CN102628937B - Radar detection method based on generalized keystone transformation and non-coherent accumulation - Google Patents

Radar detection method based on generalized keystone transformation and non-coherent accumulation Download PDF

Info

Publication number
CN102628937B
CN102628937B CN201210118307.2A CN201210118307A CN102628937B CN 102628937 B CN102628937 B CN 102628937B CN 201210118307 A CN201210118307 A CN 201210118307A CN 102628937 B CN102628937 B CN 102628937B
Authority
CN
China
Prior art keywords
target
velocity
data
echo
pulse
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.)
Expired - Fee Related
Application number
CN201210118307.2A
Other languages
Chinese (zh)
Other versions
CN102628937A (en
Inventor
刘宏伟
戴奉周
赵海刚
曹运合
周生华
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.)
Xidian University
Original Assignee
Xidian 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 Xidian University filed Critical Xidian University
Priority to CN201210118307.2A priority Critical patent/CN102628937B/en
Publication of CN102628937A publication Critical patent/CN102628937A/en
Application granted granted Critical
Publication of CN102628937B publication Critical patent/CN102628937B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Radar Systems Or Details Thereof (AREA)

Abstract

The invention discloses a radar detection method based on generalized keystone transformation and non-coherent accumulation, wherein the method mainly solves the detection problem of a high speed and highly accelerated target in a strong Gaussian white noise background. The method is implemented by the following steps: (1) generating radar target multiple-pulse echoes with Gaussian white noise added, and performing frequency domain pulse compression; (2) correcting range curvature of the pulse-compressed echoes by using the generalized keystone transformation; (3) performing fuzzy compensation on the curvature-corrected echoes by using a fuzzy factor; (4) performing non-coherent accumulation on the fuzzy-compensated echoes, and performing velocity compensation and slow time dimensional quadratic term compensation on the echoes by using a target velocity obtained in the non-coherent accumulation; (5) performing coherent accumulation on the slow time dimensional quadratic term compensated echoes to obtain the target to be detected. The method provided in the invention can eliminate effects of the range curvature and migration of the echoes on energy accumulation, can reduce computation of velocity search, and can be used in the detection of the target in the strong Gaussian white noise background.

