# Two-Channel Metal Detector Using Two Perpendicular Antennas

Authors: Kyoo Nam Choi
Journal: Journal of Sensors
 (2014)

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## Abstract

Two-channel metal detector, having two sets of perpendicularly oriented sensor antennas, is proposed to expand detectable size, ranging from mm through cm scale, of metal sensor, while conventional metal sensor is dedicated for detection only in mm or cm scale. The characteristics of the two metal detection sensor channels were investigated, respectively, and the interference effect, while in simultaneous operation, between two sensor channels was discussed. Metal detection channel, having sensitivity in mm scale, showed detectable sensitivity to moving ferrous sphere, with diameter down to 0.7 mm, at 50 kHz exciting frequency and enhanced sensitivity distribution. And metal detection channel having sensitivity in cm scale showed more uniform sensitivity distribution with the flexibility for future modular construction. The effect of interference, while in simultaneous operation of two sensors, resulted in reduced output response, but still within usable detection range. Thus it was feasible to operate two sensors, having different sensitivity range, simultaneously and to extend detection range from mm to cm scale, within practically acceptable interference.


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## Body

## 1. Introduction

The metal detection sensor is now widely used in not only food processing industry but also defense industry [1, 2] to detect metal pieces in surrounding object, and considerable efforts have been devoted to enhance sensitivity and selectivity. Foreign materials are not only metal but also wood, ceramics [3], and germs [4], which are not detectable by using metal sensor. Other methods are envisaged to detect these materials which are not detectable by using metal sensor. Among these foreign materials, the detection for metal pieces is important [5] in food industry, and various researches are concentrating on this. The demand for metal detection is high in food industry, and recently the detection methods by using X-ray [6] and light [7] have been already applied for this. However the method using electromagnetic wave is dominant, and recently the method using superconducting coil has been attempted [8, 9]. Theoretical analysis [10, 11] and sensitivity analysis [12, 13] along with the shape of metal sensor have been performed to explore the sensitivity of electromagnetic metal sensor. On the other hand, there were attempts [14] to enhance visibility of metal piece through signal processing. The parent body containing metal piece is important from the point of selectivity, and the effort to detect foreign pieces in powder has been attempted [15]. The structure of sensor head in metal detector plays an important role in terms of sensitivity, and relevant studies [16] have been conducted in this regard. Active researches have been performed for the various kinds and shapes of metal in metal sensor head [17]. However the single channel metal detection sensor has not shown sensitivity resolution through wide range of metal sizes from mm to cm scale. Thus there was a need to cascade the sensors having different sensitivity resolutions. Metal detection sensor, using electromagnetic wave, usually is strongly influenced by nearby electromagnetic wave which is within several times of sensor width; thus it is not feasible to place a second sensor in the vicinity of the first sensor. This paper is concerned with the experimental development of two channel metal sensors by cascading two metal sensors having different sensitivity resolution with minimum interference with each other. Two-perpendicular-antennas model is introduced to minimize physical interference, and the optimal signal detection method is investigated to reject the interference between metal sensors having different sensitivity resolution.


## 2. Two-Antenna Model

### 2.1. Single Channel Model

The conventional metal detection sensor with sensitivity resolution in mm scale has the antenna set, one transmitting antenna and two receiving antennas which are connected in opposite polarity to cancel reception signal while in steady state. In case when an object containing a nonspherical metal piece is fed through hollow antenna cross-sectional space as shown in Figure1, then the sensor shows good sensitivity only for one directional position, between metal piece and antenna, where the perturbation in electromagnetic flux linkages becomes maximum. In the single channel model, the moving object containing metal piece perturbs gradually from first electromagnetic flux linkages between TX antenna #1 and RX antenna #1 to second electromagnetic flux linkages between TX antenna #1 and RX antenna #2. The amounts of these spatially varying electromagnetic flux linkages induce currents into RX antennas #1 and #2, and the current difference between RX antennas #1 and #2 becomes output current, which represent the electromagnetic flux unbalance of antenna set #1.Figure 1
Conventional antenna set of metal detection sensor.The equivalent circuit of an antenna set, one transmitting and two receiving antennas, is shown as in Figure2. The instantaneous output voltage v10, in no load condition, can be expressed as the difference of mutual inductance, M1-M2, between transmitting and respective receiving antenna as shown in (1), and is also proportional to exciting frequency as shown in (3). In this model, the distance between transmitting antenna and receiving antenna is closer than the distance to passing object containing metal piece; thus antenna inductances are larger than mutual inductance, M11 and M12. If transmitting antenna is excited using sinusoidal signal, e1s=e10sin(ωt+δ), then antenna current becomes as shown in (2). Consider
(1)v10=v11-v12=(M11-M12)dip1dt,(2)ip1=jωLp1e10(ϖLp1)2+Rp12sin(ωt+δ),(3)v10=jω2Lp1e10(M11-M12)(ϖLp1)2+Rp12cos⁡(ωt+δ).Equivalent circuit of antenna set: (a) schematic diagram and (b) equivalent circuit.
(a)
(b)When the phasor expression is used for the flux linkageψ, then the phasor voltage V due to flux linkage can be expressed as in (4) where I denotes phasor current:
(4)V10=jωψ10=jω(M11-M12)Ip1.It is noted that mutual inductance variance plays a key role in determining sensitivity of metal detection sensor. The mutual inductance is expressed as in (5), in which k11 and k12 represent coupling coefficient between transmitting and receiving antennas, respectively. And these coupling coefficients have the value 0≤k11, k12≤1:
(5)M11=k11Lp1Ls1/2,M12=k12Lp1Ls1/2.In steady state of initial measurement,M11 and M12 are adjusted to M11=M12, and output voltage becomes v10≈0. When ω is higher and M11-M12 are bigger for the same size of metal piece, then it is advantageous in terms of sensitivity.


