CN109932710A - Distant object speed modification method based on sawtooth LFMCW waveform system velocity radar - Google Patents

Distant object speed modification method based on sawtooth LFMCW waveform system velocity radar Download PDF

Info

Publication number
CN109932710A
CN109932710A CN201810898984.8A CN201810898984A CN109932710A CN 109932710 A CN109932710 A CN 109932710A CN 201810898984 A CN201810898984 A CN 201810898984A CN 109932710 A CN109932710 A CN 109932710A
Authority
CN
China
Prior art keywords
frequency
distant object
lfmcw
sawtooth
modification method
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201810898984.8A
Other languages
Chinese (zh)
Other versions
CN109932710B (en
Inventor
王勋
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.)
Leihua Electronic Technology Research Institute Aviation Industry Corp of China
Original Assignee
Leihua Electronic Technology Research Institute Aviation Industry Corp of China
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 Leihua Electronic Technology Research Institute Aviation Industry Corp of China filed Critical Leihua Electronic Technology Research Institute Aviation Industry Corp of China
Priority to CN201810898984.8A priority Critical patent/CN109932710B/en
Publication of CN109932710A publication Critical patent/CN109932710A/en
Application granted granted Critical
Publication of CN109932710B publication Critical patent/CN109932710B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Abstract

The present invention relates to a kind of distant object speed modification method based on sawtooth LFMCW waveform system velocity radar, the speed modification method includes: fast time dimension FFT measurement target range;Slow time dimension FFT obtains Doppler frequency shift and remote echo frequency displacement;Carrier frequency is corrected to obtain the velocity amplitude of distant object.Modification method of the invention can solve the error occurred when the slow time dimension FFT calculating speed of linear frequency modulation continuous wave radar on distant object and big chirp rate at all, consumption resource is smaller in the signal processing, is easily achieved, and can be widely used in coherent system LFMCW radar.

