Method and apparatus for metal detection employing digital signal processing

• US 7,432,715 B2
• Filed: 08/26/2005
• Issued: 10/07/2008
• Est. Priority Date: 08/26/2004
• Status: Active Grant

• Current Assignee: Minelab Electronics Pty Limited (Codan Ltd.)
• Original Assignee: Minelab Electronics Pty Limited (Codan Ltd.)
• Inventors: Stamatescu, Laurentiu
• Primary Examiner(s): LEDYNH, BOT L
• Application Number:
  US11/574,065
• Publication Number:
  US 20070296415A1
• Time in Patent Office: 1,138 Days
• Field of Search: 324228-229, 324/234, 324238-243, 324256-258, 324/326, 324329-331, 324/345, 702 35- 38, 702/94, 702/104, 702115-116, 702/124, 702/150, 702/158, 702/166, 702/172
• US Class Current: 324/345
• CPC Class Codes: G01V 3/104 using several coupled or uncoupled coils G01V3/101 takes precedence

Abstract

A metal detector employing digital means for the generation of highly quality reference signals used for transmission and demodulation and capable of continuously monitoring the parameters of the transmitting and receiving coils. Using the monitored signals and calibration of the measurements paths in both amplitude-frequency and phase-frequency, the effects of the targets and magnetic and/or conductive grounds on the transmitting and receiving coils are greatly reduced, leaving the received signals substantially free of instrumental effects. Methods of ground tracking and filtering are described to separate target information from the ground plus-target receive signals. Single-and multi-frequency operation, with or without modulation for both sinusoidal and square wave transmission, is described, as are means to detect abnormal situations and to find and operate at resonance.

Claims

1. A metal detector of the continuous wave type including;

a transmission circuit and a transmitter coil adapted to produce an interrogating magnetic field for detection of a target;

a receiving coil and a receiving circuit adapted to receive and process a receive signal produced by a target and its environment in the interrogating field;

further including at least one digital signal generator adapted to generate at least one pair of reference sinusoidal signals of the same frequency;

wherein there is produced one or more output signals which are a linear combination of selected of said reference signals, said output signals being applied to a transmitter which produces at least one transmission signal said transmission signal being applied to the transmission circuit and transmitter coil combination to produce an interrogating magnetic field for detection of a target.

2. The metal detector of claim 1 wherein the digital signal generator generates two sinusoidal reference signals in quadrature.

3. The metal detector of claim 1 wherein the sinusoidal reference signals are produced with constant amplitude, substantially undistorted and substantially free of spurious signals.

4. The metal detector of claim 1 wherein the sinusoidal reference signals are generated using a method combining a direct digital synthesis method with a method producing mathematically correct results employing trigonometric identities.

5. The metal detector of claim 4, wherein the reference signal value corresponding to an angle φ

, which differs from an angle θ

for which the reference signal value is tabulated by an amount δ

such that φ

=θ

+δ

, is generated using the trigonometric identities;

cos(φ

)=cos(θ

+δ

)=cos(θ

)+[α

cos θ

−

β

sin θ

],

sin (φ

)=sin(θ

+δ

)=sin(θ

)+[α

sin θ

−

β

cos θ

],

and wherein

α

=−

2sin²(δ

/2), β

=sin(δ

),

and where for computational convenience values of α and

β

can be stored in an auxiliary table.

6. The metal detector of claim 1 including means adapted to monitor the current through and/or the voltage across the transmitter coil and/or the transmission circuit, the values provided by said current or voltage monitoring being processed in combination with the receive signal to identify, at least in part, those components of the received signal which are due to the changes in the transmit coil parameters produced by targets or varying soil or environmental conditions.

7. The metal detector of claim 6 wherein the processing of the monitored current and/or voltage values results in determination of the instantaneous phases and amplitudes of the signals transmitted by the transmitting coil.

