This application is based upon and claims the benefit of priority from Japanese Patent Applications No. 2010-134436, filed Jun. 11, 2010; No. 2010-260631, filed Nov. 22, 2010; and No. 2010-260632, filed Nov. 22, 2010; the entire contents of all of which are incorporated herein by reference.
1. Field
Embodiments described herein relate generally to a radar return signal processing apparatus and method, which accurately detect a target signal only from a radar return signal containing both target signal and clutter signal.
2. Background
A weather radar observes precipitation by receiving an echo from a weather target, and analyzing received power. Weather radar exploits the Doppler effect exhibited by an electromagnetic wave to determine wind velocity by analyzing the Doppler frequency of a radar return signal. Similarly, surveillance radar detects an aircraft by receiving and processing an echo from the aircraft.
Radar return signals include clutter consisting of echoes from ground, mountains and sea, in addition to target signals. As clutter interferes with observation, a radar return signal processing apparatus uses a moving target indicator (MTI) to eliminate clutter.
A moving target indicator eliminates a clutter signal by means of a low-pass filter with a preset cutoff frequency, by using the difference between the frequency changes in a target signal and clutter signal. Therefore, signal components lower than the preset cutoff frequency are eliminated without discriminating a target signal from a clutter signal.
For example, in weather radar, when a meteorological echo and clutter have an equivalent frequency change, it is impossible to accurately eliminate the clutter signal only, and it is impossible to accurately observe precipitation and wind velocity.
As described above, in a conventional radar return signal processing apparatus, when a target signal and clutter signal have an equivalent frequency change, it is impossible to accurately discriminate a target signal from the clutter signal, and the target signal may be eliminated.
In general, according to one embodiment, a radar return signal processing apparatus includes an acquisition unit, an estimation unit and an extraction unit. The acquisition unit acquires a frequency spectrum determined by an average Doppler frequency, spectrum width, and received power of each echo group, from a radar return signal obtained repeatedly at regular intervals. The estimation unit estimates an optimum mixed density function by learning modeling a shape of the frequency spectrum by calculating repeatedly a sum of density functions of each of the echoes. The extraction unit extracts information on any one of the echoes included in the radar return signal, from a parameter of the estimated mixed density function.
Hereinafter, embodiments will be explained with reference to the accompanying drawings.
A reflected signal of a radar wave received by the antenna 14 is sent to a receiver 15 through the circulator 13. The receiver 15 amplifies the signal received by the antenna 14, and converts the frequency to a baseband. The output of the receiver 15 is sent to a radar return signal processor 16.
The radar return signal processor 16 digitizes the input radar return signal into by means of an analog-to-digital converter 161, converts the digital data into complex IQ data by means of an IQ detector 162, and obtains observation data based on a meteorological echo by eliminating a terrestrial echo component by means of an observation processor 163.
First, a frequency spectrum is obtained by converting a radar return signal into a frequency domain (step S11). Then, the obtained frequency spectrum is modeled by a mixed density function (step S12). An optimum parameter of the mixed density function is estimated by learning (step S13). An average Doppler frequency, spectrum width, and received power of a target signal are calculated from the estimated parameter, and output as an observation result (step S14).
Prior knowledge may be used for estimating an optimum parameter of a mixed density function corresponding to the frequency spectrum.
In
(Embodiment 1)
In
f1(x|θ1)=(2πθ12)−1/2exp{−(x−θ11)2/(2θ12)} (1)
A Von-Mises distribution f2(x|θ2) expressed by the following equation (2) is used as a distribution for modeling a meteorological echo.
f2(x|θ2)=exp{θ22 cos (x−θ21)}/{2πI0(θ22)} (2)
I0 indicates a 0-order correction Bessel function.
Based on the equations (1) and (2), a mixed density function f(x|θ) for modeling a frequency spectrum is expressed by the following equation (3).
f(x|θ)=τ1f1(x|θ1)+τ2f2(x|θ2) (3)
Then, mixing ratios T1,i and T2 ,i are calculated from the given mixed density function by the following equations (4) and (5) (step S43).
T1,i=τ1f1(xi|θ1)/{f(x|θ)} (4)
T2,i=τ2f2(xi|θ2)/{f(x|θ)} (5)
Next, a prior distribution is determined from previously observed data (step S44). First, a parameter associated with the power of a clutter signal follows a beta distribution p1(τ1) expressed by the following equation (6).
p1(τ1)={τ1α−1(1−τ1)β−1}/B(α,β) (6)
B(α,β) indicates a beta function.
A parameter associated with a Doppler frequency of a clutter signal follows a normal distribution p2(θ11) expressed by the following equation (7).
p2(θ11)=(2πφ2)−1/2exp{−(θ11−φ1)2/(2φ2)} (7)
A parameter associated with a spectrum width of a clutter signal follows a gamma distribution p3(θ12) expressed by the following equation (8).
p3(θ12)=b−θ12a−1exp(−θ12/b)/Γ(a) (8)
Γ(a) indicates a gamma function. Parameters α, β, φ1, φ2, a, b of a prior distribution are determined from the data on a previously observed clutter signal.