Description

Distant object speed amendment based on sawtooth LFMCW waveform system velocity radar Method
Technical field
The invention belongs to Radar Signal Processing Technology fields, more particularly to a kind of sawtooth LFMCW waveform system that is based on to test the speed The distant object speed modification method of radar.
Background technique
Linear frequency modulation continuous wave (Linear Frequency Modulated Continuous Wave, LFMCW) radar With very high range resolution and range accuracy, have in terms of low blind range zone than pulse radar more obvious excellent Point.
It is illustrated in fig. 1 shown below as zigzag LFMCW waveform.
LFMCW radar emission signal model may be expressed as:
s1(t)=cos (2 π f0t+πμt2), 0≤t≤Te (1)
In formula, μ=B/Te, μ is LFM slope, and B is modulating bandwidth, TeFor frequency modulation period sweep frequency band time;f0Linearly to adjust The initial frequency (carrier frequency) of frequency pulse.
Assuming that being that the position R has a point scatter in distance, radar receives its echo-signal are as follows:
sr(t)=acos [2 π f0(t-Δτ)+πμ(t-Δτ)2], 0≤t- Δ τ≤Te (2)
In formula, a is signal amplitude, with target radar scattering cross-section product (RadarCrossSection, RCS), distance, Antenna gain is related;Δ τ=2R/c is time delay, and c is the light velocity.
The reference signal of frequency mixer input are as follows:
sref(t)=cos (2 π fr0+πμt2), 0≤t≤Te (3)
In formula, fr0For the initial frequency of reference signal LFM, f is usually enabledr0=f0
Receive signal be mixed with reference signal, the complex signal model after low-pass filtering are as follows:
The instantaneous frequency of the signal are as follows:
Above formula shows that the distance of target is directly proportional to instantaneous frequency.So carrying out sampling and to sampling sequence to signal is received Column carry out FFT, are f in frequencyiThe corresponding target range of peak position be
Practical LFMCW radar is fast time dimension FFT in sweep frequency band, and frequency peak calculates mesh according to above formula (6) Subject distance.Slow time dimension FFT is between each sweep frequency band, frequency peak corresponds to target velocity.
However when being tested the speed using sawtooth LFMCW waveform, distant object causes carrier frequency to change, and then influences whether The calculated result of distant object, therefore it cannot ignore, the velocity amplitude after needing to correct detection, to improve computational accuracy.
Summary of the invention
The object of the present invention is to provide a kind of distant object speed based on sawtooth LFMCW waveform system velocity radar to repair Correction method, when being tested the speed for correcting using sawtooth LFMCW waveform, distant object causes carrier frequency to change, and then will affect To distant object calculated result the problem of.
In order to achieve the above objectives, the technical solution adopted by the present invention is that: one kind is tested the speed thunder based on sawtooth LFMCW waveform system The distant object speed modification method reached, the speed modification method include:
Fast time dimension FFT measures target range;
Slow time dimension FFT obtains Doppler frequency shift and remote echo frequency displacement;
Carrier frequency is corrected to obtain the velocity amplitude of distant object.
Further, the target range are as follows:
In formula: fiFor frequency, c is the light velocity, and μ is LFM slope, μ=B/Te, B is modulating bandwidth, TeFor the frequency modulation period.
Further, revised target speed value is
In formula: fiFor frequency, foFor frequency published originally, c is the light velocity, and μ is LFM slope, μ=B/Te, B is modulating bandwidth, TeTo adjust Frequency period, R0For target range.
Modification method of the invention can solve linear frequency modulation continuous wave on distant object and big chirp rate at all The error occurred when the slow time dimension FFT calculating speed of radar, consumes that resource is smaller, is easily achieved in the signal processing, and It can be widely used in coherent system LFMCW radar.
Detailed description of the invention
The drawings herein are incorporated into the specification and forms part of this specification, and shows and meets implementation of the invention Example, and be used to explain the principle of the present invention together with specification.
Fig. 1 is to emit signal transient frequency and time relationship schematic diagram in the prior art.
Fig. 2 is distant object speed modification method flow chart of the invention.
Fig. 3 is the echo-signal three-dimensional spectrogram obtained according to the simulation parameter in the embodiment of the present invention.
Specific embodiment
To keep the purposes, technical schemes and advantages of the invention implemented clearer, below in conjunction in the embodiment of the present invention Attached drawing, technical solution in the embodiment of the present invention is further described in more detail.
Practical short distance and distant object echo simulation process, each parameter declaration of simulation process, which is given below, see the table below 1:
1 simulated program of table inputs parameter
Parameter description Unit State Simulation parameter
Frequency modulation cycle Te S Input 1e-3
Modulating bandwidth B Hz Input 1e8
Target range R0 m Input [1.1e6,5e3,2.5e4]
Target velocity v m/s Input [23,7,33]
Target signal to noise ratio dB Input [20,15,10]
Carrier frequency fo Hz Input 1e10
Fast time dimension sample rate fs Hz Input 2.5e7
Fast time dimension FFT points N fft2 Input 4096
Slow time dimension FFT points N fft1 Input 64
Simulation result is as shown in Fig. 2, may determine that three target range door simulation results are followed successively by according to echo signal-to-noise ratio [2732,3551,1367], actual distance are [1.1e6,5e3,2.5e4].
First verify that whether emulation is correct: not fuzzy distance Ru, it may be assumed that
Ru=c*Te/2 (9)
Wherein, TeFor the frequency modulation period, c is the light velocity.
Distance R after fuzzy0, it may be assumed that
Wherein, fsFor fast time dimension sample rate, Nfft2 is fast time dimension FFT points.Distance after three object removals are fuzzy Door is [2731.8,3551,1366.2].
It can be seen that range gate simulation result is consistent with calculated result, simulation result is errorless, and emulation data are available.
Three target velocity dimension simulation results are followed successively by [28,31,14], and true velocity is [23,7,33].
Do not obscure speed Vu, it may be assumed that
Wherein, f0For carrier frequency, speed V after obscuring0, it may be assumed that
Wherein, Nfft1 is slow time dimension FFT points.Carrier frequency is according to f0It calculates, is tied after the not fuzzy speed of three object removals Fruit is [35.13,30.86,13.8].It can be seen that short distance (km or so) target, speed is according to carrier frequency f0Calculate, as a result and Simulation value is essentially the same, but remote echo wave speed and simulation value are widely different.
The method of the present invention be exactly given from principle remote echo wave speed and the widely different reason of simulation value and Solution.Slow time dimension echo-signal is chirped in fact it can be seen from formula before, and practical FFT is calculated To frequency be broadband, centre frequency is
Revised carrier frequency is f0', it may be assumed that
Carrier frequency is calculated using above formula, obtain result after the not fuzzy speed of three object removals be [27.4274,30.86, 13.8], it can be seen that and simulation result is almost the same.
By above-mentioned steps as can be seen that the method for the present invention can correct remote echo LFMCW Computational Method of Velocity Measurement due to Carrier frequency changes bring error, there is important application prospect in practical projects.
The method of the present invention can solve linear frequency modulation continuous wave body on distant object and big chirp rate from principle The error occurred when the slow time dimension FFT calculating speed of radar processed, has the advantages that compared with prior art
(1) it is easily achieved in this method engineering, it is smaller that signal processing consumes resource;
(2) the method for the present invention solves bring error when LFMCW waveform tests the speed from principle;
(3) the method for the present invention can be widely used in coherent system LFMCW radar.
The above, optimal specific embodiment only of the invention, but scope of protection of the present invention is not limited thereto, In the technical scope disclosed by the present invention, any changes or substitutions that can be easily thought of by anyone skilled in the art, It should be covered by the protection scope of the present invention.Therefore, protection scope of the present invention should be with the protection model of the claim Subject to enclosing.