### 2.2. Two-Channel Model

In the two antenna sets as shown in Figure3, the moving object after passing antenna set #1 perturbs gradually from third electromagnetic flux linkages between TX antenna #2 and RX antenna #4 to fourth electromagnetic flux linkages between TX antenna #2 and RX antenna #3. Also the amounts of spatially varying electromagnetic flux linkages induce currents into RX antennas #4 and #3, and the current difference between RX antennas #4 and #3 becomes output current of antenna set #2.Figure 3
Two antenna sets of metal detection sensor.It is difficult to calculate the variance of mutual inductance for the moving object; thus experimental method is attempted. By using the model in Figure4, the output voltage in each antenna set becomes the product of mutual inductance matrix and instantaneous current of each transmitting antenna as in
(6)[V10V20]=jω[M11-M12M21-M22M13-M14M23-M24][Ip1Ip2].Figure 4
Sensor layout for two antenna sets.AssumeIT11 is phasor current in one conductor of TX antenna #1, D is the distance, P in subscript is the remote point outside antenna, T in first subscript alphabet is transmitting antenna, R in first subscript alphabet is receiving antenna, the number in second subscript numeric is antenna number, the number in third subscript numeric is conductor number of antenna, and 4th through 6th alphabet and numeric follow the same convention as in 1st through 3rd alphabet and numeric. Then DR11T11 is the distance between one conductor of RX antenna #1 and one conductor of TX antenna #1, and DT11P is the distance between one conductor of TX antenna #1 and a remote point P. The flux linkage ψR11T11 with one conductor of RX antenna #1 due to one conductor of TX antenna #1 can be expressed as in
(7)ψR11T11=2×10-7(IT11ln⁡DT11PDR11T11).If we consider flux linkage to one conductor of receiving antenna #1 from two transmitter antennas, this flux linkageψR11 can be expressed as in
(8)ψR11=ψR11T11+ψR11T12+ψR11T21+ψR11T22=2×10-7(IT11ln⁡DT11PDR11T11+IT12ln⁡DT12PDR11T12+IT21ln⁡DT21PDR11T21+IT22ln⁡DT22PDR11T22)=2×10-7(IT11ln⁡1DR11T11+IT12ln⁡1DR11T12+IT21ln⁡1DR11T21+IT22ln⁡1DR11T22+IT11ln⁡DT11P+IT12ln⁡DT12P+IT21ln⁡DT21P+IT22ln⁡DT22P1DR11T11).In this configuration, the sum of two currents in TX antenna #1 is zero,IT11+IT12=0; also likewise IT21+IT22=0 for TX antenna #2. Let the point P move infinitely far away so that the set of terms containing logarithms of ratios of distances from P becomes infinitesimal; then the ratio of the distances approaches 1. Substituting these into (8) and recombining some logarithmic terms, we have (9) with the unit weber-turns/meter:
(9)ψR11=2×10-7(IT11ln⁡DR11T12DR11T11+IT21ln⁡DR11T22DR11T21).Thus flux linkageψR1 in RX antenna #1 becomes sum of ψR11 and ψR12 as shown in
(10)ψR1=2×10-7(IT11ln⁡DR11T12DR11T11+IT11ln⁡DR12T12DR12T11+IT21ln⁡DR11T22DR11T21+IT21ln⁡DR12T22DR12T21)=2×10-7((ln⁡DR11T12DR11T11+ln⁡DR12T12DR12T11)IT11+(ln⁡DR11T22DR11T21+ln⁡DR12T22DR12T21)IT21)=4×10-7(ln⁡DR11T12DR12T12DR11T11DR12T11IT11+ln⁡DR11T22DR12T22DR11T21DR12T21IT21).Likewise all mutual inductances includingM11 and M21 are expressed in a similar way as is shown in
(11)M11=4×10-7ln⁡DR11T12DR12T12DR11T11DR12T11,M21=4×10-7ln⁡DR11T22DR12T22DR11T21DR12T21,M12=4×10-7ln⁡DR21T12DR22T12DR21T11DR22T11,M22=4×10-7ln⁡DR21T22DR22T22DR21T21DR22T21,M13=4×10-7ln⁡DR31T12DR32T12DR31T11DR32T11,M23=4×10-7ln⁡DR31T22DR32T22DR31T21DR32T21,M14=4×10-7ln⁡DR41T12DR42T12DR41T11DR42T11,M24=4×10-7ln⁡DR41T22DR42T22DR41T21DR42T21.When a foreign object, for example, a metal cube, passes through the above flux linkage, then the above mutual inductanceM will be perturbed, and the perturbed flux linkage is converted to voltage at sensor output port. For the metal sphere, having radius a, which is x meters from the center of antenna conductor, the field intensity becomes Hx=I/2πx, and accordingly the flux density at the distance x is Bx=μI/2πx webers/m2. Thus flux linkage by metal sphere becomes as in (12), and this amount perturbs the mutual inductances in steady state:
(12)ψx=∑i=144πa2μIi2πxi.


