Radio direction-finding using time of arrival measurements

• US 4,797,679 A
• Filed: 06/09/1987
• Issued: 01/10/1989
• Est. Priority Date: 06/10/1986
• Status: Expired due to Fees

• Current Assignee: Thorn EMI Electronics Limited (Universal Music Group NV)
• Original Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Inventors: Mallinson, Peter, Cusdin, Anthony R., Dadds, Alan F.
• Primary Examiner(s): Blum, Theodore M.
• Application Number:
  US07/059,730
• Time in Patent Office: 581 Days
• Field of Search: 342/424, 342/442, 342/375, 342/446, 342/387, 342/388, 342/389, 342/394
• US Class Current: 342/387
• CPC Class Codes: G01S 3/50 the waves arriving at the antennas being pulse modulated and the time difference of their arrival being measured
• CPC Class Codes: G04F 10/00 Apparatus for measuring unknown time intervals by electric means

Abstract

A method and a system for radio direction-finding by measuring the Time of Arrival (ToA) of the leading edge of signals from a distant source at two relatively closely spaced receiving elements. In order to give a good degree of immunity to multipath, the times at which the instantaneous detected amplitudes of the received signals first exceed a minimal threshold value such that received signals can be satisfactorily distinguished from noise is measured in such a manner that the measured time is not affected by multipath which involves more than a few meters additional path length for the indirect, delayed signal. A suitable timing circuit is disclosed.

By making ToA measurements on three coplanar, non-collinear receivers, directions of incidence in three dimensions can be determined.

A method and a system using both ToA and phase-difference measurements can provide the accuracy of interferometry but be simpler and cheaper.

Claims

1. A method of determining the direction of incidence of electromagnetic wave signals from a distant source from the time of arrival of the leading edge of the wave signals, wherein the method comprises:

receiving said signals at a plurality of mutually spaced wave-receiving elements,

detecting the respective instantaneous amplitude of the signal received at each element,

measuring the times at which the detected amplitudes of wave signals received respectively at at least two of said elements first exceed a minimal threshold value such that signals can be satisfactorily distinguished from noise and which is substantially less than the minimum peak value of signals whose direction of incidence is to be determined by said method, the time being measured in such a manner that the measured time is generally unaffected by multipath propagation,

determining the difference between the measured times in respect of one pair or of a plurality of pairs of said elements, wherein the two elements of said one pair or of each of at least two of said plurality of pairs are sufficiently close together that the length of the interval of time within which signals from the same source must arrive at the two elements is so short that there is a high probability in operation that no signals from another source will arrive in that interval, and

deriving a representation of the direction of incidence from the time difference(s) utilising the relationship

space="preserve" listing-type="equation">cos α

=cδ

t/d

where α

is the angle between the direction of incidence of the signals and the line joining the two elements of a said pair, d is the distance between those two elements, δ

t is the time difference in respect of that pair of elements, and c is the free-space velocity of electromagnetic waves.

2. A method as claimed in claim 1 using three substantially coplanar but substantially non-collinear elements to form at least two said pairs, the method comprising deriving a representation of the angle θ

and/or a representation of the angle β

utilising the relationship

space="preserve" listing-type="equation">sin (90-α

)=sin θ

cos β

in respect of each of said at least two pairs, wherein θ

is the angle between the direction of incidence projected into the plane of the three elements and the normal in said plane to the line joining the two elements of a said pair, and β

is the angle between the direction of incidence and said plane.

3. A method as claimed in claim 1 which further comprises determining a parameter representative of the rate of increase of the detected amplitude of the respective signal received at at least one of the elements in the region of said threshold value, and determining the direction of incidence of received signals only if said parameter satifies a criterion representing a minimum rate of increase in said region.

4. A method as claimed in claim 3 which comprises measuring the time at which the detected amplitude first exceeds an adjacent further threshold value, wherein said parameter is the difference between the measured times in respect of the two threshold values, and wherein said criterion is that said parameter does not exceed a maximum value.

5. A method as claimed in claim 3 which comprises differentiating the increasing detected amplitude at least in said region, wherein said parameter is the rate of increase in detected amplitude derived by differentiation, and wherein said criterion is that said parameter exceeds a minimum value.