Claims (3)

1. the distant object speed modification method based on sawtooth LFMCW waveform system velocity radar, which is characterized in that the speed Spending modification method includes:
Fast time dimension FFT measures target range;
Slow time dimension FFT obtains Doppler frequency shift and remote echo frequency displacement;
Carrier frequency is corrected to obtain the velocity amplitude of distant object.
2. the distant object speed amendment side according to claim 1 based on sawtooth LFMCW waveform system velocity radar Method, which is characterized in that the target range are as follows:
In formula: fiFor frequency, c is the light velocity, and μ is LFM slope, μ=B/Te, B is modulating bandwidth, TeFor the frequency modulation period.
3. the distant object speed amendment side according to claim 2 based on sawtooth LFMCW waveform system velocity radar Method, which is characterized in that revised target speed value is
In formula: fiFor frequency, foFor frequency published originally, c is the light velocity, and μ is LFM slope, μ=B/Te, B is modulating bandwidth, TeFor frequency modulation week Phase, R0For target range.
CN201810898984.8A 2018-08-08 2018-08-08 Long-distance target speed correction method based on sawtooth LFMCW waveform system speed measurement radar Active CN109932710B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810898984.8A CN109932710B (en) 2018-08-08 2018-08-08 Long-distance target speed correction method based on sawtooth LFMCW waveform system speed measurement radar

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810898984.8A CN109932710B (en) 2018-08-08 2018-08-08 Long-distance target speed correction method based on sawtooth LFMCW waveform system speed measurement radar

Publications (2)

Publication Number Publication Date
CN109932710A true CN109932710A (en) 2019-06-25
CN109932710B CN109932710B (en) 2023-03-03

Family

ID=66984467

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810898984.8A Active CN109932710B (en) 2018-08-08 2018-08-08 Long-distance target speed correction method based on sawtooth LFMCW waveform system speed measurement radar

Country Status (1)