Description

Radar detecting method based on General keystone transform and the accumulation of non-coherent
Technical field
The invention belongs to Radar Technology field, relate to object detection method, can be used for efficiently processing based on the detections of radar of coherent pulse echo repeatedly in white Gaussian noise environment.
Background technology
In Radar Targets'Detection field, can run into the situation that target to be detected is high-speed motion, this class target has very high speed and acceleration conventionally, traditional method is that a plurality of pulse echos are directly carried out to slow time dimension FFT, if can there is not range walk when target is low-speed motion, thereby the energy accumulation of each target echo can be got up reach by target detection object out.But because target is high-speed motion, make, at pulse internal object integration time, larger range walk to occur, and the high acceleration of target also can cause the range curvature of echo envelope, if paired pulses echo directly carries out slow time dimension FFT, the energy accumulation of same range unit can only be got up, signal gross energy is dispersed on a plurality of range units, the peak value of gained pulse accumulation result is much lower when there is not range walk and range curvature, thereby can not obtain good testing result, even can lose objects when serious, existing research introduction can be got rid of the range walk of target generation to accumulating the impact of result by keystone method, but for reaching good accumulation result, the range curvature of the echo envelope that the high acceleration while also needing target travel causes is removed the impact of accumulation result, also do not have at present good method to solve.
In the situation that movable information the unknown of target, if obtain the velocity information of target by the method for accumulation, usual method is, first set very large speed search scope and certain speed search step-length, the echo envelope that then can cause according to each search speed of the calculating number of walking about, paired pulses echo carries out envelope ring shift, again the pulse echo of carrying out after envelope ring shift is done to non-coherent accumulation, the result finally each possible search speed being accumulated compares, maximum speed corresponding to accumulation result is the velocity estimation value of target.The result of doing is like this that need to take very high search arithmetic amount be cost, therefore, is necessary to look for a kind of method that reduces operand.
Summary of the invention
The object of the invention is to the deficiency for above-mentioned prior art, a kind of radar detecting method based on General keystone transform and the accumulation of non-coherent is proposed, to reduce the operand of target velocity search, get rid of the impact of high acceleration on target energy accumulation, thereby be conducive to improve radar to the high detection performance of accelerating target of high speed.
For achieving the above object, radar target detection method of the present invention, comprises the steps:
1) approximate model and the noise model of radar high speed high acceleration moving target are expressed as
Figure BDA0000155747130000021
and d (l, t m);
2), according to target approximate model and noise model, obtain radar pulse echo:
And paired pulses echo with the fast time for variable, be FFT and transform to frequency of distance territory, obtain echo apart from frequency domain data z (f, the t of dimension m), wherein f represents frequency of distance;
3) by frequency domain data z (f, the t of distance dimension m) along distance dimension, do frequency domain pulse compression, the data after pulse compression are designated as to z ' (f, t m), and to the data z ' after this pulse compression (f, t m) in slow time variable t mwith new time variable τ mreplace, variable alternate form is
Figure BDA0000155747130000025
the data that variable obtains after replacing are designated as z ' (f, τ m);
4) setting fuzzy factor scope is [n min, n max], n wherein minminimum, n maxmaximum, N altogether, and be all positive integer, data z ' (f, τ after with the fuzzy factor within the scope of this, variable being replaced m) carrying out fuzzy compensation, the echo data after compensation is designated as z ' i(f, τ m), i=1 ... N;
5) to the echo frequency domain data z ' after fuzzy compensation i(f, τ m), i=1 ... N carries out the time domain interpolation that in each range unit, p is ordered, and the data after time domain interpolation are designated as
Figure BDA0000155747130000026
i=1 ... N;
6) utilize the data after time domain interpolation, when calculating target velocity and being v, echo envelope range walk is counted the umber of pulse w in k and same range unit k;
7) according to target friction speed ripple range walk number k and same range unit umber of pulse w next time kdifference, the data after time domain interpolation are carried out to ring shift, and the N group echo data after ring shift are carried out to non-coherent accumulation, obtain N and organize non-coherent accumulation result, be designated as
Figure BDA0000155747130000027
i=1 ... N, wherein || expression be modulo operation;
8) N is organized to non-coherent accumulation result
Figure BDA0000155747130000028
i=1 ... N compares, and gets and wherein accumulates the velocity ambiguity factor of n that the fuzzy factor corresponding to result of peak value maximum is target kestimated value, be designated as
Figure BDA0000155747130000029
and speed corresponding to the accumulation peak value of getting this maximum is fuzzy rear target initial velocity v 0estimated value, be designated as
Figure BDA0000155747130000031
9) initial velocity estimated value after the objective fuzzy that utilization obtains
Figure BDA0000155747130000032
with fuzzy factor estimated value
Figure BDA0000155747130000033
calculate the estimated value of target initial velocity
