time; t isCPI=MTr
As one improvement of the above technical solution, the target detection is performed on the coherent accumulation result, and the motion parameter estimation is performed on the detected target; the specific process comprises the following steps:
coherent accumulation result Rrv(rsc,vsc) Carrying out target detection;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is smaller than a preset threshold value, judging that the target is not detected;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is greater than or equal to a preset threshold value, judging that the target is detected, and performing motion parameter estimation on the detected target;
according to Rrv(rsc,vsc) R corresponding to peak point positionscObtaining the distance R between the target and the radar0_est
According to Rrv(rsc,vsc) V corresponding to peak point positionscCorresponding vhb_scAnd mamb_scCalculating the radial velocity v of the target relative to the radarr_est
vr_est=2vhb_sc+mamb_sc·vprf (13)
According to the pair ssokt(rsc+vsctn,tn) Performing discrete chirp-Fourier transform to obtain the acceleration a of the targetr_est
The invention also provides a long-time coherent accumulation system for the uniform acceleration maneuvering target, which comprises the following components:
the pulse compression module is used for performing pulse compression processing on the echo signal to obtain a pulse-compressed signal;
the second-order Keystone conversion module is used for carrying out second-order Keystone conversion on the signals after pulse compression to obtain second-order Keystone converted signals;
the coherent accumulation module is used for determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation in the search distance-search speed range according to the obtained second-order Keystone converted signal to obtain a coherent accumulation result;
and the target detection module is used for carrying out target detection on the coherent accumulation result and carrying out motion parameter estimation on the detected target.
As an improvement of the above technical solution, the specific implementation process of the pulse compression module is as follows:
the radar adopts a linear frequency modulation signal as a transmitting signal, and the radar receiver receives a target echo signal sraw(tr,tm):
Figure BDA0003267956260000071
Wherein A isrIs the amplitude of the echo signal; t is trThe time is fast;
Figure BDA0003267956260000072
represents the unit imaginary number; c is the speed of light; exp (·) represents an exponential function based on the natural logarithm e; f. ofcIs the center frequency of the transmitted signal; t ispIs the duration of the transmitted signal; krA frequency modulation rate for transmitting a chirp signal; t is tmIs a slow time, tm=mTr(ii) a Wherein M is 0,1,2,. M; t isrFor the pulse repetition interval, M represents the coherent accumulated total number of pulses;
Rt(tm) For the target and radar at tmInstantaneous distance of time:
Figure BDA0003267956260000073
wherein R is0Is the initial distance of the target relative to the radar; a isrRepresents the acceleration of the target; v. ofrRepresents the radial velocity of the target relative to the radar:
vr=vb+Mamb·vprf (16)
wherein v isbTo search for base-band unambiguous velocity, vb∈[-vprf/2,vprf/2];MambSearching fuzzy speed multiple; v. ofprfλ × PRF/2 is the blur speed; wherein PRF is pulse repetition frequency of radar, and PRF is 1/Tr(ii) a λ is the wavelength of the transmitted signal, λ is c/fc
For echo signal sraw(tr,tm) Performing pulse compression to obtain a pulse-compressed signal src(tr,tm):
Figure BDA0003267956260000074
Wherein A isrcThe amplitude of the signal after pulse compression; b isrFor transmitting signal bandwidth, Br=KrTp
As one of the improvements of the above technical solution, a specific implementation process of the second-order Keystone transformation module is as follows:
for the pulse-compressed signal src(tr,tm) Fast edge time trFourier transform is carried out to obtain a fast time frequency-slow time domain signal Srm(fr,tm):
Figure BDA0003267956260000081
Wherein f isrIs a fast time trCorresponding fast time frequency, ArmIs the signal amplitude.
