EP0261142A1 - Metal detection in conducting media using a two frequency signal - Google Patents

Metal detection in conducting media using a two frequency signal

Info

Publication number
EP0261142A1
EP0261142A1 EP87901005A EP87901005A EP0261142A1 EP 0261142 A1 EP0261142 A1 EP 0261142A1 EP 87901005 A EP87901005 A EP 87901005A EP 87901005 A EP87901005 A EP 87901005A EP 0261142 A1 EP0261142 A1 EP 0261142A1
Authority
EP
European Patent Office
Prior art keywords
signal
frequency
signals
interrogation
low
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP87901005A
Other languages
German (de)
French (fr)
Inventor
Bruce Halcro Candy
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Minelab Electronic Industries Ltd
Original Assignee
Minelab Electronic Industries Ltd
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Filing date
Publication date
Application filed by Minelab Electronic Industries Ltd filed Critical Minelab Electronic Industries Ltd
Publication of EP0261142A1 publication Critical patent/EP0261142A1/en
Withdrawn legal-status Critical Current

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Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/08—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation operating with magnetic or electric fields produced or modified by objects or geological structures or by detecting devices
    • G01V3/10—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation operating with magnetic or electric fields produced or modified by objects or geological structures or by detecting devices using induction coils
    • G01V3/104—Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation operating with magnetic or electric fields produced or modified by objects or geological structures or by detecting devices using induction coils using several coupled or uncoupled coils
    • A—HUMAN NECESSITIES
    • A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61N—ELECTROTHERAPY; MAGNETOTHERAPY; RADIATION THERAPY; ULTRASOUND THERAPY
    • A61N1/00—Electrotherapy; Circuits therefor
    • A61N1/02—Details
    • A61N1/04—Electrodes
    • A61N1/05—Electrodes for implantation or insertion into the body, e.g. heart electrode
    • A61N1/056—Transvascular endocardial electrode systems