Figure BDA0000155747130000034
then by the target initial velocity estimated value of estimating to obtain
Figure BDA0000155747130000035
to with fuzzy factor estimated value corresponding echo frequency numeric field data
Figure BDA0000155747130000037
carry out velocity compensation, then the echo data after compensation is transformed to apart from time domain, the distance time domain data after conversion is designated as
Figure BDA0000155747130000038
10) to converting later distance time domain data by the method for Dechirp, carry out the search of frequency modulation rate, obtain frequency modulation rate γ aestimated value, be designated as
Figure BDA00001557471300000310
and then obtained the estimated value of target travel acceleration
Figure BDA00001557471300000311
11) use the estimated value of the aimed acceleration obtaining
Figure BDA00001557471300000312
to the data after velocity compensation
Figure BDA00001557471300000313
carry out the compensation of slow time dimension quadratic phase item, and the data after compensation are done to the coherent accumulation of slow time dimension, the peak value of coherent accumulation is the target of detection.
The present invention, owing to utilizing the method for pulse accumulation to carry out target detection, can effectively suppress noise; Simultaneously owing to utilizing General keystone transform correction target envelope range curvature, make the result of non-coherent accumulation after correction distance bending more approach target echo actual energy; In addition owing to utilizing the method for velocity ambiguity compensation to dwindle the hunting zone of target initial velocity, the non-coherent accumulation operand after General keystone transform is reduced greatly.
Below in conjunction with accompanying drawing, working of an invention is described in detail.
Accompanying drawing explanation
Fig. 1 is the general flow chart of realizing of the present invention;
Fig. 2 is the testing result figure that adopts existing conventional sense method;
Fig. 3 is the testing result figure that adopts existing optimum detection methodology;
Fig. 4 is the testing result figure that adopts the inventive method.
Embodiment
With reference to Fig. 1, specific implementation step of the present invention is as follows:
Step 1, the radar target multiple-pulse echo of generation plus noise.
1a) the approximate model of radar target multiple-pulse echo:
s ( t ^ , t m ) = A 0 rect [ t - 2 R ^ ( t m ) c T p ] exp [ jπγ ( t ^ - 2 R ( t m ) c ) 2 ] exp [ - j 4 π f c R ( t m ) c ] exp ( - j 4 πf c v t ^ c )
In formula, rect ( u ) = 1 | u | ≤ 1 / 2 0 | u | > 1 / 2 , T pbe pulsewidth, γ is frequency modulation rate,
Figure BDA0000155747130000042
be the fast time, t is full-time, and m is integer, T rpulse-recurrence time, f cfor radar emission signal carrier frequency, t m=mT rthe slow time, A 0that scattering point returns wave intensity,
Figure BDA0000155747130000043
t mtarget is to the distance of radar, R constantly 0for target initial time distance, v is target velocity, and a is aimed acceleration, and c is the light velocity;
1b) noise model:
By the noise in continuous N time echo take matrix representation as:
Figure BDA0000155747130000044
wherein, l is range unit label, and u (l) represents the noise power of l range unit, g (l, t m) be the noise phase of l range unit in m pulse, column vector g (l) adds up the independently multiple Gaussian random variable of M dimension zero-mean with u (l), and M represents transponder pulse number, m=1,2 ..., M;
1c) utilize the approximate model of radar target multiple-pulse echo
Figure BDA0000155747130000045
and noise generate the radar target multiple-pulse echo of plus noise: z ( t ^ , t m ) = s ( t ^ , t m ) + d ( t ^ , t m ) .
Step 2, is FFT to the radar target multiple-pulse echo of plus noise along distance dimension.
Because more Range cell migration and range curvature at the direct processing target in Distance Time territory are inconvenient, so paired pulses echo
Figure BDA0000155747130000048
will be with the fast time
Figure BDA0000155747130000049
for variable, be FFT and transform to frequency of distance territory, obtain frequency domain data z (f, t m), what wherein FFT represented is Fast Fourier Transform (FFT), f represents frequency of distance.
Step 3, frequency domain data z (f, the t of paired pulses echo m) carry out pulse compression.
3a) by frequency domain data z (f, the t of following formula paired pulses echo m) do frequency domain pulse compression:
H ( t ^ ) = rect ( t ^ T p ) exp ( - jπγ t ^ 2 )
In formula,
Figure BDA00001557471300000411
indicating impulse compression function, rect ( u ) = 1 | u | ≤ 1 / 2 0 | u | > 1 / 2 ,
Figure BDA00001557471300000413
the fast time, T pbe pulsewidth, γ is frequency modulation rate;
3b) frequency of distance of the pulse echo after pulse compression-slow time domain data are designated as to z ' (f, t m), this packet has contained target echo and noise information, and this example only carries out theoretical analysis to target echo, therefore write out the concrete form of the later target echo signal of pulse pressure, is:
s 1 ( f , t m ) = A ′ rect ( f Δf ) exp ( - j 2 πf ( 2 R 0 c + f d γ ) ) exp ( - j 2 π f d ( f c + f ) f c t m )
· exp ( - j πγ a ( f c + f ) f c t m 2 ) ,
In formula, A ' expression is done the echo strength after frequency pulse pressure to target echo, and Δ f is radar emission signal bandwidth,
Figure BDA0000155747130000053
for the Doppler frequency of target, λ is radar wavelength, and target is to the distance of radar
Figure BDA0000155747130000054
r 0for target initial time distance, v is target velocity, and a is aimed acceleration, t mthe slow time, f cfor radar emission signal carrier frequency, c is the light velocity;
Due to target high-speed motion, make the envelope of target echo signal that the skew being directly proportional to Doppler frequency can occur, the distance of its skew is
Figure BDA0000155747130000055
but the distance of this skew is identical for each echo, therefore do not consider.