To Srm(fr,tm) T in (1)mThe following variable substitutions were made:
Figure BDA0003267956260000082
wherein, tnA new slow time variable after variable substitution;
after the variable substitution, the signal becomes:
Figure BDA0003267956260000083
to Srm(fr,tn) Fast edge time trPerforming inverse Fourier transform, and making r equal to ctrAnd/2, obtaining a second-order Keystone converted signal ssokt(r,tn):
Figure BDA0003267956260000084
Wherein v isr1=vhb+Mambvprf(ii) a Wherein the content of the first and second substances,
Figure BDA0003267956260000085
vhb∈[-vprf/4,vprf/4]。
as one of the improvements of the above technical solution, the implementation process of the coherent accumulation module is as follows:
suppose a search distance rscSearching for base band unambiguous velocity vhb_scAnd searching for a fuzzy velocity multiple mamb_sc
Setting a search distance rscHas a search range of [ rmin,rmax]If the corresponding search step is Δ r, the number of search distances is determined
Figure BDA0003267956260000086
Further obtaining:
rsc=nrΔr+rmin (22)
wherein n isr=0,1,2,…,Nr-1, the number of search distances; r isminFor searching for a distance rscMinimum value of (d); r ismaxFor searching for a distance rscMaximum value of (d);
setting search speed vsc
vsc=vhb_sc+mamb_scvprf
It should be noted that v isscCorresponds to vr1Rather than the true velocity v of the targetr
Wherein v ishb_scFor searching the base-band unambiguous velocity, the search range is [ -v ]prf/4,vprf/4]If the corresponding search step is Δ v, the base band unambiguous velocity search number is Nv
Figure BDA0003267956260000091
Further obtaining:
Figure BDA0003267956260000092
mamb_scfor searching fuzzy speed multiple, its search range is [ Mamb_min,Mamb_max]And the corresponding search step length is 1, and then:
mamb_sc=Mamb_min,Mamb_min+1,Mamb_min+2,…,Mamb_max-1,Mamb_max
wherein M isamb_minSearching the minimum value of the fuzzy speed multiple; mamb_maxSearching the maximum value of the fuzzy speed multiple;
according to the set search distance rscAnd a search velocity vscExtracting a signal s after second-order Keystone transformationsokt(r,tn) Signal s insokt(rsc+vsctn,tn) Discrete chirp-Fourier transform is carried out, and then the quadratic term coefficient is estimated to be a according to the peak position of the obtained transform resultr_est
According to ar_estAnd vhb_scConstructing phase compensation equation Hv_a(tn):
Figure BDA0003267956260000093
Equation of phase compensation H to be constructedv_a(tn) Substituting the following Radon-Fourier transform algorithm formula into the search distance-search speed domain (r)sc,vsc) Carrying out phase-coherent accumulation to obtain a phase-coherent accumulation result Rrv(rsc,vsc):
Figure BDA0003267956260000094
Wherein, TCPIThe coherent accumulation time; t isCPI=MTr
As an improvement of the above technical solution, the specific implementation process of the target detection module is as follows:
coherent accumulation result Rrv(rsc,vsc) Carrying out target detection;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is smaller than a preset threshold value, judging that the target is not detected;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is greater than or equal to a preset threshold value, judging that the target is detected, and performing motion parameter estimation on the detected target;
according to Rrv(rsc,vsc) R corresponding to peak point positionscObtaining the distance R between the target and the radar0_est
According to Rrv(rsc,vsc) V corresponding to peak point positionscCorresponding vhb_scAnd mamb_scCalculating the radial velocity v of the target relative to the radarr_est
vr_est=2vhb_sc+mamb_sc·vprf (26)
According to the pair ssokt(rsc+vsctn,tn) Performing discrete chirp-Fourier transform to obtain the acceleration a of the targetr_est
Compared with the prior art, the invention has the beneficial effects that:
the method of the invention simultaneously utilizes the amplitude and phase information in the radar echo of the maneuvering target to carry out long-time coherent accumulation, and can effectively improve the signal-to-noise ratio of the radar echo, thereby improving the detection performance of the radar to the target; in addition, the method only carries out two-dimensional search of distance and speed, the target echo energy is accumulated in a two-dimensional distance-speed space, the target detection is also only carried out in the two-dimensional distance-speed space, the calculation complexity is low, the real-time processing of radar signals is facilitated, the method is beneficial to engineering realization, and the method has popularization and application values.
Drawings
FIG. 1 is a flow chart of a long-time coherent accumulation method for a uniform acceleration maneuvering target provided by the invention;
FIG. 2 is a diagram illustrating the result of compression of echo pulses received by a radar;
FIG. 3 is a schematic diagram of coherent accumulation results in a long-time coherent accumulation method for a uniform acceleration maneuvering target provided by the invention;
fig. 4 is a schematic diagram of a result of discrete chirp-Fourier transform of a signal extracted when a search distance and a search speed correspond to a target in the long-time coherent accumulation method for a uniform acceleration maneuvering target provided by the invention;
FIG. 5 is a graph showing the results of prior art Moving Target Detection (MTD);
FIG. 6 is a diagram illustrating the result of a Radon-Fourier transform of the prior art;
FIG. 7 is a diagram illustrating the result of a prior art generalized Radon-Fourier transform.
Detailed Description
The invention will now be further described with reference to the accompanying drawings and examples.
The invention provides a long-time coherent accumulation method and a long-time coherent accumulation system for a uniform acceleration maneuvering target, and particularly relates to a long-time coherent accumulation method and a long-time coherent accumulation system for radar echoes of the uniform acceleration maneuvering target based on second-order Keystone and Radon-Fourier transformation;
the method comprises the following steps: pulse compression is carried out on a radar receiving target echo signal, second-order distance migration is corrected through second-order Keystone transformation, then coherent accumulation of target energy is achieved through distance and speed combined search, and finally target detection and parameter estimation are carried out on coherent accumulation results. The invention solves the problems of range migration and Doppler walk in the echo when the radar observes a uniform acceleration target for a long time, and effectively improves the signal-to-noise ratio of the radar echo, thereby improving the detection performance of the target. In addition, the invention only carries out two-dimensional search of distance and speed, accumulates target echo energy in a two-dimensional distance-speed space, and only needs to carry out target detection in the two-dimensional distance-speed space, so that the calculation complexity is low, the radar signal real-time processing is convenient, the engineering realization is facilitated, and the method has popularization and application values.
