Gated FMCW DF radar and signal processing for range/doppler/angle determination
First Claim
1. A compact antenna for reception of radar signals, the antenna being part of a radar signal receiving system which includes a receiver and a transmission line, the antenna having an electrical efficiency which is a function of frequency and which causes an external source to contribute an external noise signal during detection of a desired signal, the antenna comprising:
- two magnetic dipoles with each dipole having a phase center, the magnetic dipoles being contained in orthogonal planes and having co-linear phase centers; and
an electric dipole having a phase center, the electric dipole being contained in a plane which is mutually orthogonal to the planes of the magnetic dipoles, the phase center of the electric dipole being co-linear with the phase centers of the magnetic dipoles, wherein the antenna has a desired electrical efficiency which results in the external noise signal being substantially equivalent to but of greater magnitude than an internal noise signal resulting from sources internal to the receiver, transmission line, and antenna.
1 Assignment
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Accused Products
Abstract
A lower-frequency compact radar system for wide-angle surveillance. Direction-finding receive antennas consisting of colocated orthogonal electric and magnetic dipoles provide target angles from the radar. The size of this antenna unit is reduced to the point where internal noise is comparable to external to achieve maximum compactness. High sensitivity is achieved with an efficient class of pulsed/gated, linearly swept-frequency waveforms that are generated and processed digitally. For backscatter radars, close to 50% duty factors are realized. The rules for waveform design and processing overcome problems of range/Doppler aliasing and/or blind zones. After mixing in the receiver, processing bandwidths are much less than RF signal bandwidths, so that simple, inexpensive personal computers are used for real-time signal processing. Digital FFT algorithms determine target range and Doppler, and DF algorithms determine its angles. Frequency hopping can be incorporated in the waveform design by synchronizing all timing and sampling functions, allowing spread-spectrum advantages while still achieving the high sensitivity afforded by coherent processing.
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Citations
26 Claims
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1. A compact antenna for reception of radar signals, the antenna being part of a radar signal receiving system which includes a receiver and a transmission line, the antenna having an electrical efficiency which is a function of frequency and which causes an external source to contribute an external noise signal during detection of a desired signal, the antenna comprising:
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two magnetic dipoles with each dipole having a phase center, the magnetic dipoles being contained in orthogonal planes and having co-linear phase centers; and an electric dipole having a phase center, the electric dipole being contained in a plane which is mutually orthogonal to the planes of the magnetic dipoles, the phase center of the electric dipole being co-linear with the phase centers of the magnetic dipoles, wherein the antenna has a desired electrical efficiency which results in the external noise signal being substantially equivalent to but of greater magnitude than an internal noise signal resulting from sources internal to the receiver, transmission line, and antenna. - View Dependent Claims (2, 3, 4, 5, 6)
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7. A method for determining the azimuth angle to an object, the method comprising:
receiving a vertically polarized signal from the object by means of a compact radar antenna, the antenna being part of a radar signal receiving system which includes a receiver and a transmission line, the antenna having an electrical efficiency which is a function of frequency and which causes an external source to contribute an external noise signal during detection of a desired signal, wherein the antenna comprises; two magnetic dipoles with each dipole having a phase center, the magnetic dipoles being contained in orthogonal planes and having co-linear phase centers; an electric dipole having a phase center, the electric dipole being contained in a plane which is mutually orthogonal to the planes of the magnetic dipoles, the phase center of the electric dipole being co-linear with the phase centers of the magnetic dipoles, wherein the antenna has a desired electrical efficiency which results in the external noise signal being substantially equivalent to but of greater magnitude than an internal noise signal resulting from sources internal to the receiver, transmission line, and antenna; and
processing the received signal to determine the azimuth angle.- View Dependent Claims (8, 9)
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10. A method for determining the azimuth and elevation angles to an object, the method comprising:
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receiving an arbitrarily polarized signal from the object by means of a compact radar antenna, the antenna being part of a radar signal receiving system which includes a receiver and a transmission line, the antenna having an electrical efficiency which is a function of frequency and which causes an external source to contribute an external noise signal during detection of a desired signal, wherein the antenna comprises; three magnetic dipoles with each dipole having a phase center, the magnetic dipoles being contained in orthogonal planes and including two orthogonal horizontal magnetic dipoles and one mutually orthogonal vertical magnetic dipole; and an electric dipole having a phase center, wherein the phase centers of the magnetic dipoles and the phase center of the electric dipole are co-located, and further, wherein the antenna has a desired electrical efficiency which results in the external noise signal being substantially equivalent to but of greater magnitude than an internal noise signal resulting from sources internal to the receiver, transmission line, and antenna; and processing the received signal to determine the azimuth and elevation angles. - View Dependent Claims (11, 12)
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13. A method of generating a radar waveform and processing a received radar signal which is the result of the waveform being reflected by an object to obtain direction, range, and doppler or radial velocity data for the object, the method comprising:
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(1) generating a waveform having a substantially linear increase in frequency during a sweep repetition time interval, the waveform having a sweep width or increase in frequency dependent upon a desired range resolution, wherein the waveform is repeated during each subsequent sweep repetition time interval, the sweep repetition interval being equal to the reciprocal of a sweep repetition frequency; (2) transmitting the waveform by an antenna which is connected to a transmitter operating in a pulsed mode, wherein the pulse period is less than the sweep repetition interval, and further, wherein the transmitter is operated so that it has a duty factor of up to fifty percent; (3) receiving the reflected waveform with an antenna which is connected to a receiver, the receiver being gated so that it is turned off during the transmission of the waveform by the transmitter; (4) mixing the received waveform with the waveform generated in (1), thereby producing a baseband radar echo signal having a center near zero frequency, the radar echo having an offset from zero frequency which depends on a range to the object and the object'"'"'s radial velocity; (5) sampling the mixed waveform at a sampling rate which is less than a signal bandwidth corresponding to a desired target range resolution, wherein the sampling rate is higher than two times a bandwidth of a modulation of the mixed waveform corresponding to data which is the target signal information; and (6) processing the sampled waveform to obtain range, doppler, and directional information for the object. - View Dependent Claims (14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26)
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17. The method of claim 13, wherein the pulsing of the transmitter and gating of the receiver are performed in a manner so that a first spectral sideband at the pulse repetition frequency is greater in magnitude than a baseband information signal of all possible received object signals, thereby providing a method of generating a radar waveform and processing a received radar signal which significantly reduces range aliasing.