6. A method of determining the direction of incidence of electromagnetic wave signals from a distant source, the method comprising:

receiving said signals at each of a plurality of mutually spaced wave-receiving elements,

measuring the phase difference between the signals received respectively at the two elements of one pair of said elements or the respective phase differences between the signals received respectively at the two elements of each of a plurality of substantially collinear pairs of said elements with different respective spacings, wherein the phase measurement on said one pair or on the closest-spaced of said pairs is ambiguous in the operating range of directions o incidence and the operating frequency range,

determining by a method as claimed in claim 1 the appropriate direction of incidence of said signals from the times of arrival of the leading edges of corresponding wave signals received respectively at two of said plurality of elements the line joining said two elements is parallel to and substantially coincident with the line joining said one pair or said plurality of substantially collinear pairs, wherein the range of possible values of the actual time difference due to the uncertainty in the difference between the measured times corresponds to a range of angles of incidence whose magnitude is not greater than the magnitude of the range of angles of incidence corresponding to the unambiguous range of phase difference measurement on said one pair or said closest-spaced pair, and

resolving the ambiguity in said ambiguous phase measurement by comparing the possible directions represented thereby with the approximate direction determined from the difference between the measured times.

13. A system for determining the direction of incidence of electromagnetic wave signals from a distant source, comprising:

a plurality of mutually spaced wave-receiving elements,

means for measuring the phase difference between the signals received respectively at the two elements of one pair of said elements or the respective phase differences between the signals received respectively at the two elements of each of a plurality of substantially collinear pairs of said elements with different respective spacings, wherein the phase measurement on said one pair or on the closest-spaced of said pairs is ambiguous in the operating range of directions of incidence and the operating frequency range,

means, comprising a system as claimed in claim 6, for determining the approximate direction of incidence of said signals from the times of arrival of the leading edges of corresponding signals received respectively at two of said plurality of elements, the line joining said two elements is parallel to and substantially coincident with the line joining said one pair or said plurality of substantially collinear pairs, wherein the range of possible values of the actual time difference due to the uncertainty in the difference between the measured times corresponds to a range of angles of incidence whose magnitude is not greater than the magnitude of the range of angles of incidence corresponding to the unambiguous range of phase difference measurement on said one pair or said closest-spaced pair, and

means for resolving the ambiguity in said ambiguous phase measurement by comparing the possible directions represented thereby with the approximate direction determined from the difference between the measured times.

14. A system as claimed in claim 13 comprising phase-difference measuring means, approximate-direction-determining means and ambiguity-resolving means operable in respect of a first pair or a first plurality of substantially collinear pairs of the elements and of a second pair or a second plurality of substantially collinear pairs of the elements to derive first and second unambiguous phase measurements, wherein the line joining the elements of said first pair or said first plurality of pairs and the line joining the elements of said second pair or said second plurality of pairs are substantially coplanar and inclined to one another, said first and second phase measurements being representative of the angle α

between the direction of incidence and the line joining the elements of the respective pair(s), and further comprising means for deriving a representation of the angle θ and

/or a representation of the angle β

, where θ

is the angle between the direction of incidence projected into the plane of the lines and the normal to a respective one of said line in said plane and where β

is the angle between the direction of incidence and said plane, from the first and second unambiguous phase measurements utilising the relationship

space="preserve" listing-type="equation">sin (90 degrees-α

)=sin θ

cos β

.

15. A system as claimed in claim 14 wherein said lines are mutually perpendicular.

16. A system as claimed in claim 14 wherein the approximate-direction-determining means are operable in respect of the times of arrival at a common element and at each of two elements respectively on the two lines.

17. A system as claimed in claim 16 wherein the phase-difference measuring means are operable to measure the phase differences between said common element and each of two elements respectively on the two lines.

18. A system as claimed in claim 14 comprising three or more mutually inclined successively adjacent pairs or plurality of pairs of elements, means for measuring the amplitude of wave signals received at one or more elements of each of said three or more pairs or plurality of pairs, and means for selecting as said first pair or plurality of pairs one of said three or more pairs or plurality of pairs in respect of which the amplitude is at least as great as the amplitude in respect of each of the remaining pairs or plurality of pairs and as said second pair or plurality of pairs a pair or plurality of pairs adjacent said first pair or plurality of pairs in respect of which the amplitude is at least as great as the amplitude in respect of any other adjacent pair or plurality of pairs.