Country Link
CN (1) CN109932710B (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080129582A1 (en) * 2006-12-05 2008-06-05 Hung-Tao Hsieh Tracking target method of radar with frequency modulation continuous wave
CN106842166A (en) * 2017-03-31 2017-06-13 东南大学 A kind of solution velocity ambiguity method suitable for LFMCW radar system
WO2017165728A1 (en) * 2016-03-24 2017-09-28 RFNAV, Inc. Low cost 3d sonar, lidar, all weather radar imaging and 3d association method for autonomous vehicle navigation
CN108279403A (en) * 2018-01-04 2018-07-13 电子科技大学 Parallel Implementation method is converted based on the Keystone apart from framing
CN108287335A (en) * 2018-04-19 2018-07-17 广州合智瑞达科技有限公司 A method of ranging and range rate being carried out to multiple target using the frequency modulated signal of LFMCW radars

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080129582A1 (en) * 2006-12-05 2008-06-05 Hung-Tao Hsieh Tracking target method of radar with frequency modulation continuous wave
WO2017165728A1 (en) * 2016-03-24 2017-09-28 RFNAV, Inc. Low cost 3d sonar, lidar, all weather radar imaging and 3d association method for autonomous vehicle navigation
CN106842166A (en) * 2017-03-31 2017-06-13 东南大学 A kind of solution velocity ambiguity method suitable for LFMCW radar system
CN108279403A (en) * 2018-01-04 2018-07-13 电子科技大学 Parallel Implementation method is converted based on the Keystone apart from framing
CN108287335A (en) * 2018-04-19 2018-07-17 广州合智瑞达科技有限公司 A method of ranging and range rate being carried out to multiple target using the frequency modulated signal of LFMCW radars

Also Published As

Publication number Publication date
CN109932710B (en) 2023-03-03

Similar Documents

Publication Publication Date Title
CN106353748B (en) Signal processing apparatus and method for fmcw radar range-measurement system
CN103823215A (en) Linear frequency modulation continuous wave radar distance measuring method
CN107843892B (en) High-speed target Doppler velocity measurement method based on least square method
CN104166126A (en) Echo signal simulation method used for continuous wave radar
CN107907878A (en) The method that high accuracy obtains fmcw radar distance measure
CN107346017B (en) The intensive target simulation method of pulse compression radar based on frequency matching filtering
CN109001697A (en) A kind of multiple target radar echo simulator
US9465063B2 (en) Method and system for the estimation and cancellation of multipath delay of electromagnetic signals, in particular SSR replies
CN110850384B (en) Method for generating broadband deskew echo based on sweep frequency data
US11255956B2 (en) Method for measuring the flow velocity of a medium
CN108490443A (en) Multiple submatrixes synthetic aperture sonar ω k imaging algorithms based on analytic solutions and NUFFT
CN107064924B (en) Self-checking method of hump speed measuring radar
CN105024770B (en) Quantitative testing for sensitivity of a non-coherent FMCW autodyne receiver
Yi et al. Active cancellation analysis based on the radar detection probability
CN116087908A (en) Radar high-precision level meter measuring method based on cooperative operation
CN108445477A (en) The precision distance measurement method of airdrome scene foreign bodies detection radar
Widyantara et al. Analysis of non linear frequency modulation (NLFM) waveforms for pulse compression radar
KR102610917B1 (en) Continuous wave radar and ranging method using the continuous wave radar
US8207888B1 (en) Systems and methods of range tracking
CN113805166A (en) Target tracking and ranging method and system of radar level meter
Chaudhari et al. Frequency estimator to improve short range accuracy in FMCW radar
CN109932710A (en) Distant object speed modification method based on sawtooth LFMCW waveform system velocity radar
RU2486540C1 (en) Simulator of false radar target during linear frequency-modulated signal probing
CN108241144A (en) A kind of fmcw radar waveform modulated method and device
RU186130U1 (en) MULTIFUNCTIONAL RADAR TARGET SIMULATOR

Legal Events

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