8. The metal detector of claim 7 wherein the means to monitor include, within the transmission circuitry, a sensor element operatively connected to the transmitting coil, the voltage across which or the current through which, is amplified, filtered and applied to an analogue to digital converter to produce a digital signal proportional to the current in the transmitting coil.

9. The metal detector of claim 8 wherein the sensor element includes a low value resistor, current transformer, low value inductor or large value capacitor.

10. The metal detector of claim 8 wherein the means to monitor includes amplifying the total voltage across the transmitting coil and sensor element, filtering this and applying it to an analogue to digital converter.

11. The metal detector of claim 6 wherein the values of current and/or voltage are used to detect and correct for abnormal operating conditions including transmitting coil short-circuit or open-circuit.

12. The metal detector of claim 6 wherein the values of current and/or voltage are used in conjunction with the digital signal generator to find one or more resonant frequencies of the transmitting circuit and therefore to reduce the current consumption of the transmitter or to maximize the current through the transmitting coil.

13. The metal detector of claim 1 wherein there are means to monitor the values of receiving coil parameters which vary in use, the parameter values provided by said monitoring being processed in combination with the receive signal to identify, at least in part, the varying component of the received signals which is due to changes in the receive coil parameters produced by targets and varying soil or environmental conditions.

14. The metal detector of claim 13 wherein the means to monitor includes the generation of a pair of additional reference signals having a frequency different to any one or all of the frequencies of the transmitted signal or harmonics thereof, one of the additional reference signals being applied to the receiving coil with a suitable magnitude, the resultant signal in the receiving coil being detected by the receiving circuitry as part of the receive signal, the resultant signal being separated from the receive signal by post-processing to determine receiving coil parameters.

15. The metal detector of claim 1 where the output signal is a digitally constructed signal and is applied to a digital to analogue converter to generate a transmission signal that is substantially a linear combination of sinusoidal signals and applied to the transmitter which is a linear amplifier.

16. The metal detector of claim 15 where the frequencies of the reference signals are not integer multiples of each other.

17. The metal detector of claim 15 where the relative amplitudes of the sinusoidal signals that make up the transmission signal are controlled to maximize the response of specific targets or to avoid the saturation of the receiver and/or analogue to digital converter following the receiver.

18. The metal detector of claim 15 where the transmission circuit includes at least one circuit consisting of a transformer where each winding has substantially the same inductance as the transmitter coil and connected such that two signals of different frequency can be applied to the transmitter coil without each significantly influencing the other.

19. The metal detector of claim 1 wherein the digital signal generator generates an output signal that is substantially a square wave.

20. The metal detector of claim 19 wherein the frequency of one of the reference signal pairs is the fundamental frequency of the square wave and the other reference signal pairs are harmonics of the fundamental.

21. The metal detector of claim 19 wherein the output signal is applied directly to the transmitter, which is a switching amplifier.

22. The metal detector of claim 1 where the transmit signals are modulated in one of a multitude of possible modulations and the receive signals are demodulated and low pass filtered to yield the in phase and in quadrature components and their derivatives with respect to frequency at each transmitted frequency.

23. The metal detector of claim 1 where ground related components in the receive signal are substantially separated from target related signals in the receive signal using a method that employs models for the ground which include an independent magnetic component and an independent conductive component, the method further including the effects of varying coupling between the transmitter coil or the receiving coil and the ground.

24. The metal detector of claim 23 wherein the ground signal is estimated continuously with estimates for the values of the magnetic and conductive components are updated over a longer time span than estimates for the value of the coupling.

25. The metal detector of claim 23 wherein a model employed is that of a super paramagnetic medium.

26. The metal detector of claim 1 where the target components more contaminated with ground related signals are estimated using a matched filter employing as a template the target components less contaminated with ground related signals.

27. The metal detector of claim 1 where the amplitude-frequency and phase-frequency characteristics of each individual element and/or groups of elements are calibrated over the frequency ranges of interest.

