Enhanced sonde recognition

• US 7,567,875 B2
• Filed: 10/14/2005
• Issued: 07/28/2009
• Est. Priority Date: 10/14/2005
• Status: Active Grant

• Current Assignee: Radiodetection Limited
• Original Assignee: Radiodetection Limited
• Inventors: Royle, John Mark
• Primary Examiner(s): Le; John H
• Application Number:
  US11/249,749
• Publication Number:
  US 20070084636A1
• Time in Patent Office: 1,383 Days
• Field of Search: 702/65, 702/66, 702/75, 702/127, 702189-194, 702/197, 375/232, 375/259, 375/345, 324/326, 324/329, 340/333, 340/572.5, 340/854, 175/45, 175/259
• US Class Current: 702/65
• CPC Class Codes: G01V 3/08 operating with magnetic or electric fields produced or modified by objects or geological structures or by detecting devices with electromagnetic waves G01V3/12

Abstract

A detector for locating a sonde is comprised of a plurality of antennas, a corresponding number of signal isolator modules 1 and a geometrical evaluation module. The magnetic signal generated by the sonde has a fundamental frequency and harmonic frequencies. A frequency spectrum analyzer 29 which forms part of the signal isolator module 1 has frequency bins which are aligned with the fundamental frequency and a plurality of harmonic frequencies of the magnetic signal produced by the sonde. The frequency bins follow variations in the frequency of the magnetic signal produced by the sonde which allows the detector to detect the sonde at a separation of up to 30m.

Claims

1. A digital signal isolator module for detecting an oscillating magnetic signal produced by a sonde, the digital signal isolator module comprising:

an analog-to-digital converter to convert an analog signal, received from an antenna, to a digital signal, the analog signal including fundamental and harmonic frequencies associated with an oscillating magnetic signal; and

a digital signal processor, coupled to the analog-to-digital converter, to process the digital signal, the digital signal processor including a frequency spectrum analyser having an output and frequency bins that are substantially aligned with the fundamental frequency and a plurality of the harmonic frequencies of the magnetic signal.

2. A digital signal isolator module as claimed in claim 1, wherein the frequency bins are adapted to follow frequency variation of the magnetic signal produced by the sonde.

3. A digital signal isolator module as claimed in claim 1, wherein the output from the spectrum analyser is passed to a matched filter which produces a rank correlation coefficient.

4. A digital signal isolator module as claimed in claim 3, wherein the output from the matched filter is passed to an arbitrator which decides whether the sonde is detectable by the detector or not.

5. A digital signal isolator module as claimed in claim 1, wherein the frequency spectrum analyser comprises a complex discrete Fourier transform.

6. A digital signal isolator module as claimed in claim 5, wherein one of the frequency bins of the frequency spectrum analyser is aligned within 20 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

7. A digital signal isolator module as claimed in claim 5, wherein one of the frequency bins of the frequency spectrum analyser is aligned within 10 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

8. A digital signal isolator module as claimed in claim 5, wherein one of the frequency bins of the frequency spectrum analyser is aligned within 5 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

9. A digital signal isolator module as claimed in claim 5, the output of the frequency spectrum analyser being comprised of measurements of the fundamental frequency and harmonic frequencies of the magnetic signal produced by the sonde and measurements of noise, allowing a signal to noise ratio to be calculated for the fundamental frequency and harmonic frequencies, wherein the signal to noise ratio for at least 4 of the harmonic frequencies is greater than 6 dB.

10. A digital signal isolator module as claimed in claim 5, wherein the signal to noise ratio for at least 8 of the harmonic frequencies is greater than 6 dB.

11. A digital signal isolator module as claimed in claim 1, wherein the signal to noise ratio for at least 16 of the harmonic frequencies is greater than 6 dB.

12. The digital signal isolator module of claim 1, wherein the digital signal processor includes:

a homodyne mixer to process the digital signal received from the analog-to-digital converter;

a decimator and down sampler coupled to the homodyne mixer;

a low pass filter coupled to the decimator and down sampler; and

a complex signal combiner, coupled to the low pass filter, to output magnitude and phase information associated with the oscillating magnetic signal.