## 2.1. Single Channel Model

The conventional metal detection sensor with sensitivity resolution in mm scale has the antenna set, one transmitting antenna and two receiving antennas which are connected in opposite polarity to cancel reception signal while in steady state. In case when an object containing a nonspherical metal piece is fed through hollow antenna cross-sectional space as shown in Figure1, then the sensor shows good sensitivity only for one directional position, between metal piece and antenna, where the perturbation in electromagnetic flux linkages becomes maximum. In the single channel model, the moving object containing metal piece perturbs gradually from first electromagnetic flux linkages between TX antenna #1 and RX antenna #1 to second electromagnetic flux linkages between TX antenna #1 and RX antenna #2. The amounts of these spatially varying electromagnetic flux linkages induce currents into RX antennas #1 and #2, and the current difference between RX antennas #1 and #2 becomes output current, which represent the electromagnetic flux unbalance of antenna set #1.Figure 1
Conventional antenna set of metal detection sensor.The equivalent circuit of an antenna set, one transmitting and two receiving antennas, is shown as in Figure2. The instantaneous output voltage v10, in no load condition, can be expressed as the difference of mutual inductance, M1-M2, between transmitting and respective receiving antenna as shown in (1), and is also proportional to exciting frequency as shown in (3). In this model, the distance between transmitting antenna and receiving antenna is closer than the distance to passing object containing metal piece; thus antenna inductances are larger than mutual inductance, M11 and M12. If transmitting antenna is excited using sinusoidal signal, e1s=e10sin(ωt+δ), then antenna current becomes as shown in (2). Consider
(1)v10=v11-v12=(M11-M12)dip1dt,(2)ip1=jωLp1e10(ϖLp1)2+Rp12sin(ωt+δ),(3)v10=jω2Lp1e10(M11-M12)(ϖLp1)2+Rp12cos⁡(ωt+δ).Equivalent circuit of antenna set: (a) schematic diagram and (b) equivalent circuit.
(a)
(b)When the phasor expression is used for the flux linkageψ, then the phasor voltage V due to flux linkage can be expressed as in (4) where I denotes phasor current:
(4)V10=jωψ10=jω(M11-M12)Ip1.It is noted that mutual inductance variance plays a key role in determining sensitivity of metal detection sensor. The mutual inductance is expressed as in (5), in which k11 and k12 represent coupling coefficient between transmitting and receiving antennas, respectively. And these coupling coefficients have the value 0≤k11, k12≤1:
(5)M11=k11Lp1Ls1/2,M12=k12Lp1Ls1/2.In steady state of initial measurement,M11 and M12 are adjusted to M11=M12, and output voltage becomes v10≈0. When ω is higher and M11-M12 are bigger for the same size of metal piece, then it is advantageous in terms of sensitivity.