As shown in fig. 1, the method specifically includes:
step S1) target echo distance to pulse compression
The radar adopts a linear frequency modulation signal as a transmitting signal, a radar receiver receives a target echo signal, and pulse compression processing is carried out on the target echo signal to obtain a signal after pulse compression;
specifically, the radar adopts a linear frequency modulation signal as a transmitting signal, and the radar receiver receives a target echo signal sraw(tr,tm):
Figure BDA0003267956260000111
Wherein A isrIs the amplitude of the echo signal; t is trThe time is fast;
Figure BDA0003267956260000112
represents the unit imaginary number; c is the speed of light; exp (·) represents an exponential function based on the natural logarithm e; f. ofcTo transmit signalsThe center frequency of (d); t ispIs the duration of the transmitted signal; (ii) a KrA frequency modulation rate for transmitting a chirp signal; t is tmIs a slow time, tm=mTr(ii) a Wherein M is 0,1,2,. M; t isrFor the pulse repetition interval, M represents the coherent accumulated total number of pulses;
Rt(tm) For the target and radar at tmInstantaneous distance of time:
Figure BDA0003267956260000121
wherein R is0Is the initial distance of the target relative to the radar; a isrRepresents the acceleration of the target; v. ofrRepresents the radial velocity of the target relative to the radar:
vr=vb+Mamb·vprf (29)
wherein v isbTo search for base-band unambiguous velocity, vb∈[-vprf/2,vprf/2];MambSearching fuzzy speed multiple; v. ofprfλ × PRF/2 is the blur speed; wherein PRF is pulse repetition frequency of radar, and PRF is 1/Tr;λ=c/fcIs the transmit signal wavelength;
for echo signal sraw(tr,tm) Performing pulse compression processing to obtain a pulse compressed signal:
Figure BDA0003267956260000122
wherein A isrcThe amplitude of the signal after pulse compression; b isrFor transmitting signal bandwidth, Br=KrTp
Step S2) second order Keystone transformation
For the pulse-compressed signal src(tr,tm) Fast edge time trFourier transform is carried out to obtain a fast time frequency-slow time domain signal Srm(fr,tm):
Figure BDA0003267956260000123
Wherein f isrIs a fast time trCorresponding fast time frequency, ArmIs the signal amplitude.
To Srm(fr,tm) T in (1)mThe following variable substitutions were made:
Figure BDA0003267956260000124
wherein, tnA new slow time variable after variable substitution;
after the variable substitution, the signal becomes:
Figure BDA0003267956260000131
to Srm(fr,tn) Fast edge time trPerforming inverse Fourier transform, and making r equal to ctrAnd/2, obtaining a second-order Keystone converted signal ssokt(r,tn):
Figure BDA0003267956260000132
In the above formula, vr1=vhb+Mambvprf(ii) a Wherein the content of the first and second substances,
Figure BDA0003267956260000133
vhb∈[-vprf/4,vprf/4]。
after second-order Keystone conversion, the base band does not blur the speed vhbHas become half of the original.
Step S3) distance-speed two-dimensional search for realizing coherent accumulation
Determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation in a search distance-search speed domain according to the obtained second-order Keystone converted signal to obtain a coherent accumulation result;
specifically, assume that the search distance rscSearching for base band unambiguous velocity vhb_scAnd searching for a fuzzy velocity multiple mamb_sc
Setting a search distance rscHas a search range of [ rmin,rmax]If the corresponding search step is Δ r, the number of search distances is determined
Figure BDA0003267956260000134
Further obtaining:
rsc=nrΔr+rmin (35)
wherein n isr=0,1,2,…,Nr-1,nrNumber of search distance; r isminFor searching for a distance rscMinimum value of (d); r ismaxFor searching for a distance rscMaximum value of (d);
setting search speed vsc
vsc=vhb_sc+mamb_scvprf
It should be noted that v isscCorresponds to vr1Rather than the true velocity v of the targetr
Wherein v ishb_scFor searching the base-band unambiguous velocity, the search range is [ -v ]prf/4,vprf/4]If the corresponding search step is Δ v, the base band unambiguous velocity search number is Nv
Figure BDA0003267956260000141
Further obtaining:
Figure BDA0003267956260000142
mamb_scfor searching fuzzy speed multiple, its search range is [ Mamb_min,Mamb_max]And the corresponding search step length is 1, and then:
mamb_sc=Mamb_min,Mamb_min+1,Mamb_min+2,…,Mamb_max-1,Mamb_max
wherein M isamb_minSearching the minimum value of the fuzzy speed multiple; mamb_maxSearching the maximum value of the fuzzy speed multiple;
according to the set search distance rscAnd a search velocity vscExtracting a signal s after second-order Keystone transformationsokt(r,tn) Signal s insokt(rsc+vsctn,tn) Discrete chirp-Fourier transform is carried out, and then the quadratic term coefficient is estimated to be a according to the peak position of the obtained transform resultr_est
According to ar_estAnd vhb_scConstructing phase compensation equation Hv_a(tn):
Figure BDA0003267956260000143
Equation of phase compensation H to be constructedv_a(tn) Substituted into the following Radon-Fourier transform algorithm formula, in the search distance-search speed domain (r)sc,vsc) Carrying out phase-coherent accumulation to obtain a phase-coherent accumulation result Rrv(rsc,vsc):
Figure BDA0003267956260000144
Wherein, TCPIThe coherent accumulation time; t isCPI=MTr
Step S4) object detection and motion parameter estimation
And carrying out target detection on the coherent accumulation result, and carrying out motion parameter estimation on the detected target.