Next, Q(θ|θ(t)) is maximized by partially differentiating an expected value of a log likelihood function with a penalty shown in the equation (8) (step S45).
Q(θ|θ(t))=Σni=1[yiT1,i{log τ1f1(θ1|xi)}+yiT2,i{log τ2f2(θ2|xi)}]+S1 log {p1(τ1)}+S2 log {p2(θ11)}+S3 log {p3(θ12)} (9)
The term n indicates the number of samples for Fourier transformation. The term (t) indicates the number of repetitions of steps S43 and S45. The parameters are updated by the following equations.
τ1={Σni=1yiT1,i+S1(α−1)}/{Σni=1yi+S1(α+β−2)} (10)
τ2=1−τ1 (11)
θ11={Σni=1yiT1,ixi+S2(φ1θ12/φ2)}/{Σni=1yiT1,i+S2(θ12/φ2)} (12)
θ12=(1−S3){Σni=1yiT1,i(xi−θ11)2/Σni=1yiT1,i}+S3{−Σni=1yiT1,i+2(a−1)+[{Σni=1yiT1,i−2(a−1)}2+8/bΣni=1yiT1,i(xi−θ11)2]1/2}/{4/b} (13)
θ21=tan−1 {(Σni=1yiT2, i sin xi)/(Σni=1yiT2,i cos xi)} (14)
I1(θ22)/I0(θ22)=Σni=1yiT2,i cos (xi−θ21)/Σni=1yiT2,i (15)
As described above, θ22 can be obtained by solving the equation (15). S1, S2 and S3 take 1 or 0. S1 is 1 when the prior knowledge of the power of a clutter signal is used, and S1 is 0 when it is not used. S2 is 1 when the prior knowledge of a Doppler frequency of a clutter signal is used, and S2 is 0 when it is not used. S3 is 1 when the prior knowledge of a spectrum width of a clutter signal is used, and S3 is 0 when it is not used.
Next, whether the parameters calculated by the above equations are converged is determined (step S46). In this step, when the difference between the parameter for calculating a mixing ratio and the updated parameter is 1/1000 or lower, the parameters are judged as being converged. If the difference is higher, steps S43 and S45 are repeated by using the calculated parameters.
When the parameters are judged as being converged, an average Doppler frequency, spectrum wide, and received power of a meteorological echo are calculated from the parameters of the estimated Von-Muses distribution (step S47). Then, precipitation and wind velocity are calculated from the average Doppler frequency, spectrum wide, and received power of the estimated meteorological echo (step S48).
By the above processing, even if a terrestrial echo caused by ground clutter is overlapped with a meteorological echo as a clutter signal, the components of the meteorological echo and terrestrial echo can be accurately estimated, and precipitation and wind velocity can be accurately estimated from the data.
(Embodiment 2)
In the embodiment 1, a frequency spectrum of a return signal is modeled by the sum of two density functions assuming a meteorological echo and a terrestrial echo (ground clutter). A certain effect can be expected by such processing, but an actual return signal includes clutter components such as noise (clutter echo) other than a terrestrial echo. If a frequency spectrum of such a return signal is modeled by the sum of two density functions assuming a meteorological and a terrestrial echo, an error may occur in estimation of a meteorological echo.
In the embodiment 2, a frequency spectrum of a return signal is modeled by the sum of three density functions including a clutter echo such as noise. The embodiment will be explained by referring again to
In
f1(x|θ1)=(2πθ12)−1/2exp{−(x−θ11)2/(2θ12)} (16)
A Von-Mises distribution f2(x|θ2) expressed by the following equation (17) is used as a distribution for modeling a meteorological echo.
f2(x|θ2)=exp {θ22 cos (x−θ21)}/{2πI0(θ22)} (17)
I0 indicates a 0-order correction Bessel function.
An even distribution f3(x|θ3) expressed by the following equation (18) is used as a distribution for modeling a clutter echo other than the above.
f3(x|θ3)=1/(2Vnyq) (18)
Vnyq indicates a Nyqist rate.
Based on the equations (16), (17) and (18), a mixed density function f(x|θ) for modeling a frequency spectrum is expressed by the following equation (19).
f(x|θ)=τ1f1(x|θ1)+τ2f2(x|θ2)+τ3f3(x|θ3) (19)
Then, mixing ratios T1, I, T2, i and T3, i are calculated from the given mixed density function by the following equations (20), (21) and (22) (step S43).
T1,i=τ1f1(xi|θ1)/{f(xi|θ)} (20)
T2,i=τ2f2(xi|θ2)/{f(xi|θ)} (21)
T3,i=τ3f3(xi|θ3)/{f(xi|θ)} (22)
Next, a prior distribution is determined from previously observed data (step S44). First, a parameter associated with the power of a clutter signal follows a beta distribution p1(τ1) expressed by the following equation.
p1(τ1)={τ1α−1(1−τ1)β−1}/B(α,β) (23)
B(α,β) indicates a beta function.