Definitions

  • This specificat ion refers to a metal detector" of a type used for the purpose of discrim inating metal w ithin the ground which can be used as a single detector or an array of detectors where used to detect metal objects in soil on a moving conveyor system.
  • the invention is directed to some difficulties encountered when using a metal detector in the presence of ground containing substantial varying proportions of mildly electrically conducting soil components, such as brackish water and metal sulfides, and which may also contain magnetic soils which usually comprise contain ferrous oxide and various ferrites.
  • Highly conductive metal objects are different from the ground in that the ratio of resistive to reactive ratio is usually substantially different from that of the background soil.
  • metal objects are located by determining statistically significant changes in this reactive to resistive ratio of the scale size typical of the objects sought. If the reactive to resistive ratio is highly variable, which is often the case with a mix of magnetic soils and brackish water, the object detection sensitivity is thus reduced substantially compared to relatively homogeneous ground.
  • metal detectors there are a number of types of metal detectors each having a different type of operation. The best of these that are used for location of metal objects such as coins, gold nuggets, treasure caches etc , all have certain properties which are outlined below:
  • the induced signal in the received coil results from two sources, namely, from varying currents flowing in the transmitting coil, and varying (retransmitting) magnetic sources in the local environment under the influence of the transmitted magnetic field. For each Fourier component transmitted, the received signals resulting from local environmental sources induce both resistive and reactive components in the receiving coil.
  • the dominant "magnetic" ground component has a reactive (magnetic) component usually much greater that the resistive (loss) component (usually by about 30 to 200 times).
  • the ratio of the loss component in the Ironstone to it's magnetic component is spacially correlated in ground, but the ratio of resistive electrically conducting component to reactive ironstone component is not correlated.
  • the best of the existing metal detectors transmit a single frequency sinusoidal magnetic signal (distortion ⁇ 30dB) at between 1kHz to a few 10's of kHz.
  • the received signal is synchronously demodulated and passed through a low-pass filter to remove both noise and carrier related signals.
  • the better metal detectors have a "ground balance" control which enables the detector to be set to be insensitive to a local area of ground. This is normally performed by the user by varying a potentiometer or is performed automatically In effect varying the "ground balance” selects a varying linear combination of the reactive and resistive components. This can be represented by standard phasor diagrams, where the T axis represents the reactive component and the "X" the resistive component Vector mathematics can then be applied.
  • the detector “null” is settable between the reactive axis and about 10 degrees between this axis toward the resistive axis. This accommodates most ground conditions. In the more difficult environments described above, this adjustment need be made very frequently for best results. Worse, most detectors do not have sufficient "ground balance" control range to accommodate the extremes of ground containing predominatly ironstone or predominantly salt water.
  • apparatus for detecting remote metal target objects in soil by interrogation including means to transmit at least two substantially sinusoidal magnetic transmitted signals of different frequency, the apparatus being characterised in that there are means to effect at least two signals each derived from the synchronous demodulation of the composite incoming interrogation signal, whereby at least one demodulator reference is derived from one of the said transmitted signals, and another demodulator reference is derived from the other said transmitted signal, the apparatus being adapted to provide a resultant signal derived from linear combinations of the said demodulated signals which will provide discernable target discrimination information when within interrogated conducting soils or background conducting fluids.
  • a "simple first order" object can be described in terms of a single characteristic frequency Wo, for which the resistive component is a maximum and the magnitude of the resistive component equals that of the reactive component.
  • the said reactive component is to be taken as the "eddy current" associated anti-magnetic reactive component. If the interrogating frequency is W, then the relative resistive component is proportional to W*Wo/(Wo*Wo+W*W), and the reactive component is proportional to 2*W*W/(Wo*Wo+W*W)
  • the resistive component is proportional to the interrogation frequency, and the reactive component is very much less that the resistive component, host objects or mildly electrically conducting ground components can be described as having a distributed "Wo" rather than just a single frequency.
  • the distributions are typically relatively fairly narrow, and for most the mildy electrically conducting soil components, the resistive component is proportional to the interrogation frequency at the operating frequencies and scale sizes described above.
  • One means of substantially reducing sensitivity to mildly conductive components is to measure resistive components at two frequencies and subtract these after scaling each by the inverse of the associated frequency of each:
  • the 2 frequencies be F 1 and F2
  • the associated instantaneous ground components be X1e, X 1m, R1e, R1m, X2e, X2m, R2e, and R2m, where "X” stands for “reactive”, “R” for “resistive”, “1” for “f1”, “2” for “F2”, “e” for mildly electrically conductive and “m” for “ironstone”.
  • X and R may be represented as 2 vectors at right angles. If the system gains for each frequency are assumed equal:
  • the "ground balance” constant "k2" may be factory set and the value of "k1" altered to adjust the detector ground balance, "k1" may be adjusted manually or automatically.
  • FIG. 1 shows the block diagram of a preferred embodiment
  • FIG. 2 is a circuit of a dual frequency resonator
  • FIG. 3 is a circuit of a dual frequency resonator
  • FIG. 4 is the impedance frequency response of Fig. 2 and 3
  • FIG. 5 is a circuit of a triple frequency resonator
  • FIG. 6 is a circuit of a triple frequency resonator
  • FIG. 7 is the impedance frequency response of Fig. 5 and 6.
  • an oscillator 1 produces a frequency of W1 radians per second
  • an oscillator 2 produces a frequency of Wh radians per second, where Wh>Wl.
  • Sinusoidal outputs from these are fed into a combiner and amplifier 3.
  • This combined and amplified signal is applied to the transmitting coil 5 across which a dual resonator 4 is connected, which is described later.
  • Current flowing through the transmitting coil is passed through a low valued resistor 6, across which a resulant voltage appears which is used as a magnetic field phase sensor.
  • the receiver coil 7 picks up retransmitted signals from the interrogated environment (as well as directly from the transmitting coil).
  • the induced emf across the receiver is demodulated by a synchronous demodulator 8.
  • the digital reference 9 to this demodulator is driven by a phase-locked loop and phase-shifter 10.
  • This phase-locked loop is locked to the frequency of oscillator 1 and the phase of the current of Wl flowing through the resistor 6. This phase may be shifted for ground balancing purposes.
  • the induced emf across the receiver is demodulated by a synchronous demodulator
  • the digital reference 12 to this demodulator is driven by a phase-locked loop and phase-shifter 13.
  • This phase-locked loop is locked to the frequency of oscillator 2 and the phase of the current of Wh flowing through the resistor 6. This phase may be shifted for ground balancing purposes.
  • the output of the demodulator 8 is passed through a low-pass filter 14 and the output of of the demodulator 1 1 is passed through a low-pass filter 15.
  • the output of the low-pass filter 15 is scaled and subtracted by a subtracter 16 to produce an output 16.
  • the scaling factor is selected so that, when the phases of the digital references 9 and 12 are adjusted so that both the outputs of the low-pass filters 14 and 15 give substantially no response to the interrogation of a substantially lossless ferrite, then for these phase settings the output is substantially insensitive to the interrogation of objects with characteristic frequencies at least 20 times greater than Wh.
  • FIG. 2 A useful resonator for power efficiency and impedance frequency response is given in figure 2 to 7.
  • Figure 2 and 3 show dual frequency resonators, while figure 5 and 6 show triple resonators.
  • the resultant impedance frequency response is shown in figure 4 for the dual resonators and figure 7 for the triple resonators.
  • Wh and Wl refer to the high and low frequency resonant frequencies, and "Wo" to the "zero" of the impedance response. Equations for the dual resonator are contractable, and the solutions are:

Abstract

Un appareil permettant la détection électrique d'objets métalliques éloignés dans un environnement légèrement conducteur comprend une bobine émettrice (5) émettant simultanément deux signaux magnétiques de fréquence différente à partir de deux oscillateurs (1, 2) et une bobine réceptrice (7) recevant deux signaux retransmis à partir des objets métalliques. Les deux signaux retransmis sont traités par des démodulateurs différents (8, 11). Les informations concernant les objets métalliques sont obtenues soit en produisant un signal qui résulte de la combinaison linéaire des signaux démodulés ou en détectant la différence entre les composants résistants des signaux transmis et retransmis.An apparatus for the electrical detection of distant metal objects in a slightly conductive environment comprises a transmitter coil (5) simultaneously transmitting two magnetic signals of different frequency from two oscillators (1, 2) and a receiver coil (7) receiving two signals retransmitted from metallic objects. The two retransmitted signals are processed by different demodulators (8, 11). Information about metallic objects is obtained either by producing a signal which results from the linear combination of the demodulated signals or by sensing the difference between the resistant components of the transmitted and retransmitted signals.

Description

Metal Detecti on i n Conduct ing Med ia usi ng a two frequency signal
This specificat ion refers to a metal detector" of a type used for the purpose of discrim inating metal w ithin the ground which can be used as a single detector or an array of detectors where used to detect metal objects in soil on a moving conveyor system.
The invention is directed to some difficulties encountered when using a metal detector in the presence of ground containing substantial varying proportions of mildly electrically conducting soil components, such as brackish water and metal sulfides, and which may also contain magnetic soils which usually comprise contain ferrous oxide and various ferrites.
Highly conductive metal objects are different from the ground in that the ratio of resistive to reactive ratio is usually substantially different from that of the background soil. Thus in effect metal objects are located by determining statistically significant changes in this reactive to resistive ratio of the scale size typical of the objects sought. If the reactive to resistive ratio is highly variable, which is often the case with a mix of magnetic soils and brackish water, the object detection sensitivity is thus reduced substantially compared to relatively homogeneous ground.
There are a number of types of metal detectors each having a different type of operation. The best of these that are used for location of metal objects such as coins, gold nuggets, treasure caches etc , all have certain properties which are outlined below:
They all consist of electronic circuitry in which an alternating current signal is produced which is fed to a transmitting coil, and detection electronics which compares an emf signal induced in a receiver coil with the transmitted signal. The induced signal in the received coil results from two sources, namely, from varying currents flowing in the transmitting coil, and varying (retransmitting) magnetic sources in the local environment under the influence of the transmitted magnetic field. For each Fourier component transmitted, the received signals resulting from local environmental sources induce both resistive and reactive components in the receiving coil.
The dominant "magnetic" ground component has a reactive (magnetic) component usually much greater that the resistive (loss) component (usually by about 30 to 200 times). The dominant electrically conductive components at typical metal detecting frequencies (1 to 30 kHz) and scale sizes of the order of 10cm, have a resistive component much greater than the reactive component. It should be noted the sign of the ironstone reactive component is opposite to that of the electrically conductive reactive component.
The ratio of the loss component in the Ironstone to it's magnetic component is spacially correlated in ground, but the ratio of resistive electrically conducting component to reactive ironstone component is not correlated.
The best of the existing metal detectors transmit a single frequency sinusoidal magnetic signal (distortion < 30dB) at between 1kHz to a few 10's of kHz. The received signal is synchronously demodulated and passed through a low-pass filter to remove both noise and carrier related signals.