## 2.2. Two-Channel Model

In the two antenna sets as shown in Figure3, the moving object after passing antenna set #1 perturbs gradually from third electromagnetic flux linkages between TX antenna #2 and RX antenna #4 to fourth electromagnetic flux linkages between TX antenna #2 and RX antenna #3. Also the amounts of spatially varying electromagnetic flux linkages induce currents into RX antennas #4 and #3, and the current difference between RX antennas #4 and #3 becomes output current of antenna set #2.Figure 3
Two antenna sets of metal detection sensor.It is difficult to calculate the variance of mutual inductance for the moving object; thus experimental method is attempted. By using the model in Figure4, the output voltage in each antenna set becomes the product of mutual inductance matrix and instantaneous current of each transmitting antenna as in
(6)[V10V20]=jω[M11-M12M21-M22M13-M14M23-M24][Ip1Ip2].Figure 4
Sensor layout for two antenna sets.AssumeIT11 is phasor current in one conductor of TX antenna #1, D is the distance, P in subscript is the remote point outside antenna, T in first subscript alphabet is transmitting antenna, R in first subscript alphabet is receiving antenna, the number in second subscript numeric is antenna number, the number in third subscript numeric is conductor number of antenna, and 4th through 6th alphabet and numeric follow the same convention as in 1st through 3rd alphabet and numeric. Then DR11T11 is the distance between one conductor of RX antenna #1 and one conductor of TX antenna #1, and DT11P is the distance between one conductor of TX antenna #1 and a remote point P. The flux linkage ψR11T11 with one conductor of RX antenna #1 due to one conductor of TX antenna #1 can be expressed as in
(7)ψR11T11=2×10-7(IT11ln⁡DT11PDR11T11).If we consider flux linkage to one conductor of receiving antenna #1 from two transmitter antennas, this flux linkageψR11 can be expressed as in
(8)ψR11=ψR11T11+ψR11T12+ψR11T21+ψR11T22=2×10-7(IT11ln⁡DT11PDR11T11+IT12ln⁡DT12PDR11T12+IT21ln⁡DT21PDR11T21+IT22ln⁡DT22PDR11T22)=2×10-7(IT11ln⁡1DR11T11+IT12ln⁡1DR11T12+IT21ln⁡1DR11T21+IT22ln⁡1DR11T22+IT11ln⁡DT11P+IT12ln⁡DT12P+IT21ln⁡DT21P+IT22ln⁡DT22P1DR11T11).In this configuration, the sum of two currents in TX antenna #1 is zero,IT11+IT12=0; also likewise IT21+IT22=0 for TX antenna #2. Let the point P move infinitely far away so that the set of terms containing logarithms of ratios of distances from P becomes infinitesimal; then the ratio of the distances approaches 1. Substituting these into (8) and recombining some logarithmic terms, we have (9) with the unit weber-turns/meter:
(9)ψR11=2×10-7(IT11ln⁡DR11T12DR11T11+IT21ln⁡DR11T22DR11T21).Thus flux linkageψR1 in RX antenna #1 becomes sum of ψR11 and ψR12 as shown in
(10)ψR1=2×10-7(IT11ln⁡DR11T12DR11T11+IT11ln⁡DR12T12DR12T11+IT21ln⁡DR11T22DR11T21+IT21ln⁡DR12T22DR12T21)=2×10-7((ln⁡DR11T12DR11T11+ln⁡DR12T12DR12T11)IT11+(ln⁡DR11T22DR11T21+ln⁡DR12T22DR12T21)IT21)=4×10-7(ln⁡DR11T12DR12T12DR11T11DR12T11IT11+ln⁡DR11T22DR12T22DR11T21DR12T21IT21).Likewise all mutual inductances includingM11 and M21 are expressed in a similar way as is shown in
(11)M11=4×10-7ln⁡DR11T12DR12T12DR11T11DR12T11,M21=4×10-7ln⁡DR11T22DR12T22DR11T21DR12T21,M12=4×10-7ln⁡DR21T12DR22T12DR21T11DR22T11,M22=4×10-7ln⁡DR21T22DR22T22DR21T21DR22T21,M13=4×10-7ln⁡DR31T12DR32T12DR31T11DR32T11,M23=4×10-7ln⁡DR31T22DR32T22DR31T21DR32T21,M14=4×10-7ln⁡DR41T12DR42T12DR41T11DR42T11,M24=4×10-7ln⁡DR41T22DR42T22DR41T21DR42T21.When a foreign object, for example, a metal cube, passes through the above flux linkage, then the above mutual inductanceM will be perturbed, and the perturbed flux linkage is converted to voltage at sensor output port. For the metal sphere, having radius a, which is x meters from the center of antenna conductor, the field intensity becomes Hx=I/2πx, and accordingly the flux density at the distance x is Bx=μI/2πx webers/m2. Thus flux linkage by metal sphere becomes as in (12), and this amount perturbs the mutual inductances in steady state:
(12)ψx=∑i=144πa2μIi2πxi.


## 3. Signal Detection Method

### 3.1. Noise Rejection Using BPF

Two-channel metal detection sensor uses two different frequencies between antenna sets #1 and #2 to avoid interference. In frequency domain, this interference can be minimized by raising the frequency selectivity of receiver. Assume the characteristic of band-pass filter (BPF) in receiver #1 is|HR1(f)| and |HR2(f)| for receiver #2 and power spectral density of incoming signal is S1In⁡(f) for receiver #1 and S2In⁡(f) for receiver #2. Then power spectral densities S1BPF(f) of receiver #1 and S2BPF(f) of receiver #2 become as in
(13)[S1BPF(f)S2BPF(f)]=[|HR1(f)|2|HR1(f)|2|HR2(f)|2|HR2(f)|2][S1In⁡(f)S2In⁡(f)].As the bandwidth of BPF becomes narrower, the system will be more immune to ambient noise. However this will also increase instability in maintaining center frequency of BPF because component values are subject to change along with temperature change. So there exists the optimumQ value of BPF, from the practical point of view, which is needed to be determined by experiment.