A parameter associated with a Doppler frequency of a clutter signal follows a normal distribution p2(θ11) expressed by the following equation.
p2(θ11)=(2πφ2)−1/2exp{−(θ11−φ1)2/(2φ2)} (24)
A parameter associated with a spectrum width of a clutter signal follows a gamma distribution p3(θ12) expressed by the following equation.
p3(θ12)=b−aθ12a−1exp(−θ12/b)/Γ(a) (25)
Γ(a) indicates a gamma function. Parameters α, β, φ1, φ2, a, b of a prior distribution are determined from the data on a previously observed clutter signal.
Next, Q(θ|θ(t)) is maximized by partially differentiating an expected value of a log likelihood function with a penalty shown in the equation (25) (step S45).
Q(θ|θ(t))=Σni=1[yiT1,i {log τ1f1(θ1|xi)}+yiT2,i {log τ2f2(θ2|xi)}+yiT3,i {log τ3f3(θ3|xi)}]+S1 log {p1(τ1)}+S2 log {p2(θ11)}+S3 log {p3(θ12)} (26)
The term n indicates the number of samples for Fourier transformation. The term (t) indicates the number of repetitions of steps S43 and S45. The parameters are updated by the following equations.
τ1={Σni=1yiT1,i+S1(α−1)}/{Σni=1yi+S1(α+β−2)} (27)
τ2={Σni=1yiT2,i−S1τ1Σni=1yiT2,i}/{Σni=1yi(T2,i+S1T3,i)} (28)
τ3=1−τ1−τ2 (29)
θ11={Σni=1yiT1,ixi+S2(φ1θ12/φ2)}/{Σni=1yiT1,i+S2(θ12/φ2)} (30)
θ12=(1−S3){Σni=1yiT1,i(xi−θ11)2/Σni=1yiT1,i}+S3{−Σni=1yiT1,i+2(a−1)+[{Σni=1yiT1,i−2(a−1)}2+8/bΣni=1yiT1,i(xi−θ11)2]1/2}/{4/b} (31)
θ21=tan−1 {(Σni=1yiT2,i sin xi)/(Σni=1yiT2,i cos xi)} (32)
I1(θ22)/I0(θ22)=Σni=1yiT2,i cos(xi−θ21)/Σni=1yiT2,i (33)
θ22 can be obtained by solving the equation (33). S1, S2 and S3 take 1 or 0. S1 is 1 when the prior knowledge of the power of a clutter signal is used, and S1 is 0 when it is not used. S2 is 1 when the prior knowledge of the Doppler frequency of a clutter signal, and S2 is 0 when it is not used. S3 is 1 when the prior knowledge of the spectrum width of a clutter signal is used, and S3 is 0 when it is not used.
Next, whether the parameters calculated by the above equations are converged is determined (step S46). In this step, when the difference between the parameter for calculating a mixing ratio and the updated parameter is 1/1000 or lower, the parameters are judged as being converged. If the difference is higher, steps S43 and S45 are repeated by using the calculated parameters.
When the parameters are judged as being converged, an average Doppler frequency, spectrum wide, and received power of a meteorological echo are calculated from the parameters of the estimated Von-Muses distribution (step S47). Then, precipitation and wind velocity are calculated from the average Doppler frequency, spectrum wide, and received power of the estimated meteorological echo (step S48).
By the above processing, even if a terrestrial echo caused by ground clutter is overlapped with a meteorological echo as a clutter signal, the components of the meteorological echo and terrestrial echo can be accurately estimated, and precipitation and wind velocity can be accurately estimated from the data.
A weather radar is assumed in the above embodiment. The embodiment is applicable when a target signal is obtained by eliminating a clutter signal from an ordinary radar unit, or a radar return signal. Further, the embodiment is applicable when using a radar unit, which electronically scans a transmission beam, like an active phased array radar, and a radar unit which forms a plurality of received beams by using digital beam forming technology. Therefore, according to the above embodiment, it is possible to provide a radar return signal processing apparatus, which accurately detects a target signal only from a radar return signal containing both target signal and clutter signal having an equivalent frequency change.
As described above, according to the embodiment, a frequency spectrum determined by an average Doppler frequency, spectrum width, and received power of each echo group is acquired from a radar return signal obtained repeatedly at regular intervals, an optimum mixed density function is estimated by learning modeling a shape of the frequency spectrum by calculating repeatedly a sum of density functions of each of the echoes, and information on any one of the echoes is extracted from a parameter of the mixed density function used for the estimation. As result, according to radar the return signal processing apparatus of the constitution, when a target signal and clutter signal have an equivalent frequency change, it is possible to accurately discriminate a target signal from the clutter signal, and it gets impossible to be removed the target signal.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel embodiments described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the embodiments described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
Number | Date | Country | Kind |
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2010-134436 | Jun 2010 | JP | national |
2010-260631 | Nov 2010 | JP | national |
2010-260632 | Nov 2010 | JP | national |
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