The better metal detectors have a "ground balance" control which enables the detector to be set to be insensitive to a local area of ground. This is normally performed by the user by varying a potentiometer or is performed automatically In effect varying the "ground balance" selects a varying linear combination of the reactive and resistive components. This can be represented by standard phasor diagrams, where the T axis represents the reactive component and the "X" the resistive component Vector mathematics can then be applied.
Usually the detector "null" is settable between the reactive axis and about 10 degrees between this axis toward the resistive axis. This accommodates most ground conditions. In the more difficult environments described above, this adjustment need be made very frequently for best results. Worse, most detectors do not have sufficient "ground balance" control range to accommodate the extremes of ground containing predominatly ironstone or predominantly salt water.
There is proposed according to this invention a means of substantially reducing the signal components resulting from mildly conductive soil components, thus enabling a detector that requires only moderate ground balance adjustment, to accommodate the "usual" ironstone reactive to resistive ration changes, as the detector interrogates ground containing varying electrical conductivities and ironstone (if present). This requires interrogation at at least two frequencies. In addition a means of power efficiently transmitting at least 2 frequencies simultaneously is described.
According to this invention then there is proposed apparatus for detecting remote metal target objects in soil by interrogation including means to transmit at least two substantially sinusoidal magnetic transmitted signals of different frequency, the apparatus being characterised in that there are means to effect at least two signals each derived from the synchronous demodulation of the composite incoming interrogation signal, whereby at least one demodulator reference is derived from one of the said transmitted signals, and another demodulator reference is derived from the other said transmitted signal, the apparatus being adapted to provide a resultant signal derived from linear combinations of the said demodulated signals which will provide discernable target discrimination information when within interrogated conducting soils or background conducting fluids.
THEORY:
A "simple first order" object can be described in terms of a single characteristic frequency Wo, for which the resistive component is a maximum and the magnitude of the resistive component equals that of the reactive component. In the case of ferromagnetic metals, the said reactive component is to be taken as the "eddy current" associated anti-magnetic reactive component. If the interrogating frequency is W, then the relative resistive component is proportional to W*Wo/(Wo*Wo+W*W), and the reactive component is proportional to 2*W*W/(Wo*Wo+W*W)
if Wo»W then, W*Wo/(Wo2+W2) is approximately = W/Wo,
and 2*W2/(Wo2+ w2) is approximately = 2*(wVWo)2 «W/Wo
The Important result of this approximation is that the resistive component is proportional to the interrogation frequency, and the reactive component is very much less that the resistive component, host objects or mildly electrically conducting ground components can be described as having a distributed "Wo" rather than just a single frequency. However, the distributions are typically relatively fairly narrow, and for most the mildy electrically conducting soil components, the resistive component is proportional to the interrogation frequency at the operating frequencies and scale sizes described above.
One means of substantially reducing sensitivity to mildly conductive components is to measure resistive components at two frequencies and subtract these after scaling each by the inverse of the associated frequency of each:
Let the 2 frequencies be F 1 and F2, the associated instantaneous ground components be X1e, X 1m, R1e, R1m, X2e, X2m, R2e, and R2m, where "X" stands for "reactive", "R" for "resistive", "1" for "f1", "2" for "F2", "e" for mildly electrically conductive and "m" for "ironstone". Using standard conventions, X and R may be represented as 2 vectors at right angles. If the system gains for each frequency are assumed equal:
R1e*F2 is approximately = R2e*F1 [i]
X_e« R_e [ii]
X1 m is approximately = X2m [iii] Typically X1m»X1e, and X1 m»X2e [iv] where"-" stands for either "1" or "2" It should be noted that owing to [ii], in areas containing no magnetic soils, only the resistive components give rise to significant signals. If the output "out" is selected so that
out2=R2+k2*X2, out1=R1+k1*X1, and out=F2*out 1-F1*out2