### 3.2. Noise Rejection Using PSD

The input signal after BPF is fed into phase sensitive detector (PSD) to increase selectivity against interfering noise as in Figure5. In time domain, the output signal from two receiving antennas, which is connected to cancel each other, is fed to receiver as VIn⁡. After BPF, it is filtered to VBPF, and the product of VBPF with VREF is again filtered through LPF resulting in VLPF. In case the input signal VIn⁡ is the mixture of signals from transmitting antennas #1 and #2 and noise n(t), then VIn⁡ is expressed as in (14) and VOP as in (15). Hence,
(14)VIn⁡=E1sin(ω1t+θ1)+E2sin(ω2t+θ2)+n(t),(15)VBPF=VIn⁡*hBPF(t)=[E1sin(ω1t+θ1)+E2sin(ω2t+θ2)+n(t)E1sin(ω1t+θ1)+E2sin(ω2t+θ2)]*hBPF(t),VOP=VBPF×VREF=EREFsin(ω1t+θ1)×[E1sin(ω1t+θ1)*hBPF(t)+E2sin(ω2t+θ2)*hBPF(t)+n(t)*hBPF(t)E1].
In case the band-pass filter is ideally tuned to ω1 and low-pass filter ideally cut off unnecessary frequency component, then the output of sensor signal detector VLPF becomes as in (16). This output signal VLPF in (16) shows DC signal level which is proportional to receiver input signal with minimum interference:
(16)VLPF=VOP*hLPF(t)=EREFsin(ω1t+θ1)×[E1sin(ω1t+θ1)*hBPF(t)+E2sin(ω2t+θ2)*hBPF(t)+n(t)*hBPF(t)]*hLPF(t)≈EREFE12+α·n(t).Figure 5
Block diagram of sensor signal detector.In case the interfering signal has the same frequency as sensor detection signal, but with different phase relationship, then the signal output after LPF in Figure5 will be shifted in DC level, depending on the degree of interference, in an ideal case.


## 3.1. Noise Rejection Using BPF

Two-channel metal detection sensor uses two different frequencies between antenna sets #1 and #2 to avoid interference. In frequency domain, this interference can be minimized by raising the frequency selectivity of receiver. Assume the characteristic of band-pass filter (BPF) in receiver #1 is|HR1(f)| and |HR2(f)| for receiver #2 and power spectral density of incoming signal is S1In⁡(f) for receiver #1 and S2In⁡(f) for receiver #2. Then power spectral densities S1BPF(f) of receiver #1 and S2BPF(f) of receiver #2 become as in
(13)[S1BPF(f)S2BPF(f)]=[|HR1(f)|2|HR1(f)|2|HR2(f)|2|HR2(f)|2][S1In⁡(f)S2In⁡(f)].As the bandwidth of BPF becomes narrower, the system will be more immune to ambient noise. However this will also increase instability in maintaining center frequency of BPF because component values are subject to change along with temperature change. So there exists the optimumQ value of BPF, from the practical point of view, which is needed to be determined by experiment.


## 3.2. Noise Rejection Using PSD

The input signal after BPF is fed into phase sensitive detector (PSD) to increase selectivity against interfering noise as in Figure5. In time domain, the output signal from two receiving antennas, which is connected to cancel each other, is fed to receiver as VIn⁡. After BPF, it is filtered to VBPF, and the product of VBPF with VREF is again filtered through LPF resulting in VLPF. In case the input signal VIn⁡ is the mixture of signals from transmitting antennas #1 and #2 and noise n(t), then VIn⁡ is expressed as in (14) and VOP as in (15). Hence,
(14)VIn⁡=E1sin(ω1t+θ1)+E2sin(ω2t+θ2)+n(t),(15)VBPF=VIn⁡*hBPF(t)=[E1sin(ω1t+θ1)+E2sin(ω2t+θ2)+n(t)E1sin(ω1t+θ1)+E2sin(ω2t+θ2)]*hBPF(t),VOP=VBPF×VREF=EREFsin(ω1t+θ1)×[E1sin(ω1t+θ1)*hBPF(t)+E2sin(ω2t+θ2)*hBPF(t)+n(t)*hBPF(t)E1].
In case the band-pass filter is ideally tuned to ω1 and low-pass filter ideally cut off unnecessary frequency component, then the output of sensor signal detector VLPF becomes as in (16). This output signal VLPF in (16) shows DC signal level which is proportional to receiver input signal with minimum interference:
(16)VLPF=VOP*hLPF(t)=EREFsin(ω1t+θ1)×[E1sin(ω1t+θ1)*hBPF(t)+E2sin(ω2t+θ2)*hBPF(t)+n(t)*hBPF(t)]*hLPF(t)≈EREFE12+α·n(t).Figure 5
Block diagram of sensor signal detector.In case the interfering signal has the same frequency as sensor detection signal, but with different phase relationship, then the signal output after LPF in Figure5 will be shifted in DC level, depending on the degree of interference, in an ideal case.