19. A system as claimed in claim 18 comprising four mutually orthogonal pairs or plurality of pairs of elements.

8. A system for determining the direction of incidence of electromagnetic wave signals from a distant source from the time of arrival of the leading edge of the wave signals, wherein the system comprises:

plurality of mutually spaced wave-receiving elements,

means for detecting the respective instantaneous amplitude of the signal received at each element,

means for measuring the times at which the detected amplitudes of wave signals received respectively at at least two of said elements first exceed a minimal threshold value such that signals can be satisfactorily distinguished from noise and which is substantially less than the minimum peak value of signals whose direction of incidence is to be determined by said method, the time being measured in such a manner that the measured time is generally unaffected by multipath propagation,

means for determining the difference between the measured times in respect of one pair or of a plurality of pairs of said elements, wherein the two elements of said one pair or of each of at least two of said plurality of pairs are sufficiently close together that the length of the interval of time within which signals from the same source must arrive at the two elements is so short that there is a high probability in operation that no signals from another source will arrive in that interval, and

means for deriving a representation of the direction of incidence from the time difference(s) utilising the relationship

space="preserve" listing-type="equation">cos α

=cδ

t/d

where α

is the angle between the direction of incidence of the signals and the line joining the two elements of a said pair, d is the distance between those two elements, δ

t is the time difference in respect of that pair of elements, and c is the free-space velocity of electromagnetic waves.

7. A method of determining the direction of incidence of electromagnetic wave signals from a distant source, the method comprising performing a method as claimed in claim 6 in respect of a first pair or a first plurality of substantially collinear pairs of the elements to derive a first unambiguous phase measurement, performing a method as claimed in claim 11 in respect of a second pair or a second plurality of pairs of substantially collinear pairs of the elements to derive a second unambiguous phase measurement, wherein the line joining the elements of said first pair or said first plurality of pairs and the line joining the elements of said second pair or said second plurality of pairs are substantially coplanar and inclined to one another, said first and second phase measurements being representative of the angle α

between the direction of incidence and the line joining the elements of the respective pair(s), and deriving a representation of the angle θ and

/or a representation of the angle β

, where θ

is the angle between the direction of incidence projected into the plane of the lines and the normal to a respective one of said lines in said plane and where β

is the angle between the direction of incidence and said plane, from the first and second unambiguous phase measurements utilising the relationship

space="preserve" listing-type="equation">sin (90 degrees-α

)=sin θ

cos β

.

9. A system as claimed in claim 8 comprising three substantially coplanar bu substantially non-collinear elements disposed to form at least two said pairs, wherein said means for deriving a representation of the direction of incidence comprises means for deriving a representation of the angle θ

and/or a representation of the angle δ

utilising the relationship

space="preserve" listing-type="equation">sin (90 -α

)=sin θ

cos β

in respect of each of said at least two pairs, wherein θ

is the angle between the direction of incidence projected into the plane of the three elements and the normal in said plane to the line joining the two elements of a said pair, and β

is the angle between the direction of incidence and said plane.

10. A system as claimed in claim 8 comprising means for determining a parameter representative of the rate of increase of the detected amplitude of the respective signal received at at least one of the elements in the region of said threshold value, and means for inhibiting the determination of the direction of incidence if said parameter does not satisfy a criterion representing a minimum rate of increase in said region.

11. A system as claimed in claim 10 wherein the parameter-determining means comprise means for measuring the time at which the detected amplitude first exceeds an adjacent further threshold value, said parameter being the difference between the measured times in respect of the two threshold values, and said criterion being that said parameter does not exceed a maximum value.

12. A system as claimed in claim 10 wherein the parameter-determining means comprise means for differentiating the increasing detected amplitude at least in said region, said parameter being the rate of increase in detected amplitude derived by differentiation, and said criterion being that said parameter exceeds a minimum value.

20. A timing circuit comprising a clock pulse generator, a tapped delay device having a plurality of n mutually spaced taps, a latch coupled to the delay device for latching any signal on each of the n taps, and a decoding device coupled to the latch for producing a time representation signal from the signal(s) latched from the n taps, characterised in that an input signal to be timed is coupled to the input of the delay device, in that the clock pulse generator is normally operable to clock the latch, in that the circuit comprises inhibiting means responsive to the presence of a signal on at least one of the n taps when the latch is clocked to inhibit further clocking of the latch, and in that the decoding device is operable to produce the time representation signal corresponding to the interval between the time that said input signal reaches the tap nearest the input of the delay device and the preceding clock pulse.