28. A method for detecting metallic targets in a ground including the steps of

providing a transmission circuit and a transmitter coil adapted to produce an interrogating magnetic field for detection of a target;

providing a receiving coil and a receiving circuit adapted to receive and process a receive signal produced by a target and its environment in the interrogating field;

generating by digital means at least one pair of reference sinusoidal signals of the same frequency;

producing one or more output signals which are a linear combination of selected of said reference signals;

transmitting said output signal to produce the interrogating magnetic field for detection of a target.

29. The method of claim 28 wherein the sinusoidal reference signals are generated using a method combining a direct digital synthesis method with a mathematically correct method employing trigonometric identities.

30. The method of claim 29, wherein the reference signal value corresponding to an angle φ

, which differs from an angle θ

for which the reference signal value is tabulated by an amount δ

such that φ

=θ

+δ

is generated using the trigonometric identities;

cos(φ

)=cos(θ

+δ

)=cos(θ

)+[α

cos θ

−

β

sin θ

],

sin (φ

)=sin(θ

+δ

)=sin(θ

)+[α

sin θ

−

β

cos θ

],

and wherein

α

=−

2sin²(φ

/2), β

=sin(δ

),

and where for computational convenience values of α and

β

can be stored in an auxiliary table.

31. The method of claim 28 further including monitoring the values of parameters of the transmit coil which vary with time or with characteristics of the ground or with movement over the ground, the values provided by said monitoring being processed in combination with a received signal to identify, at least in part, that component of the received signal which is due to the changes in the transmit coil parameters produced by targets and varying soil or environmental conditions.

32. The method of claim 28 further including monitoring the values of receiving coil parameters which vary in use, the parameter values provided by said monitoring being processed in combination with the receive signal to identify, at least in part, the varying component of the received signals which is due to changes in the receive coil parameters produced by targets and varying soil or environmental conditions.

33. The method of claim 32 including the generation of a pair of additional reference signals having a frequency different to any one or all of the frequencies of the transmitted signal or harmonics thereof, one of the additional reference signals being applied to the receiving coil with a suitable magnitude, the resultant signal in the receiving coil being detected by the receiving circuitry as part of the receive signal, the resultant signal being separated from the receive signal by post-processing to determine receiving coil parameters.

34. The method of claim 32 further including the use of a digital signal generator and the values provided by said monitoring to find one or more resonant frequencies of the transmitting circuit and therefore to reduce the current consumption of the transmitter or to maximize the current through the transmitting coil.

35. The method of claim 28 where the output signal is a digitally constructed signal and is applied to a digital to analogue converter to generate a transmission signal that is substantially a linear combination of sinusoidal signals and applied to the transmitter which is a linear amplifier.

36. The method of claim 28 where the frequencies of the reference signals are not integer multiples of each other.

37. The method of claim 28 where the relative amplitudes of the sinusoidal signals that make up the transmission signal are controlled to maximize the response of specific targets or to avoid the saturation of the receiver and/or analogue to digital converter following the receiver.

38. The method of claim 28 further including the modulation of the transmit signal in one of a plurality of possible modulations and the receive signals are demodulated and low pass filtered to yield the in phase and in quadrature components and their derivatives with respect to frequency at each transmitted frequency.

39. The method of claim 28 where ground related components in the receive signal are substantially separated from target related signals in the receive signal using a method that employs models for the ground which include an independent magnetic component and an independent conductive component, the method further including the effects of varying coupling between the transmitter coil or the receiving coil and the ground.

40. The method of claim 39 wherein the ground signal is estimated continuously with estimates for the values of the magnetic and conductive components are updated over a longer time span than estimates for the value of the coupling.

41. The metal detector of claim 40 wherein a model employed is that of a super paramagnetic medium.

42. The method of claim 28 where the target components more contaminated with ground related signals are estimated using a matched filter employing as a template the target components less contaminated with ground related signals.

43. The method of claim 28 where the amplitude-frequency and phase-frequency characteristics of each individual element and/or groups of elements are calibrated over the frequency ranges of interest.