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18. The method of claim 13 wherein the processing of the sampled waveform further comprises:
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sampling the previously sampled waveform to produce a time series of data, the sampling being performed at a sampling rate equal to M times the pulse repetition frequency, wherein M is a power of two; segmenting the time series into M separate sub-series, wherein each sub-series has a length substantially equal to 1/M of the unsegmented time series, and further wherein, each sub-series consists of every M-th consecutive point of the unsegmented time series; performing a first Fast-Fourier-Transform on each of the M separate sub-series to obtain the range of the object; performing a second Fast-Fourier-Transform on the data obtained from performing the first Fast-Fourier-Transform on each of the M separate sub-series to obtain the doppler or radial velocity of the target; and recombining the data obtained from performing the second Fast-Fourier-Transform on each of the M separate sub-series into a single series, thereby significantly reducing range or doppler aliasing when the pulsing of the transmitter and gating of the receiver cannot be repeated at a rate so that a first spectral sideband at the pulse repetition frequency is greater in magnitude than a baseband information signal of all possible received object signals.
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19. The method of claim 13, wherein the receiving antenna further comprises:
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two magnetic dipoles with each dipole having a phase center, the magnetic dipoles being contained in orthogonal planes and having co-linear phase centers; and an electric dipole having a phase center, the electric dipole being contained in a plane which is mutually orthogonal to the planes of the magnetic dipoles, the phase center of the electric dipole being co-linear with the phase centers of the magnetic dipoles, wherein the antenna has a desired electrical efficiency which results in an external noise signal being substantially equivalent to but of greater magnitude than an internal noise signal.
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20. The method of claim 19, wherein the desired efficiency of the antenna is achieved by having:
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space="preserve" listing-type="equation">F.sub.E <
F.sub.A,where FE is the amount by which internal noise falls below external noise at the frequency corresponding to the received radar signal and FA is proportional to the antenna efficiency, where ##EQU9## where, RR is a radiation resistance of the antenna, RL is a remaining resistance of the antenna, transmission line and/or load, and XL is a remaining reactance of the antenna and/or load.
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21. The method of claim 13, wherein the receiving antenna further comprises:
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three magnetic dipoles with each dipole having a phase center, the magnetic dipoles being contained in orthogonal planes and including two orthogonal horizontal magnetic dipoles and one mutually orthogonal vertical magnetic dipole; and an electric dipole having a phase center, wherein the phase centers of the magnetic dipoles and the phase center of the electric dipole are co-located, and further, wherein the antenna has a desired electrical efficiency which results in the external noise signal being substantially equivalent to but of greater magnitude than an internal noise signal.
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22. The method of claim 21, wherein the desired efficiency of the antenna is achieved by having:
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space="preserve" listing-type="equation">F.sub.E <
F.sub.A,where FE is the amount by which internal noise falls below external noise at the frequency corresponding to the received radar signal and FA is proportional to the antenna efficiency, where ##EQU10## where, RR is a radiation resistance of the antenna, RL is a remaining resistance of the antenna, transmission line and/or load, and XL is a remaining reactance of the antenna and/or load.
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23. The method of claim 19, wherein the processing of the sampled waveform to obtain the directional information to the object further comprises:
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(1) measuring the voltages produced on each of the magnetic and electric dipoles upon reception of a vertically polarized signal; (2) representing the voltage measured on one of the magnetic dipoles as S cos Φ
, the voltage measured on the second magnetic dipole as S sin Φ and
the voltage measured on the electric dipole as S, where S is the complex amplitude of the received signal; and(3) using the voltages measured on the two magnetic dipoles and the electric dipole to solve for Φ
, where Φ
represents the azimuth angle.
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24. The method of claim 21, wherein the processing of the sampled waveform to obtain the directional information to the object further comprises:
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(1) measuring the voltages produced on each of the magnetic and electric dipoles upon reception of an arbitrarily polarized signal; (2) representing the voltage measured on the vertical magnetic dipole as Fh cos μ
, the voltage measured on the electric dipole as Fv cos μ
, the voltage measured on one of the horizontal magnetic dipoles as Fv cos Φ
+Fh sin μ
sin Φ and
the voltage measured on the other horizontal magnetic dipole as-Fv sin Φ
+Fh sin μ
cos Φ
, where Fv is the field strength of the vertically polarized component of the received signal and Fh is the field strength of the horizontally polarized component of the received signal; and(3) using the voltages measured on the three magnetic dipoles and the electric dipole to solve for Φ and
μ
, where Φ
represents the azimuth angle and μ
represents the elevation angle.
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25. The method of claim 13, wherein the generated waveform further comprises:
a substantially linear decrease in frequency during the sweep repetition time interval, the linear decrease being performed consecutive to the linear increase in frequency, wherein the linear increase and decrease in frequency have the same sweep width.
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26. The method of claim 25, wherein the processing of the sampled waveform further comprises:
performing a Fast-Fourier-Transform on the sampled data to obtain the range and doppler or radial velocity of the object.
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Specification