where"R_" and "X_" stand for the measured resistive and reactive components respectively, at the indicated frequency, and k1 and k2 have magnitudes of the order of .01, then the output will approximately be insensitive to the mildly conductive soil components, bu substitution of (i to iv) into the output expression.
The "ground balance" constant "k2" may be factory set and the value of "k1" altered to adjust the detector ground balance, "k1" may be adjusted manually or automatically.
For a better understanding of this Invention it will now be described with reference to a preferred embodiment with the assistance of drawings.
FIG. 1 shows the block diagram of a preferred embodiment,
FIG. 2 is a circuit of a dual frequency resonator,
FIG. 3 is a circuit of a dual frequency resonator,
FIG. 4 is the impedance frequency response of Fig. 2 and 3,
FIG. 5 is a circuit of a triple frequency resonator,
FIG. 6 is a circuit of a triple frequency resonator, and
FIG. 7 is the impedance frequency response of Fig. 5 and 6.
Referring to these in detail an oscillator 1 produces a frequency of W1 radians per second, and an oscillator 2 produces a frequency of Wh radians per second, where Wh>Wl. Sinusoidal outputs from these are fed into a combiner and amplifier 3. This combined and amplified signal is applied to the transmitting coil 5 across which a dual resonator 4 is connected, which is described later. Current flowing through the transmitting coil is passed through a low valued resistor 6, across which a resulant voltage appears which is used as a magnetic field phase sensor. The receiver coil 7 picks up retransmitted signals from the interrogated environment (as well as directly from the transmitting coil). The induced emf across the receiver is demodulated by a synchronous demodulator 8. The digital reference 9 to this demodulator is driven by a phase-locked loop and phase-shifter 10. This phase-locked loop is locked to the frequency of oscillator 1 and the phase of the current of Wl flowing through the resistor 6. This phase may be shifted for ground balancing purposes. Similarly the induced emf across the receiver is demodulated by a synchronous demodulator
1 1 . The digital reference 12 to this demodulator is driven by a phase-locked loop and phase-shifter 13. This phase-locked loop is locked to the frequency of oscillator 2 and the phase of the current of Wh flowing through the resistor 6. This phase may be shifted for ground balancing purposes. The output of the demodulator 8 is passed through a low-pass filter 14 and the output of of the demodulator 1 1 is passed through a low-pass filter 15. The output of the low-pass filter 15 is scaled and subtracted by a subtracter 16 to produce an output 16. The scaling factor is selected so that, when the phases of the digital references 9 and 12 are adjusted so that both the outputs of the low-pass filters 14 and 15 give substantially no response to the interrogation of a substantially lossless ferrite, then for these phase settings the output is substantially insensitive to the interrogation of objects with characteristic frequencies at least 20 times greater than Wh.
A useful resonator for power efficiency and impedance frequency response is given in figure 2 to 7. Figure 2 and 3 show dual frequency resonators, while figure 5 and 6 show triple resonators. The resultant impedance frequency response is shown in figure 4 for the dual resonators and figure 7 for the triple resonators. As indicated in these figures, "Wh" and "Wl" refer to the high and low frequency resonant frequencies, and "Wo" to the "zero" of the impedance response. Equations for the dual resonator are contractable, and the solutions are:
For figure (2);
C2=[k 1 [(Wh2+Wl 2)-Wo2]-1 /Wo2}/L1
L2=1/(C2*Wo2)
C1=Wo2*k 1/L 1
where k 1 =4/[(Wh2 +Wl 2)2-(Wh2-Wl 2)2],
For figure (3);
C2=k2*C1/(1-k2)
L2=1/[Wo2*(C1+C2)]
C1 =[Wh/[4*(Wh2-Wl2 )]-1/Wo2]/L1
where k2=Wo2/[4*(wh2-Wl2)*L I*C 1].
For example, for the network a figure (2), if the high frequency is set at 16kHz, the low at 2kHz, Wo is set as the geometric mean of Wh and Wl, and the transmission coll "LI" is 1mH, then L2= 16mH, C1 = 79mfd, C2=4.9mfd.
Several metal detectors have been constructed and tested spanning the range from 1 to 16kHz utilizing the principles described herein, with heads up to 30 cm in size, and all substantially reduce the effects of salt water. For example, if any conventional detector using a single frequency is ground balanced inland on typical dry magnetic soils, and then, without altering the ground balance setting, if the detector is used to interrogate wet sea beach sand or sea water, substantial unbalanced ground signals result This is substantially not the case. with the art described herein, for which the sea-side ground signals are similar to the inland ground signals.