Step 4, utilizes General keystone transform correction target echo range curvature.
4a) due to the speed of target, and the repetition frequency of radar transmitted pulse is lower, therefore can cause target generation velocity ambiguity, therefore the Doppler frequency of target is expressed as:
f d=f d0+n kPRF ,
In formula, f d0the later Doppler frequency of velocity ambiguity, n kbe fuzzy factor, PRF is pulse repetition rate;
4b) by the expression of target echo after the expression substitution pulse compression of target Doppler frequency, the new expression of target echo obtaining is:
s 2 ( f , t m ) = A ′ rect ( f Δf ) exp ( - j 2 πf ( 2 R 0 c + f d γ ) ) exp ( - j 2 π f d 0 ( f c + f ) f c t m )
· exp ( - j 2 πn k fPRF f c t m ) exp ( - j 2 πPRF n k t m ) exp ( - j πγ a ( f c + f ) f c t m 2 ) ,
In formula, A ' expression is done the echo strength after frequency pulse pressure to target echo, and Δ f is radar emission signal bandwidth,
Figure BDA0000155747130000058
for the Doppler frequency of target, λ is radar wavelength, and target is to the distance of radar
Figure BDA0000155747130000061
r 0for target initial time distance, v is target velocity, and a is aimed acceleration, γ adoppler frequency rate, t mthe slow time, f cfor radar emission signal carrier frequency, c is the light velocity;
According to the phase place of the 4th exponential term in the new expression of target echo after pulse compression, be 4c) integral multiple of 2 π, its value is 1, therefore after being removed, obtain the reduced representation formula s that target echo is new 3(f, t m) be:
s 3 ( f , t m ) = A ′ rect ( f Δf ) exp ( - j 2 πf ( 2 R 0 c + f d γ ) ) exp ( - j 2 π f d 0 ( f c + f ) f c t m )
· exp ( - j 2 πn k fPRF f c t m ) exp ( - j πγ a ( f c + f ) f c t m 2 ) ;
4c) because target travel acceleration is very large, therefore pulse echo easily produces range curvature, thereby can affect the result that pulse energy accumulates, for eliminating this impact, introduce General keystone transform, i.e. data z ' (f, t after paired pulses compression m) slow time variable t mintroduce variable alternate form pulse echo data after variable is replaced are designated as z ' (f, τ m);
4d) target echo signal s after paired pulses compression 3(f, t m) carry out after General keystone transform the target echo signal s obtaining 4(f, τ m) expression be:
s 4 ( f , t m ) = A ′ rect ( f Δf ) exp ( - j 2 πf ( 2 R 0 c + f d γ ) ) exp ( - j 2 π f d 0 ( f c + f ) f c f c f c + f τ m )
· exp ( - j 2 πn k fPRF f c f c f c + f τ m ) exp ( - j πγ a τ m 2 ) .
Step 5, carries out fuzzy compensation to the echo data after General keystone transform.
5a) paired pulses echo data z ' (f, τ m) in target echo signal expression analyze knownly, its 3rd exponential term is velocity ambiguity item, needs it to compensate in this example;
5b) target setting fuzzy factor n kscope [n min, n max], n wherein minfor minimum fuzzy factor estimated value, n maxfor maximum fuzzy factor estimated value, total N, and be all integer, utilize the fuzzy factor within the scope of this, constructed fuction G (f, τ m; n k) to the data z ' after General keystone transform (f, τ m) utilize following formula to carry out fuzzy compensation:
G ( f , τ m , n k ) = exp ( j 2 πn k f f c f c f + f c PRFτ m ) ,
In formula, G (f, τ m; n k) expression fuzzy compensation function, n krepresent fuzzy factor, τ mbe the slow time after variable changes, f represents frequency of distance, f cfor radar emission signal carrier frequency, PRF is the repetition frequency of radar emission signal, and the pulse echo data after fuzzy compensation are designated as to z ' i(f, τ m), i=1 ... N.
5c) with fuzzy compensation function G (f, τ m; n k) to the target echo signal s obtaining after General keystone transform 4(f, τ m) carry out fuzzy compensation, the target echo signal s after the fuzzy compensation obtaining 5(f, τ m) expression be:
s 5 ( f , τ m ) = A ′ rect ( f Δf ) exp ( - j 2 πf ( 2 R 0 c + f d γ ) ) exp ( - j 2 π f d 0 ( f c + f ) f c f c f c + f τ m )
· exp ( - j πγ a τ m 2 ) .
Step 6, to the pulse echo data z ' after fuzzy compensation i(f, τ m), i=1 ... N carries out apart from time domain interpolation, is about to the data z ' of fuzzy compensation afterpulse echo i(f, τ m), i=1 ... N carries out the time domain interpolation of p point in each range unit, p=1, and 2,3, the data after time domain interpolation are designated as
Figure BDA0000155747130000073
i=1 ... N, time domain Interpolation Theory and method refer to < < radar imagery technology > >.
Step 7, when calculating target velocity is v, the range walk of echo envelope is counted the umber of pulse w in k and same range unit k.
7a) the pulse echo data after General keystone transform are after carrying out velocity ambiguity compensation, and target velocity scope is 0≤v≤v maxtherefore, only need estimate the speed within the scope of this, calculate the fuzzyyest speed of target
Figure BDA0000155747130000074
according to the fuzzyyest speed v obtaining max, calculating target echo envelope range walk number is l=(p+1) * round (2v maxf s/ cPRF) the umber of pulse w and in same range unit l=M/l, wherein PRF represents radar transmitted pulse repetition frequency, and λ represents radar wavelength, and what round represented is the operation that rounds rounding up, f sfor signal sampling frequency;
7b) according to target echo envelope range walk, count the umber of pulse w in l and same range unit l, determine speed search step delta v:
First, get two value l of arbitrary neighborhood within the scope of range walk number 0~l-1 1and l 2, l 1< l 2;
Secondly, calculating generation range walk number is l 1time corresponding target velocity
Figure BDA0000155747130000075
be l with there is range walk number 2time corresponding target velocity v 2 = cl 2 PRF ( p + 1 ) 2 &Delta;fM ;
Then, with there is range walk number, be l 2time corresponding target velocity v 2be l with there is range walk number 1time corresponding target velocity v 1difference as speed search step delta v;