## 4. System Design

### 4.1. Metal Detection Sensor Having Sensitivity in mm Scale

Three frequencies, as 50 kHz, 200 kHz, and 400 kHz, were designed to be injected into the experimental sensor setup, having sensitivity in mm scale, to investigate frequency dependant sensitivity while in simultaneous operation with the sensor having sensitivity in cm scale. Antenna set #1 was contained in metal enclosure having outer dimension ofW55×H29×D23 cm with the opening and W30×H10×D23 cm for sensing entry to shield outer interfering noise as was shown in Figure 6. Single turn antennas were used for easy balancing between antennas.Figure 6
Photo of outer metal enclosure shielding antenna set.The output voltage from receiving antenna pair, which was connected in opposite polarity, was adjusted to produce nearly zero voltage by using two screws as shown in Figure7. And the degree of null output signal was measured as CMRR (common mode rejection ratio). After adjusting null position, internal cavity of antenna set #1 was filled with epoxy to be resistant to outer shock or vibration.Figure 7
Adjusting screws to produce zero voltage for antenna set #1.The transmitter block diagram for antenna set #1 is shown in Figure8. The 8 MHz crystal oscillator was used for temperature stability, and fundamental frequency was divided into desired frequencies. Time division switch was facilitated to select single or mixed frequencies. A part of this transmitter signal was fed into phase sensitive detector of receiver as synchronous trigger signal source. Antenna matching circuit was used to match antenna impedance with transmitter impedance.Figure 8
Block diagram of transmitter for antenna set #1.The receiver block diagram for antenna set #1 is shown in Figure9. The input signal from receiving antenna pair was fed into antenna matching circuit not only for impedance matching but also for boosting voltage. After amplification in PRE AMP block and filtering interfering signal in BPF block, the phase of input signal was compared with synchronous trigger signal in PSD block. Finally high frequency component was filtered out in LPF block, and only DC component, proportional to phase difference, appeared and was amplified in AMP block as signal output. The microprocessor was used to control frequency selection and other control parameters in MICOM block.Figure 9
Block diagram of receiver for antenna set #1.


### 4.2. Metal Detection Sensor Having Sensitivity in cm Scale

Single 20 kHz frequency was injected into the experimental sensor setup, having sensitivity in cm scale, to investigate interfering effect with the former sensor, having sensitivity in mm scale, while in simultaneous operation. The arrangement of antenna set #2 was devised to be perpendicular with antenna set #1 to avoid interference. Multiturn antennas were used to compensate sensitivity deficiency due to relatively long distance between transmitting and receiving antennas as shown in Figure10. Transmitting antenna was fabricated by using CNC machine to obtain sufficient thickness and reduce resistance, and receiving antennas were fabricated by patterning on PCB. Receiving antenna pair is connected in opposite polarity and adjusted to near zero offset.Photo of antenna set #2: (a) transmitting antenna and (b) receiving antennas.
(a)
(b)The transmitter block diagram is shown in Figure11. The exciting frequency was adjustable by using potentiometer to select frequency for optimum operation.Figure 11
Block diagram of transmitter for antenna set #2.In the receiver side as shown in Figure12, the input signal from receiving antenna pair was directly amplified in PRE AMP block without antenna matching circuit. After filtering interference signal in BPF block, the phase of input signal was compared with synchronous trigger signal from transmitter in PSD block. Finally high frequency component was filtered out in LPF block and amplified in AMP block as signal output. Only DC component, proportional to phase difference between input signal and synchronous trigger signal, appeared as signal output.Figure 12
Block diagram of receiver for antenna set #2.