21. A circuit as claimed in claim 20 further comprising a counter for counting the pulses of the clock pulse generator, wherein the inhibiting means are further operable to inhibit further counting of the clock pulses, the outputs of the decoding device and the counter being concatenated.

22. A circuit as claimed in claim 20 or 21 wherein the period of the clock pulse generator is not substantially less than the time delay between the tap nearest to and the tap furthest from the input of the delay device.

23. A circuit as claimed in claim 22 wherein said period is substantially equal to said time delay.

24. A circuit as claimed in claim 23 wherein the time delay between each adjacent pair of the n taps is the same, being equal to T, and the period of the clock pulse generator is nT.

25. A circuit as claimed in claim 20 wherein the inhibiting means are responsive to the presence of a signal on the tap nearest the input of the delay device when the latch is clocked.

26. A circuit as claimed in claim 20 wherein the decoding device is operable not to produce said time representation unless when the latch is clocked a signal is present on each tap between the input of the delay device and the tap furthest from the input of the delay device on which a signal is present.

27. A method of determining the direction of incidence of electromagnetic wave signals from a distant source from the time of arrival of the leading edge of the wave signals, wherein the method comprises:

receiving said signals at a plurality of mutually spaced wave-receiving elements;

detecting the respective instantaneous amplitude of the signal received at each element;

producing a first signal indicating when the detected amplitude at a first wave-receiving element exceeds a selected threshold value;

producing a second signal indicating when the detected amplitude at a second wave-receiving element exceeds said selected threshold value;

determining from at least the first and second signals at least the time difference between when the detected amplitudes at said first and second wave-receiving elements exceed said threshold value; and

deriving a representation of the direction of incidence from the time difference utilizing the relationship cos α

=cδ

t/d where α

is the angle between the direction of incidence of the signals and the line joining the two elements of a said pair, d is the distance between those two elements, δ

t is the time difference in respect of that pair of elements, and c is the free-space velocity of electromagnetic waves.

28. A method of determining the direction of incidence of electromagnetic wave signals from a distant source, the method comprising:

receiving said signals at each of a plurality of mutually spaced wave-receiving elements;

measuring the phase difference between the signals received respectively at the two elements of one pair of said elements or the respective phase differences between the signals received respectively at the two elements of each of a plurality of substantially collinear pairs of said elements with different respective spacings, wherein the phase measurement on said one pair or on the closest-spaced of said pairs is ambiguous in the operating range of directions of incidence and the operating frequency range;

determing the approximate direction of incidence of said signals from the times of arrival of corresponding wave signals received respectively at two of said plurality of elements, the line joining said two elements is parallel to and substantially coincident with the line joining said one pair or said plurality of substantially collinear pairs, wherein the range of possible values of the actual time difference due to the uncertainty in the difference between the measured times corresponds to a range of angles of incidence whose magnitude is not greater than the magnitude of the range of angles of incidence corresponding to the unambiguous range of phase difference measurements on said one pair or said closest-spaced pair; and

resolving the ambiguity in said ambiguous phase measurement by comparing the possible directions represented thereby with the approximate direction determined from the differences between the measured times.

29. A system for determining the direction of incidence of electromagnetic wave signals from a distant source, comprising:

a plurality of mutually spaced wave-receiving elements;

means for measuring the phase difference between the signals received respectively at the two elements of one pair of said elements or the respective phase differences between the signals received respectively at the two elements of each of a plurality of substantially collinear pairs of said elements with different respective spacings, wherein the phase measurement on said one pair or on the closest-spaced of said pairs is ambiguous in the operating range of directions of incidence and the operating frequency range;

means for determining the approximate direction of incidence of said signals from the times of arrival the corresponding signals received respectively at two of said plurality of elements, the line joining said two elements is parallel to and substantially coincident with the line joining said one pair or said plurality of substantially collinear pairs, wherein the range of possible values of the actual time difference due to the uncertainty in the difference between the measured times correspond to a range of angles of incidence whose magnitude is not greater than the magnitude of range of angles of incidence corresponding to the unambiguous range of phase difference measurement on said one pair or said closest-spaced pair; and

means for resolving the ambiguity in said ambiguous phase measurement by comparing the possible directions represented thereby with the approximate directions determined from the difference between the measured times.