7c) take Δ v as step-length, obtain 0≤v≤v maxall speed v within the scope of this, and the range walk of computing velocity target echo envelope while being v counts k=(p+1) * round (2v/ (cPRF) Δ fM), c represents the light velocity, Δ f represents radar emission signal bandwidth;
While 7d) being v according to speed, the range walk of target echo envelope is counted k, obtains the umber of pulse w in same range unit k=M/k, M indicating impulse number.
Step 8, to the echo data after time domain interpolation
Figure BDA0000155747130000082
i=1 ... N carries out ring shift:
First, take target velocity umber of pulse w in same range unit during as v kfor segment length, M pulse is divided into k group;
Then, the k group data after dividing are carried out to the ring shift of 0~k-1 position successively along distance dimension.
Step 9, carries out non-coherent accumulation to the echo data after ring shift, and soon the mould value in all pulse respective distances unit of the data after N group ring shift is added
Figure BDA0000155747130000083
i=1 ... N, completes the accumulation of non-coherent, and now N organizes non-coherent accumulation result and can occur a peak value at a certain range unit.
Step 10, target velocity is estimated.
10a) will own [n min, n max] N that obtains after fuzzy factor compensation organizes non-coherent accumulation result
Figure BDA0000155747130000084
i=1 ... N compares, and selects fuzzy factor corresponding to the accumulation result of peak value maximum as the estimated value of the fuzzy factor of target
Figure BDA0000155747130000085
and get speed corresponding to this peak-peak as objective fuzzy after the estimated value of speed calculate the estimated value of target initial velocity
Figure BDA0000155747130000087
v ^ = &lambda; ( f d 0 ^ + n k ^ PRF ) 2 ,
In formula,
Figure BDA0000155747130000091
the estimated value that represents the Doppler frequency after target generation velocity ambiguity, λ represents radar wavelength,
Figure BDA0000155747130000092
the estimated value that represents fuzzy factor;
10b) by the estimated value with fuzzy factor
Figure BDA0000155747130000093
the data of corresponding fuzzy compensation afterpulse echo are designated as
Figure BDA0000155747130000094
Step 11, the echo data after fuzzy to General keystone transform compensating for doppler
Figure BDA0000155747130000095
carry out velocity compensation.
11a) after fuzzy to the crooked also compensating for doppler of echo data correction distance, by pulse echo data z ' (f, τ m) in target echo expression can find out, there is linear coupling with the slow time in its second exponential term speed, the impact bringing for eliminating this coupling pulsed energy accumulation, is similar to
Figure BDA0000155747130000096
wherein o () represents that high-order is infinitely small, and desin speed penalty function is:
P ( f , &tau; m ; f ^ d 0 ) = exp ( j &pi;f f c f ^ d 0 &tau; m ) ,
In formula,
Figure BDA0000155747130000098
represent velocity compensation function,
Figure BDA0000155747130000099
represent the just estimated value of Doppler frequency of fuzzy rear target, f represents frequency of distance, τ mit is the slow time after variable is replaced;
11b) use velocity compensation function
Figure BDA00001557471300000910
pulse echo data are fallen in compensation
Figure BDA00001557471300000911
in frequency of distance and the exponential term of doppler velocity coupling, the pulse echo data after velocity compensation are designated as
11c) use velocity compensation function
Figure BDA00001557471300000913
to target echo signal s 5(f, τ m) carry out velocity compensation, obtain the target echo signal s after velocity compensation 6(f, τ m), be expressed as:
s 6 ( f , &tau; m ) = A &prime; rect ( f &Delta;f ) exp ( - j 2 &pi;f ( 2 R 0 c + f d &gamma; ) ) exp ( - j 2 &pi;f d 0 &tau; m ) exp ( - j&pi;&gamma; a &tau; m 2 ) ,
In formula, the echo strength of A ' expression target, Δ f is radar emission signal bandwidth, γ adoppler frequency rate,
Figure BDA00001557471300000915
for the Doppler frequency of target, λ is radar wavelength, f d0represent the Doppler frequency after fuzzy, R 0for target initial time distance, v is target velocity, and a is aimed acceleration, τ mthe slow time after variable is replaced, f cfor radar emission signal carrier frequency, c is the light velocity;
11d) to the pulse echo data after velocity compensation
Figure BDA00001557471300000916
be distance dimension IFFT, convert the signal into apart from time domain, obtain the distance-slow time domain data of pulse echo, be designated as
Figure BDA0000155747130000101
wherein IFFT represents inverse fast Fourier transform;
11e) to the target echo signal s after velocity compensation 6(f, τ m) do the distance-slow time-domain signal of the target echo that distance dimension IFFT obtains
Figure BDA0000155747130000102
be expressed as:
s 7 ( t ^ , &tau; m ) = A &prime; &prime; sin c ( &Delta;f [ t ^ - ( f d &gamma; + 2 R 0 c ) ] ) exp ( - j 2 &pi;f d 0 &tau; m ) exp ( - j&pi;&gamma; a &tau; m 2 ) ,
In formula, A " represents target echo to do the echo strength of target after IFFT.
Step 12, with Dechirp method estimating target motion acceleration.
The specific implementation of this step: the Dechirp method described in list of references < < wide and narrow strip Radar Targets'Detection and imaging technique research > >, to the pulse echo data after velocity compensation
Figure BDA0000155747130000104
carry out the estimation of doppler frequency rate, the estimated value of doppler frequency rate is designated as
Step 13, utilizes the estimated value of doppler frequency rate
Figure BDA0000155747130000106
calculate the estimated value of target travel acceleration
Figure BDA0000155747130000107
a ^ = &lambda; &gamma; a ^ 2 ,
In formula,
Figure BDA0000155747130000109
the estimated value that represents doppler frequency rate, λ represents radar wavelength.
Step 14, compensates the slow time dimension quadratic term of the echo data after velocity compensation.