Specifically, the coherent integration result Rrv(rsc,vsc) Carrying out target detection;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is smaller than a preset threshold value, judging that the target is not detected;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is greater than or equal to a preset threshold value, judging that the target is detected, and performing motion parameter estimation on the detected target;
according to Rrv(rsc,vsc) R corresponding to peak point positionscObtaining the distance R between the target and the radar0_est
According to Rrv(rsc,vsc) V corresponding to peak point positionscCorresponding vhb_scAnd mamb_scCalculating the radial velocity v of the target relative to the radarr_est
vr_est=2vhb_sc+mamb_sc·vprf (39)
According to the pair ssokt(rsc+vsctn,tn) Performing discrete chirp-Fourier transform to obtain the acceleration a of the targetr_est
The invention also provides a long-time coherent accumulation system for the uniform acceleration maneuvering target, which comprises the following components:
the pulse compression module is used for performing pulse compression processing on the echo signal to obtain a pulse-compressed signal;
specifically, the radar adopts a linear frequency modulation signal as a transmitting signal, and the radar receiver receives a target echo signal sraw(tr,tm):
Figure BDA0003267956260000151
Wherein A isrIs the amplitude of the echo signal; t is trThe time is fast;
Figure BDA0003267956260000152
represents the unit imaginary number; c is the speed of light; exp (·) represents an exponential function based on the natural logarithm e; f. ofcIs the center frequency of the transmitted signal; t ispIs the duration of the transmitted signal; krA frequency modulation rate for transmitting a chirp signal; t is tmIs a slow time, tm=mTr(ii) a Wherein M is 0,1,2,. M; t isrFor the pulse repetition interval, M represents the coherent accumulated total number of pulses;
Rt(tm) For the target and radar at tmInstantaneous distance of time:
Figure BDA0003267956260000153
wherein R is0Is the initial distance of the target relative to the radar; a isrRepresents the acceleration of the target; v. ofrRepresents the radial velocity of the target relative to the radar:
vr=vb+Mamb·vprf (42)
wherein v isbTo search for base-band unambiguous velocity, vb∈[-vprf/2,vprf/2];MambSearching fuzzy speed multiple; v. ofprfλ × PRF/2 is the blur speed; wherein PRF is pulse repetition frequency of radar, and PRF is 1/Tr(ii) a λ is the wavelength of the transmitted signal, λ is c/fc
For echo signal sraw(tr,tm) Performing pulse compression processing to obtain a pulse compressed signal:
Figure BDA0003267956260000161
wherein A isrcThe amplitude of the signal after pulse compression; b isrTo launchSignal bandwidth, Br=KrTp
The second-order Keystone conversion module is used for carrying out second-order Keystone conversion on the signals after pulse compression to obtain second-order Keystone converted signals;
for the pulse-compressed signal src(tr,tm) Fast edge time trFourier transform is carried out to obtain a fast time frequency-slow time domain signal Srm(fr,tm):
Figure BDA0003267956260000162
Wherein f isrIs a fast time trCorresponding distance frequency, ArmIs the signal amplitude.