Claims

1. Apparatus for detecting remote metal target objects in soil by interrogation including means to transmit at least two substantially sinusoidal magnetic transmitted signals of different frequency, the apparatus being characterised in that there are means to effect at least two signals each derived from the synchronous demodulation of the composite incoming interrogation signal, whereby at least one demodulator reference is derived from one of the said transmitted signals, and another demodulator reference is derived from the other said transmitted signal, the apparatus being adapted to provide a resultant signal derived from linear combinations of the said demodulated signals which will provide discernable target discrimination information when within interrogated conducting soils or background conducting fluids.
2. A metal detection system for detecting the presence of an electrically conducting metal target in soil or brackish water or both, including means for transmitting a first and second substantially sinusoidal magnetic interrogation signal, where the second signal is of higher frequency than the first, whereby the said frequency range and interrogation spacial scale size is chosed such that for brackish water, such as sea water, the resistive magnetic response is substantially proportional to the interrogation frequency,including detector means, including a coil means for transmitting the said magnetic field and detecting any retransmitted magnetic signal from the ground or any target, the detection of the said retransmitted signal processing means including a first synchronous demodulator referenced to the said first transmitted signal, and a second synchronous demodulator referenced to the said second transmitted signal, to interrogate the said retransmitted signal, and provide a first and second low-passed signal from the first and second synchronous demodulator output respectively, with the said demodulator reference phases selected whereby the said low-passed signals contain information substantially distinctive of background resistive components, an output signal is derived from a linear combination of the said first and second low-passed signals, such that the said combination is directly propotional to or at least directly proportional to changes in, the frequency of the second transmitted signal multiplied by the system gain of the said second low-passed signal multiplied by the first output signal, minus the frequency of the first transmitted signal multiplied by the system gain of the said first low-passed signal multiplied by the second output signal, where the system gain is defined as the relative sensitivity of the low-passed outputs to the interrogation of a lossless ferrite when the synchronous demodulator reference phases are set so as the maximise the low-passed signal components resulting from the interrogation of the said ferrite.
3. Apparatus as in claim 2 further including means for controlling the phase of the synchronous demodulators.
4 Apparatus as in claim 1,2 or 3 including means for efficient multi-frequency resonator, whereby the impendance measured acrqss the transmitter coil terminals is relatively high at the transmission frequencies, and the impendance frequency response has local maxima at these said frequencies.
5. Apparatus as in claim 4 further comprising the said transmission coil, across which is connected parallel networks; one type contains a capacitor connected in series with a parallel combination of a capacitor and inductor, another type consisting of a capacitor connected in series with an inductor, another type consisting of a capacitor, and yet another type consists of a series circuit of two networks of a capacitor connected in parallel with an inductor, whereby the values and combinations are selected to fulfil the requirements of claim 4.
6. A method of detecting a metal target in a mildly electrically conducting environment which comprises the steps of transmitting a magnetic field which incorporates two sinusoidal components, the frequency being different one from the other, detecting any retransmitted signal from the environment, distinguishing the resistive component for each of the said transmitted frequencies from the retransmitted signal, and detecting any difference in magnitude between the respective resistive components thus detected.
7. A method as in claim 6 further characterised in that the frequencies selected and the gains of the measured resistive components of the signals are selected whereby a direct subtraction results in cancellation of interrogated objects with characteristic frequencies at least twenty times the higher interrogation frequency, but not for those objects with less than 10 times the charateristic freqency of the higher interrogation frequency.
EP87901005A 1986-02-04 1987-02-04 Metal detection in conducting media using a two frequency signal Withdrawn EP0261142A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
AUPH442886 1986-02-04
AU4428/86 1986-02-04

Publications (1)

Publication Number Publication Date
EP0261142A1 true EP0261142A1 (en) 1988-03-30

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WO (1) WO1987004801A1 (en)
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ZA87810B (en) 1987-09-30

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