14a) the distance of the echo signal echo in the pulse echo from velocity compensation-slow time domain expression can find out, also there is quadratic phase item in pulse echo on slow time dimension, for the energy of echo can effectively be accumulated, and the data with following formula after to velocity compensation
Figure BDA00001557471300001011
carry out the compensation of slow time dimension quadratic term:
Q ( &tau; m ; &gamma; ^ a ) = exp ( j&pi; &gamma; ^ a &tau; m 2 ) ,
In formula,
Figure BDA00001557471300001013
the penalty function that represents slow time dimension quadratic phase item, τ mthe slow time after variable is replaced,
Figure BDA00001557471300001014
the estimated value that represents doppler frequency rate;
14b) the pulse echo data after slow time dimension quadratic term compensation are designated as
Figure BDA00001557471300001015
14c) use function
Figure BDA00001557471300001016
to target echo signal
Figure BDA00001557471300001017
carry out the target echo signal obtaining after slow time dimension quadratic term compensation
Figure BDA00001557471300001018
expression be:
s 8 ( t ^ , &tau; m ) = A &prime; &prime; sin c ( &Delta;f [ t ^ - ( f d &gamma; + 2 R 0 c ) ] ) exp ( - j 2 &pi; f d 0 &pi; m )
In formula, A " echo strength that represents target,
Figure BDA0000155747130000111
the fast time, τ mbe the slow time after conversion, Δ f is radar emission signal bandwidth, for the Doppler frequency of target, λ is radar wavelength, f d0represent the Doppler frequency after fuzzy, R 0for target initial time distance, v is target velocity, τ mbe the slow time after variable is replaced, c is the light velocity.
Step 15, the echo data after the compensation of slow time dimension quadratic term is done coherent accumulation.
15a) at paired pulses echo data
Figure BDA0000155747130000113
carry out successively after General keystone transform, velocity ambiguity compensation, velocity compensation and slow time dimension quadratic term compensation, to the pulse echo data that obtain
Figure BDA0000155747130000114
do the accumulation of multiple-pulse coherent, the peak value of coherent accumulation result is the target detecting;
15b) to target echo signal
Figure BDA0000155747130000115
carry out coherent accumulation, the echo signal that obtains detecting
Figure BDA0000155747130000116
expression be:
s 9 ( t ^ , f &tau; ) = A &prime; &prime; sin c ( &Delta;f [ t ^ - ( f d &gamma; + 2 R 0 c ) ] ) sin c ( T ( f &tau; - f d 0 ) ) ,
In formula, A " echo strength that represents target,
Figure BDA0000155747130000118
the fast time, f τwith τ mfor the frequency after variable FFT conversion, FFT represents Fast Fourier Transform (FFT), and γ represents frequency modulation rate, and Δ f is radar emission signal bandwidth, for the Doppler frequency of target, λ is radar wavelength, and T is coherent integration time, f d0represent the Doppler frequency after fuzzy, R 0for target initial time distance, c is the light velocity.
Effect of the present invention further illustrates by following simulation comparison test:
1. experiment scene:
Experimental data comprises with the white Gaussian noise of science software for calculation matlab R2008a emulation generation and the radar return of high speed high acceleration moving target, target number is 1, the initial distance of the relative radar of target is 900 meters, and target radial speed is 3400m/s, and target radial acceleration is 200m/s 2, radar emission carrier frequency is 1GHz, and range resolution is 2 meters, and radar pulse repetition frequency is 500Hz, and a coherent comprises 100 pulses in integration time, and signal to noise ratio (S/N ratio) is-10dB.
2. emulation content:
Utilize experimental data, carry out computer simulation experiment, provide respectively the testing result of conventional sense method, optimum detection methodology and detection method of the present invention as shown in Figure 2, Figure 3, Figure 4, wherein Fig. 2 is for adopting the testing result of conventional sense method, Fig. 3 is for adopting the testing result of optimum detection methodology, and Fig. 4 is for adopting the testing result of the method for the invention.
Conventional sense method refers to that paired pulses echo data is directly slow time dimension FFT, and optimum detection methodology refers to paired pulses echo range curvature and the range walk of pulse echo of having carried out the compensation of General keystone transform, velocity ambiguity and velocity compensation post-equalization, but the slow time dimension FFT of the pulse echo result of not carrying out slow time dimension quadratic term compensation.
3. analysis of simulation result:
As can be seen from Figure 2, while utilizing conventional sense method to detect, because target is high speed high acceleration moving, can cause range walk and the bending of pulse echo, therefore paired pulses echo data cannot accumulate out energy peak after directly adopting slow time dimension FFT, thereby target cannot be detected.
As can be seen from Figure 3, while utilizing optimum detection methodology to detect, although proofreaied and correct range curvature and the range walk of pulse echo, but do not carry out the compensation of slow time dimension quadratic phase item, thereby make target energy on slow time dimension, still disperse by energy accumulation, still target cannot to be detected.
As can be seen from Figure 4, utilize after the method for the invention, be that paired pulses echo data is after General keystone transform, velocity ambiguity compensation, velocity compensation, slow time dimension quadratic term compensation, the peak value of echo envelope has all been corrected to same range unit, thereby to being corrected to when the echoed signal of same range unit is carried out coherent accumulation, target echo energy efficient can be accumulated, thereby target detected.
In sum, when the high acceleration of high speed target is detected, the inventive method is obviously better than conventional sense method and optimum detection methodology.