To Srm(fr,tm) T in (1)mThe following variable substitutions were made:
Figure BDA0003267956260000163
wherein, tnA new slow time variable after variable substitution;
after the variable substitution, the signal becomes:
Figure BDA0003267956260000164
to Srm(fr,tn) Fast edge time trPerforming inverse Fourier transform, and making r equal to ctrAnd/2, obtaining a second-order Keystone converted signal ssokt(r,tn):
Figure BDA0003267956260000171
In the above formula, vr1=vhb+Mambvprf(ii) a Wherein the content of the first and second substances,
Figure BDA0003267956260000172
vhb∈[-vprf/4,vprf/4]。
the coherent accumulation module is used for determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation in the search distance-search speed range according to the obtained second-order Keystone converted signal to obtain a coherent accumulation result;
specifically, assume that the search distance rscSearching for base band unambiguous velocity vhb_scAnd searching for a fuzzy velocity multiple mamb_sc
Setting a search distance rscHas a search range of [ rmin,rmax]If the corresponding search step is Δ r, the number of search distances is determined
Figure BDA0003267956260000173
Further obtaining:
rsc=nrΔr+rmin (48)
wherein n isr=0,1,2,…,Nr-1,nrNumber of search distance; r isminFor searching for a distance rscMinimum value of (d); r ismaxFor searching for a distance rscMaximum value of (d);
setting search speed vsc
vsc=vhb_sc+mamb_scvprf
It should be noted that v isscCorresponds to vr1Rather than the true velocity v of the targetr
Wherein v ishb_scFor searching the base-band unambiguous velocity, the search range is [ -v ]prf/4,vprf/4]If the corresponding search step is Δ v, the base band unambiguous velocity search number is Nv
Figure BDA0003267956260000174
Further obtaining:
Figure BDA0003267956260000175
mamb_scfor searching fuzzy speed multiple, its search range is [ Mamb_min,Mamb_max]And the corresponding search step length is 1, and then:
mamb_sc=Mamb_min,Mamb_min+1,Mamb_min+2,…,Mamb_max-1,Mamb_max
wherein M isamb_minSearching the minimum value of the fuzzy speed multiple; mamb_maxSearching the maximum value of the fuzzy speed multiple;
according to the set search distance rscAnd a search velocity vscExtracting a signal s after second-order Keystone transformationsokt(r,tn) Signal s insokt(rsc+vsctn,tn) Discrete chirp-Fourier transform is carried out, and then the quadratic term coefficient is estimated to be a according to the peak position of the obtained transform resultr_est
According to ar_estAnd vhb_scConstructing phase compensation equation Hv_a(tn):
Figure BDA0003267956260000181
Equation of phase compensation H to be constructedv_a(tn) Substituting the following Radon-Fourier transform algorithm formula into the search distance-search speed domain (r)sc,vsc) Carrying out phase-coherent accumulation to obtain a phase-coherent accumulation result Rrv(rsc,vsc):
Figure BDA0003267956260000182
Wherein, TCPIThe coherent accumulation time; t isCPI=MTr
And the target detection module is used for carrying out target detection on the coherent accumulation result and carrying out motion parameter estimation on the detected target.
Specifically, the coherent integration result Rrv(rsc,vsc) Carrying out target detection;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is smaller than a preset threshold value, judging that the target is not detected;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is greater than or equal to a preset threshold value, judging that the target is detected, and performing motion parameter estimation on the detected target;
according to Rrv(rsc,vsc) R corresponding to peak point positionscObtaining the distance R between the target and the radar0_est
According to Rrv(rsc,vsc) V corresponding to peak point positionscCorresponding vhb_scAnd mamb_scCalculating the radial velocity v of the target relative to the radarr_est
vr_est=2vhb_sc+mamb_sc·vprf (52)
According to the pair ssokt(rsc+vsctn,tn) Performing discrete chirp-Fourier transform to obtain the acceleration a of the targetr_est
As shown in fig. 2-7, the method of the present invention combines with simulation tests to verify the long-time coherent accumulation method for radar echoes of a uniform acceleration maneuvering target provided by the present invention.
Center frequency f of signal emitted by radar systemc1.25GHz, transmission signal bandwidth Br40MHz, transmission duration Tp5us, pulse repetition frequency PRF 1000, coherent accumulation pulse number M1000, coherent accumulation time TCPI=1s。Corresponding fuzzy speed v of the systemprf120 m/s. The initial distance of the simulation target relative to the radar is R0100km, radial velocity vr340m/s with a radial acceleration of ar=30m/s2. The target corresponds to a base band unambiguous velocity vb-20M/s, a multiple of the blur speed Mamb=3。
FIG. 2 shows the result of the echo pulse compression received by the radar, the signal-to-noise ratio after the pulse compression is 3dB, and the visible target signal envelope generates range migration. Fig. 3 is a coherent accumulation result of the method, and it can be seen that a target signal is accumulated into a peak, and fig. 4 is a result of discrete chirp-Fourier transform of a signal extracted when the search distance and speed of the method correspond to a target. The distance R of the target can be estimated from the peak point position in FIG. 30_est99.99km, velocity vr_est340 m/s; the target acceleration a can be estimated from the peak position in fig. 4r_est=29.98m/s2
To illustrate the effectiveness of the present method, fig. 5, 6, and 7 show coherent accumulation results of 3 prior art exemplary methods. Fig. 5 and 6 are results of Moving Target Detection (MTD) and Radon-Fourier transform, respectively, and it can be seen that, due to the influence of target echo distance and doppler migration, coherent accumulation performance of conventional Moving Target Detection (MTD) and Radon-Fourier transform algorithms is significantly degraded, and a target accumulation peak cannot appear in both graphs. FIG. 7 shows a generalized Radon-Fourier transform at a search acceleration value of 30m/s2The obtained distance-speed section can see that the target signal is accumulated into a peak with the amplitude equivalent to that of the method, but the calculation amount of the algorithm is obviously higher than that of the method.