## 4.1. Metal Detection Sensor Having Sensitivity in mm Scale

Three frequencies, as 50 kHz, 200 kHz, and 400 kHz, were designed to be injected into the experimental sensor setup, having sensitivity in mm scale, to investigate frequency dependant sensitivity while in simultaneous operation with the sensor having sensitivity in cm scale. Antenna set #1 was contained in metal enclosure having outer dimension ofW55×H29×D23 cm with the opening and W30×H10×D23 cm for sensing entry to shield outer interfering noise as was shown in Figure 6. Single turn antennas were used for easy balancing between antennas.Figure 6
Photo of outer metal enclosure shielding antenna set.The output voltage from receiving antenna pair, which was connected in opposite polarity, was adjusted to produce nearly zero voltage by using two screws as shown in Figure7. And the degree of null output signal was measured as CMRR (common mode rejection ratio). After adjusting null position, internal cavity of antenna set #1 was filled with epoxy to be resistant to outer shock or vibration.Figure 7
Adjusting screws to produce zero voltage for antenna set #1.The transmitter block diagram for antenna set #1 is shown in Figure8. The 8 MHz crystal oscillator was used for temperature stability, and fundamental frequency was divided into desired frequencies. Time division switch was facilitated to select single or mixed frequencies. A part of this transmitter signal was fed into phase sensitive detector of receiver as synchronous trigger signal source. Antenna matching circuit was used to match antenna impedance with transmitter impedance.Figure 8
Block diagram of transmitter for antenna set #1.The receiver block diagram for antenna set #1 is shown in Figure9. The input signal from receiving antenna pair was fed into antenna matching circuit not only for impedance matching but also for boosting voltage. After amplification in PRE AMP block and filtering interfering signal in BPF block, the phase of input signal was compared with synchronous trigger signal in PSD block. Finally high frequency component was filtered out in LPF block, and only DC component, proportional to phase difference, appeared and was amplified in AMP block as signal output. The microprocessor was used to control frequency selection and other control parameters in MICOM block.Figure 9
Block diagram of receiver for antenna set #1.


## 4.2. Metal Detection Sensor Having Sensitivity in cm Scale

Single 20 kHz frequency was injected into the experimental sensor setup, having sensitivity in cm scale, to investigate interfering effect with the former sensor, having sensitivity in mm scale, while in simultaneous operation. The arrangement of antenna set #2 was devised to be perpendicular with antenna set #1 to avoid interference. Multiturn antennas were used to compensate sensitivity deficiency due to relatively long distance between transmitting and receiving antennas as shown in Figure10. Transmitting antenna was fabricated by using CNC machine to obtain sufficient thickness and reduce resistance, and receiving antennas were fabricated by patterning on PCB. Receiving antenna pair is connected in opposite polarity and adjusted to near zero offset.Photo of antenna set #2: (a) transmitting antenna and (b) receiving antennas.
(a)
(b)The transmitter block diagram is shown in Figure11. The exciting frequency was adjustable by using potentiometer to select frequency for optimum operation.Figure 11
Block diagram of transmitter for antenna set #2.In the receiver side as shown in Figure12, the input signal from receiving antenna pair was directly amplified in PRE AMP block without antenna matching circuit. After filtering interference signal in BPF block, the phase of input signal was compared with synchronous trigger signal from transmitter in PSD block. Finally high frequency component was filtered out in LPF block and amplified in AMP block as signal output. Only DC component, proportional to phase difference between input signal and synchronous trigger signal, appeared as signal output.Figure 12
Block diagram of receiver for antenna set #2.