13. The digital signal isolator module of claim 12, wherein the digital signal processor includes a phase control feedback loop coupled to the complex signal combiner and the homodyne mixer.

14. A method of detecting an oscillating magnetic signal produced by a sonde, the method comprising:

converting an analog signal, received from an antenna, to a digital signal, the analog signal including fundamental and harmonic frequencies associated with an oscillating magnetic signal; and

processing the digital signal, including analysing the digital signal using a frequency spectrum analyser having an output and frequency bins that are substantially aligned with the fundamental frequency and a plurality of the harmonic frequencies of the magnetic signal.

15. A method as claimed in claim 14, wherein the frequency bins follow frequency variation of the magnetic signal produced by the sonde.

16. A method as claimed in claim 14, wherein the output from the spectrum analyser is filtered to produce a rank correlation coefficient.

17. A method as claimed in claim 16, wherein the rank correlation coefficient is arbitrated to decide whether the sonde is detectable by the detector or not.

18. A method as claimed in claim 14, wherein the frequency spectrum analyser is as a complex discrete Fourier transform.

19. A method as claimed in claim 14, wherein one of the frequency bins of the frequency spectrum analyser is aligned within 20 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

20. A method as claimed in claim 14, wherein one of the frequency bins of the frequency spectrum analyser is aligned within 10 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

21. A method as claimed in claim 14, wherein one of the frequency bins of the frequency spectrum analyser is aligned within 5 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

22. A method as claimed in claim 14, the output of the frequency spectrum analyser being comprised of measurements of the fundamental frequency and harmonic frequencies of the magnetic signal produced by the sonde and measurements of noise, the method comprising measuring the signal to noise ratio of the fundamental frequency and harmonic frequencies, wherein the signal to noise ratio for at least 4 of the harmonic frequencies is greater than 6 dB.

23. A method as claimed in claim 14, wherein the signal to noise ratio for at least 8 of the harmonic frequencies is greater than 6 dB.

24. A method as claimed in claim 14, wherein the signal to noise ratio for at least 16 of the harmonic frequencies is greater than 6 dB.

25. A computer program embodied on a computer readable medium for detecting an oscillating magnetic signal produced by a sonde, the computer program comprising:

receiving a digital signal from an analog-to-digital converter, the digital signal being converted from an analog signal that includes fundamental and harmonic frequencies associated with an oscillating magnetic signal; and

processing the digital signal, including analysing the digital signal using a frequency spectrum analyzer having an output and frequency bins that are substantially aligned with the fundamental frequency and a plurality of the harmonic frequencies of the magnetic signal.

26. A computer program as claimed in claim 25, wherein the frequency bins follow frequency variation of the magnetic signal produced by the sonde.

27. A computer program as claimed in claim 25, wherein the output from the frequency spectrum analyzer is filtered to produce a rank correlation coefficient.

28. A computer program as claimed in claim 27, wherein the rank correlation coefficient is arbitrated to decide whether the sonde is detectable by the detector or not.

29. A computer program as claimed in claim 25, wherein the frequency spectrum analyzer is a complex discrete Fourier transform.

30. A computer program as claimed in claim 25, wherein one of the frequency bins of the frequency spectrum analyzer is aligned within 20 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

31. A computer program as claimed in claim 25, wherein one of the frequency bins of the frequency spectrum analyzer is aligned within 10 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

32. A computer program as claimed in claim 25, wherein one of the frequency bins of the frequency spectrum analyzer is aligned within 5 mHz of the fundamental frequency of the magnetic signal produced by the sonde.

33. A computer program as claimed in claim 25, the result of said analysing being comprised of measurements of the fundamental frequency and harmonic frequencies of the magnetic signal produced by the sonde and measurements of noise, the computer program comprising measuring the signal to noise ratio of the fundamental frequency and harmonic frequencies, wherein the signal to noise ratio for at least 4 of the harmonic frequencies is greater than 6 dB.

34. A computer program as claimed in claim 25, wherein the signal to noise ratio for at least 8 of the harmonic frequencies is greater than 6 dB.

35. A computer program as claimed in claim 25, wherein the signal to noise ratio for at least 16 of the harmonic frequencies is greater than 6 dB.