Finally, it should be noted that the above embodiments are only used for illustrating the technical solutions of the present invention and are not limited. Although the present invention has been described in detail with reference to the embodiments, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted without departing from the spirit and scope of the invention as defined in the appended claims.

Claims (10)

1. A long-time coherent accumulation method for a uniform acceleration maneuvering target, characterized by comprising:
the radar adopts a linear frequency modulation signal as a transmitting signal, a radar receiver receives a target echo signal, and pulse compression processing is carried out on the echo signal to obtain a signal after pulse compression;
performing second-order Keystone conversion on the pulse-compressed signal to obtain a second-order Keystone converted signal;
determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation on the signal after the second-order Keystone conversion in the search distance-search speed domain to obtain a coherent accumulation result;
and carrying out target detection on the coherent accumulation result, and carrying out motion parameter estimation on the detected target.
2. The long-time coherent accumulation method for the uniform acceleration maneuvering target according to claim 1, characterized in that the radar adopts a chirp signal as a transmission signal, a radar receiver receives a target echo signal, and pulse compression processing is performed on the echo signal to obtain a pulse-compressed signal; the specific implementation process is as follows:
the radar adopts a linear frequency modulation signal as a transmitting signal, and the radar receiver receives a target echo signal sraw(tr,tm):
Figure FDA0003267956250000011
Wherein A isrIs the amplitude of the echo signal; t is trThe time is fast;
Figure FDA0003267956250000012
representing unit imaginary number(ii) a c is the speed of light; exp (·) represents an exponential function based on the natural logarithm e; f. ofcIs the center frequency of the transmitted signal; t ispIs the duration of the transmitted signal; krA frequency modulation rate for transmitting a chirp signal; t is tmIs a slow time, tm=mTr(ii) a Wherein M is 0,1,2,. M; t isrFor the pulse repetition interval, M represents the coherent accumulated total number of pulses;
Rt(tm) For the target and radar at tmInstantaneous distance of time:
Figure FDA0003267956250000013
wherein R is0Is the initial distance of the target relative to the radar; a isrRepresents the acceleration of the target; v. ofrRepresents the radial velocity of the target relative to the radar:
vr=vb+Mamb·vprf (3)
wherein v isbTo search for base-band unambiguous velocity, vb∈[-vprf/2,vprf/2];MambSearching fuzzy speed multiple; v. ofprfλ × PRF/2 is the blur speed; wherein PRF is pulse repetition frequency of radar, and PRF is 1/Tr(ii) a λ is the wavelength of the transmitted signal, λ is c/fc
For target echo signal sraw(tr,tm) Performing pulse compression to obtain a pulse-compressed signal src(tr,tm):
Figure FDA0003267956250000021
Wherein A isrcThe amplitude of the signal after pulse compression; b isrFor transmitting signal bandwidth, Br=KrTp
3. The long-time coherent accumulation method for the uniform acceleration maneuvering target according to claim 1, characterized in that the second-order Keystone transform is performed on the pulse-compressed signal to obtain a second-order Keystone transformed signal; the specific implementation process is as follows:
for the pulse-compressed signal src(tr,tm) Fast edge time trFourier transform is carried out to obtain a fast time frequency-slow time domain signal Srm(fr,tm):
Figure FDA0003267956250000022
Wherein f isrIs a fast time trCorresponding fast time frequency, ArmIs the signal amplitude;
to Srm(fr,tm) T in (1)mThe following variable substitutions were made:
Figure FDA0003267956250000023
wherein, tnA new slow time variable after variable substitution;
after the variable substitution, the signal becomes:
Figure FDA0003267956250000024
to Srm(fr,tn) Fast edge time trPerforming inverse Fourier transform, and making r equal to ctrAnd/2, obtaining a second-order Keystone converted signal ssokt(r,tn):
Figure FDA0003267956250000031
In the above formula, vr1=vhb+Mambvprf(ii) a Wherein the content of the first and second substances,
Figure FDA0003267956250000032
vhb∈[-vprf/4,vprf/4]。
4. the long-time coherent accumulation method for the uniform acceleration maneuvering target according to claim 1, characterized in that the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter are determined according to a preset search parameter range, a combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter is traversed, and two-dimensional search and coherent accumulation are performed in a search distance-search speed domain according to the obtained second-order Keystone converted signal to obtain a coherent accumulation result; the specific implementation process is as follows:
suppose a search distance rscSearching for base band unambiguous velocity vhb_scAnd searching for a fuzzy velocity multiple mamb_sc
Setting a search distance rscHas a search range of [ rmin,rmax]If the corresponding search step is Δ r, the number of search distances is determined
Figure FDA0003267956250000033
Further obtaining:
rsc=nrΔr+rmin (9)