Claims (8)

1. the radar target detection method based on General keystone transform and the accumulation of non-coherent, comprises the steps:
1) approximate model and the noise model of radar high speed high acceleration moving target are expressed as and d (l, t m), wherein, l is range unit label,
Figure FDA0000430332210000012
represent the fast time, t mrepresent slow time variable;
2), according to target approximate model and noise model, obtain radar pulse echo:
Figure FDA0000430332210000013
and paired pulses echo
Figure FDA0000430332210000014
with the fast time
Figure FDA0000430332210000015
for variable, be FFT and transform to frequency of distance territory, obtain echo apart from frequency domain data z (f, the t of dimension m), wherein f represents frequency of distance;
3) by frequency domain data z (f, the t of distance dimension m) along distance dimension, do frequency domain pulse compression, the data after pulse compression are designated as to z'(f, t m), and to the data z'(f after this pulse compression, t m) in slow time variable t mwith new time variable τ mreplace, variable alternate form is the data that variable obtains after replacing are designated as z'(f, τ m), f wherein cfor radar emission signal carrier frequency;
4) setting fuzzy factor scope is [n min, n max], n wherein minminimum, n maxmaximum, from minimum to maximum, N is individual altogether, and is all positive integer, the data z'(f after with the fuzzy factor within the scope of this, variable being replaced, τ m) carrying out fuzzy compensation, the echo data after compensation is designated as
5) to the echo frequency domain data after fuzzy compensation pass the time domain interpolation that in each range unit of row, p is ordered, p=1,2,3, the data after time domain interpolation are designated as
Figure FDA0000430332210000017
6) utilize the data after time domain interpolation, when calculating target velocity and being v, echo envelope range walk is counted the umber of pulse w in k and same range unit k;
7) according to target friction speed ripple range walk number k and same range unit umber of pulse w next time kdifference, the data after time domain interpolation are carried out to ring shift, and the N group echo data after ring shift are carried out to non-coherent accumulation, obtain N and organize non-coherent accumulation result, be designated as
Figure FDA0000430332210000018
wherein || expression be modulo operation, M indicating impulse number;
8) N is organized to non-coherent accumulation result
Figure FDA0000430332210000021
compare, get and wherein accumulate the velocity ambiguity factor of n that the fuzzy factor corresponding to result of peak value maximum is target kestimated value, be designated as
Figure FDA0000430332210000022
and speed corresponding to the accumulation peak value of getting this maximum is fuzzy rear target initial velocity v 0estimated value, be designated as
Figure FDA0000430332210000023
9) initial velocity estimated value after the objective fuzzy that utilization obtains
Figure FDA0000430332210000024
with fuzzy factor estimated value
Figure FDA0000430332210000025
calculate the estimated value of target initial velocity then by the target initial velocity estimated value of estimating to obtain
Figure FDA0000430332210000027
to with fuzzy factor estimated value
Figure FDA0000430332210000028
corresponding echo frequency numeric field data
Figure FDA00004303322100000219
carry out velocity compensation, then the echo data after compensation is transformed to apart from time domain, the distance time domain data after conversion is designated as
Figure FDA0000430332210000029
10) to converting later distance time domain data
Figure FDA00004303322100000210
by the method for Dechirp, carry out the search of frequency modulation rate, obtain frequency modulation rate γ aestimated value, be designated as
Figure FDA00004303322100000211
and then obtained the estimated value of target travel acceleration
Figure FDA00004303322100000212
11) use the estimated value of the aimed acceleration obtaining
Figure FDA00004303322100000213
to the data after velocity compensation carry out the compensation of slow time dimension quadratic phase item, and the data after compensation are done to the coherent accumulation of slow time dimension, the peak value of coherent accumulation is the target of detection.
2. method according to claim 1, wherein described in step 3) by frequency domain data z (f, the t of distance dimension m) along distance dimension, do frequency domain pulse compression, by following formula, undertaken:
In formula,
Figure FDA00004303322100000216
indicating impulse compression function,
Figure FDA00004303322100000217
the fast time, T pbe pulsewidth, γ is frequency modulation rate.
3. method according to claim 1, wherein step 4) data after described one group of fuzzy factor of use is replaced variable carry out fuzzy compensation, utilize following formula to carry out:
Figure FDA00004303322100000218
In formula, G (f, τ m; n k) expression fuzzy compensation function, n krepresent fuzzy factor, τ mbe the slow time after variable is replaced, f represents frequency of distance, f cfor radar emission signal carrier frequency, PRF is the repetition frequency of radar emission signal.
4. method according to claim 1, the umber of pulse in echo envelope range walk number and same range unit during calculating target velocity and be v described in step 6) wherein, carry out as follows:
6a) calculate the fuzzyyest speed of target
Figure FDA0000430332210000031
according to the fuzzyyest speed v obtaining max, calculating target echo envelope range walk number is l=(p+1) * round (2v maxf s/ cPRF) the umber of pulse w and in same range unit l=M/l, wherein PRF represents radar transmitted pulse repetition frequency, and λ represents radar wavelength, and what round represented is the operation that rounds rounding up, f sfor signal sampling frequency, p=1,2,3, c represents the light velocity, M indicating impulse number;
6b) according to target echo envelope range walk, count the umber of pulse w in l and same range unit l, determine speed search step delta v:
First, get two value l of arbitrary neighborhood within the scope of range walk number 0~l-1 1and l 2, l 1< l 2;
Secondly, calculate target velocity corresponding when range walk number occurring being l1 be l with there is range walk number 2time corresponding target velocity
Figure FDA0000430332210000033
Δ f represents radar emission signal bandwidth;
Then, with there is range walk number, be l 2time corresponding target velocity v 2be l with there is range walk number 1time corresponding target velocity v1 difference as speed search step delta v;
6c) take Δ v as step-length, obtaining target velocity scope is 0≤v≤v maxall speed v within the scope of this, and the range walk of computing velocity target echo envelope while being v counts k=(p+1) * round (2v/ (cPRF) Δ fM), c represents the light velocity, Δ f represents radar emission signal bandwidth;
While 6d) being v according to speed, the range walk of target echo envelope is counted k, obtains the umber of pulse w in same range unit k=M/k, M indicating impulse number.
5. method according to claim 1, wherein described in step 7) according to target at friction speed ripple range walk number and same range unit umber of pulse w next time kdifference, the data after time domain interpolation are carried out to ring shift, be to the N group data after time domain interpolation
Figure FDA0000430332210000034
all proceed as follows:
First, take target velocity umber of pulse w in same range unit during as v kfor segment length, M pulse is divided into k group;
Then, the k group data after dividing are carried out to the ring shift of 0~k-1 position successively along distance dimension.
6. method according to claim 1, calculates the estimated value of target initial velocity in wherein said step 9) and described step 10)
Figure FDA0000430332210000041
with the estimated value of calculating target travel acceleration
Figure FDA0000430332210000042
with following formula, calculate:
In formula,
Figure FDA0000430332210000045
the estimated value of first Doppler frequency after expression target generation velocity ambiguity, λ represents radar wavelength,
Figure FDA0000430332210000046
the estimated value that represents fuzzy factor, the estimated value that represents doppler frequency rate, PRF is the repetition frequency of radar emission signal.
7. method according to claim 1, wherein described in step 9) with estimating that the target initial velocity estimated value pair echo frequency numeric field data corresponding with fuzzy factor estimated value obtaining carry out velocity compensation, utilize following formula to carry out:
Figure FDA0000430332210000048
In formula, represent velocity compensation function, represent the just estimated value of Doppler frequency of fuzzy rear target, f represents frequency of distance, τ mit is the slow time after variable is replaced.
8. according to the method described in right 1, the data of the estimated value of the aimed acceleration that wherein use described in step 11) obtains after to velocity compensation are carried out the compensation of slow time dimension quadratic phase item, utilize following formula to carry out:
Figure FDA00004303322100000411
In formula,
Figure FDA00004303322100000412
the penalty function that represents slow time dimension quadratic phase item, τ mthe slow time after variable is replaced,
Figure FDA00004303322100000413
the estimated value that represents doppler frequency rate.
CN201210118307.2A 2012-04-20 2012-04-20 Radar detection method based on generalized keystone transformation and non-coherent accumulation Expired - Fee Related CN102628937B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201210118307.2A CN102628937B (en) 2012-04-20 2012-04-20 Radar detection method based on generalized keystone transformation and non-coherent accumulation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201210118307.2A CN102628937B (en) 2012-04-20 2012-04-20 Radar detection method based on generalized keystone transformation and non-coherent accumulation