wherein n isr=0,1,2,…,Nr-1 is the number of search distances; r isminFor searching for a distance rscMinimum value of (d); r ismaxFor searching for a distance rscMaximum value of (d);
setting search speed vsc
vsc=vhb_sc+mamb_scvprf
It should be noted that v isscCorresponds to vr1Rather than the true velocity v of the targetr
Wherein v ishb_scFor searching basebandUnambiguous velocity, with a search range of [ -v ]prf/4,vprf/4]If the corresponding search step is Δ v, the base band unambiguous velocity search number is Nv
Figure FDA0003267956250000034
Further obtaining:
Figure FDA0003267956250000035
mamb_scfor searching fuzzy speed multiple, its search range is [ Mamb_min,Mamb_max]And the corresponding search step is 1, and then:
mamb_sc=Mamb_min,Mamb_min+1,Mamb_min+2,…,Mamb_max-1,Mamb_max
wherein M isamb_minSearching the minimum value of the fuzzy speed multiple; mamb_maxSearching the maximum value of the fuzzy speed multiple;
according to the set search distance rscAnd a search velocity vscExtracting a signal s after second-order Keystone transformationsokt(r,tn) Signal s insokt(rsc+vsctn,tn) Discrete chirp-Fourier transform is carried out, and then the quadratic term coefficient is estimated to be a according to the peak position of the obtained transform resultr_est
According to ar_estAnd vhb_scConstructing phase compensation equation Hv_a(tn):
Figure FDA0003267956250000041
Equation of phase compensation H to be constructedv_a(tn) Substituting the following Radon-Fourier transform algorithm formula into the search distance-search speed domain (r)sc,vsc) Carrying out phase-coherent accumulation to obtain a phase-coherent accumulation result Rrv(rsc,vsc):
Figure FDA0003267956250000042
Wherein, TCPIThe coherent accumulation time; t isCPI=MTr
5. The method for accumulating the coherent integration result for the uniform acceleration maneuvering target for the long time according to the claim 1, characterized in that the coherent integration result is subjected to target detection, and the detected target is subjected to motion parameter estimation; the specific process comprises the following steps:
coherent accumulation result Rrv(rsc,vsc) Carrying out target detection;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is smaller than a preset threshold value, judging that the target is not detected;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is greater than or equal to a preset threshold value, judging that the target is detected, and performing motion parameter estimation on the detected target;
according to Rrv(rsc,vsc) R corresponding to peak point positionscObtaining the distance R between the target and the radar0_est
According to Rrv(rsc,vsc) V corresponding to peak point positionscCorresponding vhb_scAnd mamb_scCalculating the radial velocity v of the target relative to the radarr_est
vr_est=2vhb_sc+mamb_sc·vprf (13)
According to the pair ssokt(rsc+vsctn,tn) Performing discrete chirp-Fourier transform to obtain the acceleration a of the targetr_est
6. A long-term coherent accumulation system for a uniform acceleration maneuver target, the system comprising:
the pulse compression module is used for performing pulse compression processing on the echo signal to obtain a pulse compressed signal;
the second-order Keystone conversion module is used for carrying out second-order Keystone conversion on the signals after pulse compression to obtain second-order Keystone converted signals;
the coherent accumulation module is used for determining the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of the search parameter according to the preset search parameter range, traversing the combination of the search distance, the search baseband unambiguous speed and the search ambiguous speed multiple of each search parameter, and performing two-dimensional search and coherent accumulation in the search distance-search speed range according to the obtained second-order Keystone converted signal to obtain a coherent accumulation result;
and the target detection module is used for carrying out target detection on the coherent accumulation result and carrying out motion parameter estimation on the detected target.
7. The long-time coherent accumulation system for the uniform acceleration maneuvering target according to claim 6, characterized in that the pulse compression module is realized by the following specific processes:
the radar adopts a linear frequency modulation signal as a transmitting signal, and the radar receiver receives a target echo signal sraw(tr,tm):
Figure FDA0003267956250000051
Wherein A isrIs the amplitude of the echo signal; t is trThe time is fast;
Figure FDA0003267956250000052
represents the unit imaginary number; c is the speed of light; exp (·) represents an exponential function based on the natural logarithm e; f. ofcIs the center frequency of the transmitted signal; t ispIs the duration of the transmitted signal; krTo transmit linearlyThe frequency modulation rate of the frequency modulated signal; t is tmIs a slow time, tm=mTr(ii) a Wherein M is 0,1,2,. M; t isrFor the pulse repetition interval, M represents the coherent accumulated total number of pulses;
Rt(tm) For the target and radar at tmInstantaneous distance of time:
Figure FDA0003267956250000053
wherein R is0Is the initial distance of the target relative to the radar; a isrRepresents the acceleration of the target; v. ofrRepresents the radial velocity of the target relative to the radar:
vr=vb+Mamb·vprf (16)
wherein v isbTo search for base-band unambiguous velocity, vb∈[-vprf/2,vprf/2];MambSearching fuzzy speed multiple; v. ofprfλ × PRF/2 is the blur speed; wherein PRF is pulse repetition frequency of radar, and PRF is 1/Tr(ii) a λ is the wavelength of the transmitted signal, λ is c/fc
For echo signal sraw(tr,tm) Performing pulse compression to obtain a pulse-compressed signal src(tr,tm):
Figure FDA0003267956250000061
Wherein A isrcThe amplitude of the signal after pulse compression; b isrFor transmitting signal bandwidth, Br=KrTp
8. The long-time coherent accumulation system for the uniform acceleration maneuvering target according to claim 6, characterized in that the second-order Keystone transformation module is realized by the following specific processes:
to pulse pressureReduced signal src(tr,tm) Fast edge time trFourier transform is carried out to obtain a fast time frequency-slow time domain signal Srm(fr,tm):
Figure FDA0003267956250000062
Wherein f isrIs a fast time trCorresponding fast time frequency, ArmIs the signal amplitude;
to Srm(fr,tm) T in (1)mThe following variable substitutions were made:
Figure FDA0003267956250000063
wherein, tnA new slow time variable after variable substitution;
after the variable substitution, the signal becomes:
Figure FDA0003267956250000064
to Srm(fr,tn) Fast edge time trPerforming inverse Fourier transform, and making r equal to ctrAnd/2, obtaining a second-order Keystone converted signal ssokt(r,tn):
Figure FDA0003267956250000071
Wherein v isr1=vhb+Mambvprf(ii) a Wherein the content of the first and second substances,
Figure FDA0003267956250000072
vhb∈[-vprf/4,vprf/4]。
9. the long-time coherent accumulation system for the uniform acceleration maneuvering target according to claim 6, characterized in that the coherent accumulation module is realized by the following specific processes:
suppose a search distance rscSearching for base band unambiguous velocity vhb_scAnd searching for a fuzzy velocity multiple mamb_sc
Setting a search distance rscHas a search range of [ rmin,rmax]If the corresponding search step is Δ r, the number of search distances is determined
Figure FDA0003267956250000073
Further obtaining:
rsc=nrΔr+rmin (22)
wherein n isr=0,1,2,…,Nr-1,nrNumber of search distance; r isminFor searching for a distance rscMinimum value of (d); r ismaxFor searching for a distance rscMaximum value of (d);
setting search speed vsc
vsc=vhb_sc+mamb_scvprf
It should be noted that v isscCorresponds to vr1Rather than the true velocity v of the targetr
Wherein v ishb_scFor searching the base-band unambiguous velocity, the search range is [ -v ]prf/4,vprf/4]If the corresponding search step is Δ v, the base band unambiguous velocity search number is Nv
Figure FDA0003267956250000074
Further obtaining:
Figure FDA0003267956250000075
mamb_scto search for a fuzzy speed multiple, the search thereofIn the range of [ Mamb_min,Mamb_max]And the corresponding search step length is 1, and then:
mamb_sc=Mamb_min,Mamb_min+1,Mamb_min+2,…,Mamb_max-1,Mamb_max
wherein M isamb_minSearching the minimum value of the fuzzy speed multiple; mamb_maxSearching the maximum value of the fuzzy speed multiple;
according to the set search distance rscAnd a search velocity vscExtracting a signal s after second-order Keystone transformationsokt(r,tn) Signal s insokt(rsc+vsctn,tn) Discrete chirp-Fourier transform is carried out, and then the quadratic term coefficient is estimated to be a according to the peak position of the obtained transform resultr_est
According to ar_estAnd vhb_scConstructing phase compensation equation Hv_a(tn):
Figure FDA0003267956250000081
Equation of phase compensation H to be constructedv_a(tn) Substituting the following Radon-Fourier transform algorithm formula into the search distance-search speed domain (r)sc,vsc) Carrying out phase-coherent accumulation to obtain a phase-coherent accumulation result Rrv(rsc,vsc):
Figure FDA0003267956250000082
Wherein, TCPIThe coherent accumulation time; t isCPI=MTr
10. The long-time coherent accumulation system for the uniform acceleration maneuvering target according to claim 6, characterized in that the target detection module is realized by the following specific processes:
coherent accumulation result Rrv(rsc,vsc) Carrying out target detection;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is smaller than a preset threshold value, judging that the target is not detected;
if coherent accumulation results Rrv(rsc,vsc) If the accumulated peak value is greater than or equal to a preset threshold value, judging that the target is detected, and performing motion parameter estimation on the detected target;
according to Rrv(rsc,vsc) R corresponding to peak point positionscObtaining the distance R between the target and the radar0_est
According to Rrv(rsc,vsc) V corresponding to peak point positionscCorresponding vhb_scAnd mamb_scCalculating the radial velocity v of the target relative to the radarr_est
vr_est=2vhb_sc+mamb_sc·vprf (26)
According to the pair ssokt(rsc+vsctn,tn) Performing discrete chirp-Fourier transform to obtain the acceleration a of the targetr_est
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Publication number Priority date Publication date Assignee Title
CN115685169A (en) * 2022-11-09 2023-02-03 哈尔滨工程大学 Underwater sound weak moving target detection method based on broadband keystone transformation

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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