Publications (2)

Publication Number Publication Date
CN102628937A CN102628937A (en) 2012-08-08
CN102628937B true CN102628937B (en) 2014-02-12

Family

ID=46587230

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201210118307.2A Expired - Fee Related CN102628937B (en) 2012-04-20 2012-04-20 Radar detection method based on generalized keystone transformation and non-coherent accumulation

Country Status (1)

Country Link
CN (1) CN102628937B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109085590A (en) * 2018-10-16 2018-12-25 中国人民解放军国防科技大学 Broadband direct acquisition data ISAR imaging method based on ARP (Address resolution protocol) segmented coherent accumulation

Families Citing this family (25)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103323829B (en) * 2013-06-04 2015-09-09 中国人民解放军海军航空工程学院 Based on the radar moving targets long-time phase-coherent accumulation detection method of Radon-fractional order ambiguity function
CN103810325B (en) * 2014-01-08 2016-08-17 西安电子科技大学 The linear thinned array antenna optimization method of low sidelobe based on SQP
CN103760555B (en) * 2014-01-23 2016-05-18 西安电子科技大学 A kind of method that improves airborne radar detection Tracking Integrative precision
CN104076351B (en) * 2014-06-30 2017-02-08 电子科技大学 Phase-coherent accumulation detection method for high-speed high maneuvering target
CN104215959B (en) * 2014-09-22 2017-01-11 西安电子科技大学 Method for estimating radial initial speeds and radial acceleration of multiple maneuvering targets
CN104730498A (en) * 2015-04-01 2015-06-24 西安电子科技大学 Target detection method based on Keystone and weighting rotating FFT
CN106597403B (en) * 2016-11-29 2018-12-11 西安电子工程研究所 A kind of high-speed target phase-coherent accumulation detection method based on segmented compensation
CN106646447B (en) * 2017-01-18 2019-03-26 武汉雷博合创电子科技有限公司 Radar target long time integration detection method based on linear frequency modulation continuous wave
CN106970371B (en) * 2017-04-28 2019-05-14 电子科技大学 A kind of object detection method based on Keystone and matched filtering
CN107356908B (en) * 2017-06-23 2020-07-03 中国电子科技集团公司第二十研究所 Frequency agile signal coherent accumulation method
CN107450055B (en) * 2017-07-15 2020-04-14 西安电子科技大学 High-speed maneuvering target detection method based on discrete linear frequency modulation Fourier transform
CN107561508B (en) * 2017-08-24 2020-12-29 电子科技大学 Coherent accumulation detection method for uniformly accelerated moving target
CN108776332B (en) * 2018-04-24 2021-05-28 国家海洋局第一海洋研究所 Method for detecting marine maneuvering target by using high-frequency ground wave radar
CN108398676B (en) * 2018-05-04 2021-10-26 电子科技大学 External radiation source radar weak moving target detection method
CN108896971B (en) * 2018-05-10 2022-03-22 西安电子科技大学 Simulation method for echoes of small targets floating on sea surface
CN108896976A (en) * 2018-07-05 2018-11-27 电子科技大学 A kind of coherent processing method for multichannel external illuminators-based radar
CN108549064A (en) * 2018-07-24 2018-09-18 电子科技大学 External sort algorithm moving-target detection method based on Doppler frequency fuzzy compensation in arteries and veins
CN109765540B (en) * 2019-02-26 2021-03-19 南京莱斯电子设备有限公司 Frequency stepping system meter wave radar target extraction method
CN112327289A (en) * 2020-10-29 2021-02-05 内蒙古工业大学 Method and device for estimating slope distance and speed of moving target
CN113203998B (en) * 2021-04-23 2022-08-26 上海交通大学 ISAR translation compensation and imaging method, system, medium and device
CN113238191B (en) * 2021-05-10 2022-06-24 电子科技大学 Double-base MIMO radar echo non-coherent accumulation method based on cuckoo search
US12007468B2 (en) 2021-12-10 2024-06-11 Raytheon Company Range-doppler keystone processing for direct sampled radar data from targets with long range and high velocity using waveforms with high bandwidth, high duty factor, and long dwell
CN115453462B (en) * 2022-07-28 2024-07-30 西安电子科技大学 Rapid calculation method for time-frequency difference parameters of radar echo signals of external radiation source
CN115685169B (en) * 2022-11-09 2023-07-14 哈尔滨工程大学 Water sound weak moving target detection method based on broadband keystone transformation
CN116736297B (en) * 2023-08-09 2023-10-10 中国科学院空天信息创新研究院 Heterogeneous multi-frame joint phase-coherent accumulation method

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7450057B2 (en) * 2006-10-20 2008-11-11 Northrop Grumman Space & Missions Systems Corp. Signal processing for accelerating moving targets
US7969345B2 (en) * 2009-04-13 2011-06-28 Raytheon Company Fast implementation of a maximum likelihood algorithm for the estimation of target motion parameters
CN102073043B (en) * 2010-11-04 2013-02-13 电子科技大学 Multi-frame phase coherence accumulation target tracking-before-detecting method
CN102426354A (en) * 2011-09-16 2012-04-25 西安电子科技大学 Broadband radar detection method based on weighted sequence statistics and multiple-pulse coherence accumulation

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109085590A (en) * 2018-10-16 2018-12-25 中国人民解放军国防科技大学 Broadband direct acquisition data ISAR imaging method based on ARP (Address resolution protocol) segmented coherent accumulation

Also Published As

Publication number Publication date
CN102628937A (en) 2012-08-08

Similar Documents

Publication Publication Date Title
CN102628937B (en) Radar detection method based on generalized keystone transformation and non-coherent accumulation
CN106970371B (en) A kind of object detection method based on Keystone and matched filtering
CN104076351B (en) Phase-coherent accumulation detection method for high-speed high maneuvering target
CN102998672B (en) Step frequency inverse synthetic aperture radar (ISAR) imaging method based on coherent processing
CN106872974B (en) High-precision motion target imaging method based on hypersonic platform Two-channels radar
CN107132534B (en) Optimization method for high-speed radar target frequency domain detection
CN109541568B (en) Radar maneuvering target cross-range and Doppler unit fast coherent accumulation detection method
Suo et al. Detection of high‐speed and accelerated target based on the linear frequency modulation radar
CN102590812B (en) SAR (synthetic aperture radar) real-time imaging method based on frequency modulated continuous wave
CN108089171B (en) A kind of radar rapid detection method for unmanned plane target
CN101592733B (en) Parallel real-time imaging processing method for inverse synthetic aperture radar
CN103197317B (en) Synthetic aperture radar (SAR) imaging method based on field programmable gate array (FPGA)
CN109799488B (en) Nonparametric search radar maneuvering target long-time coherent accumulation method
CN106338727A (en) Target detection method of auxiliary vehicle driving radar
CN102749621B (en) Bistatic synthetic aperture radar (BSAR) frequency domain imaging method
CN103399310A (en) Method for detecting radar weak moving target based on PD (Phase Differentiation) RLVD (Radon-Lv Distribution)
CN109581318B (en) Radar high maneuvering target coherent accumulation detection method based on time reversal non-uniform sampling
CN101738606A (en) Method for detecting coherent integration of radar target based on generalized Doppler filter bank
CN111551922B (en) Three-dimensional space double/multi-base radar high-speed target detection method
CN104849708A (en) High-speed maneuvering target parameter estimation method based on frequency domain polynomial phase transformation
CN107843892A (en) A kind of high-speed target Doppler velocity measurement method based on least square method
CN109613507B (en) Detection method for high-order maneuvering target radar echo
CN104502898A (en) Maneuvering target parameter estimation method by combining correction RFT (Radon-Fourier Transform) and MDCFT (Modified Discrete Chirp-Fourier Transform)
CN102778674A (en) Chirp pulse time delay estimation method for non-uniform sampling
CN111007473B (en) High-speed weak target detection method based on distance frequency domain autocorrelation function

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20140212