## 5. Measurement

### 5.1. Metal Detection Sensor Having Sensitivity in mm Scale

For this sensing channel, the sensitivity is the key part of the sensor. The minimum size of detectable metal piece is related to the degree of canceling signals from receiving antenna pair, because this limits the maximum amplification ratio. And this figure of merit (FOM) is represented by CMRR, which is the logarithmic value of differential output, 2 mVpp (before amplification), over single channel output, 10 Vpp. The measured CMRR was −74 dB as shown in
(17)CMRR[dB]=20log⁡(0.2V/gain10V)=-74[dB].The dependency of output voltage on ferrous metal size was investigated, using ferrous test balls having diameter of 0.8 mm, 1.0 mm, and 1.2 mm at 50 kHz exciting frequency and 33 Hz LPF (low-pass filter) cutoff frequency after PSD (phase sensitive detector). Measurement data showed that output voltage was almost linearly proportional to the volume as in Figure13. The minimum detectable size was up to the diameter of 0.8 mm using 33 Hz LPF (low-pass filter) cutoff frequency.Figure 13
Signal output versus Fe ball volume.The dependency of output voltage on applying frequency (50 kHz, 200 kHz, and 400 kHz) was investigated using Fe ball of 1.2 mm diameter as shown in Figure14. Measurement data showed that output voltage was increasing with applying frequency, and this was closely matched if we multiplied the frequency characteristics of antenna matching circuit to the theoretically expected value.Figure 14
Signal output versus applying frequency using Fe ball,D=1.2 mm.The metal detection sensor using differential loop antennas usually suffers a nonuniform sensitivity distribution inside hollow center area of coil which is used for sample passage due to the nature of loop coil. It is necessary, ideally, to maintain equal sensitivity throughout sensing area. Otherwise the sample metal ball will be undetectable when passing the center area, even if it was detectable when passing edge area. Therefore it is necessary to compensate sensitivity distribution for close to equal sensitivity as possible. The sensitivity distribution was measured for the above sensing entry,W300mm×H100 mm, by applying 50 kHz and using Fe test ball of 1.2 mm diameter as shown in Figure 15(a). Two small copper plates on center of receiving antenna coil, in horizontal direction, were patched to compensate sensitivity in sensing entry by providing more electromagnetic flux linkages. Measurement data showed that the sensitivity was −6 dB at the center of sensing entry as shown in Figure 15(b), which was +4 dB enhancement in comparison to the case without patches.Sensitivity plot of sensing entry (output voltage versus position in sensing entry using FeD=1.2 mm ball): (a) before patching and (b) after patching.
(a)
(b)The bandwidth of LPF after PSD is critical for sensitivity enhancement. In the conventional LPF, the narrower the bandwidth is, the lower the noise level is. However, for the metal sensor for moving object detection, the sensitivity is degraded if the bandwidth of LPF is too narrow, because frequency component due to moving object is attenuated. On the contrary, the noise level soars if the bandwidth of LPF is too wide, resulting in degraded SNR (signal to noise ratio). Also the improved SNR by narrowing the bandwidth of LPF does not mean increasing sensitivity unless it is amplified. Therefore the signal of this ultrahigh sensitivity metal sensor, operating close to detection limit, is only able to be amplified after lowering noise level without sacrificing usable frequency component of moving object. The effect of LPF bandwidth was measured, by varying cutoff frequency, to find optimum sensitivity when exciting frequency of 50 kHz is applied. During the experiment, the signal was amplified for the level which was equivalent to decreasing noise floor, while keeping overall system gain, because there did not exist a margin for signal amplification due to inherent noise level for ultrahigh sensitivity metal sensor operating close to detection limit. The cutoff frequencies of LPF, from 33 Hz to lower than 11 Hz, were attempted, and the frequency below 11 Hz resulted in weaker signal output due to too deep attenuation of signal frequency component. The cutoff frequency of 11 Hz showed the best performance for the moving object which was similar to practical application. The signal responses at 11 Hz cutoff frequency together with 33 Hz cutoff frequency are shown in Figure16 for comparison purpose.Figure 16
The effect of cutoff frequency of LPF forD=1.2 mm ferrous test ball, Y=200 mV/div, X=100 ms/div.Further test is conducted by applying 50 kHz for ferrous test sample ball having 0.8 mm and 0.7 mm diameter using the same LPFfco⁡=11 Hz to find detection limit as shown in Figure 17. Measurement showed that this metal sensor was able to detect ferrous test sample ball down to 0.7 mm diameter. Thus the minimum detectable size of Fe ball was extended from 0.8 mm diameter to 0.7 mm diameter by optimizing the cutoff frequency of LPF.Detection limit of metal sensor: (a)D=0.8 mm ferrous test ball (Y=50 mV/div, X=200 ms/div), (b) D=0.7 mm ferrous test ball (Y=20 mV/div, X=200 ms/div).
(a)
(b)


### 5.2. Metal Detection Sensor Having Sensitivity in cm Scale

Measured data showed that the previous ultrahigh sensitivity metal sensor had the linear response range of about 0.7 mm~4 mm of Fe ball diameter when the exciting frequency was 50 kHz and cutoff frequency of LPF was 11 Hz. Over this size limit, the sensor detects the presence of metal, but the output response becomes saturated and unable to set further threshold point for different size of Fe test ball. Of course, the detectable size can be altered by varying the sensor gain; however the detection range remains similar to the above. The metal sensor having sensitivity in cm scale was devised with the flexibility to locate the other sensor in adjacent axis to compensate direction dependent sensitivity. Thus this sensor enables sensing throughout wide range of metal sizes from mm to cm scale, if it is combined with the previous ultrahigh sensitivity metal sensor.The single channel response was measured, with reduced gain, to characterize the frequency characteristics of sensor by using TX antenna #2 and RX antenna #3, as shown in Figure18. In the experiment test metal plate occupying 66% of antenna surface was inserted to find the effect of metal in sensitivity through projected frequency range. The high peak around 50 kHz was observed, and this was regarded as frequency matching characteristics between antenna and transmitter. However the effect of metal piece was similar within the range 40~60%, which was defined as output voltage after inserting versus output voltage before inserting, as shown in Figure 19. It is noted that the sensitivity is increasing along with the frequency increase as expected, even if the absolute value of output voltage is decreasing in higher frequency region due to frequency matching characteristics.Figure 18
Signal output of receiver #2 for single channel using RX antenna #3,X = frequency, Y = A.U.Figure 19
Effect of frequency in metal sensing, output voltage after inserting versus before inserting,X = frequency, Y = A.U.The effect of distance “d” between transmitting antenna and receiving antenna was investigated by separating the distance by two times, and the ratio was calculated, the output voltage at L=2d over the output voltage at L=d, as shown in Figure 20. The measured result shows the tendency, close to the rule of ∝1/d2. The deviation between the ideal data and measured data is regarded due to leaked electromagnetic fluxes as the distance is farther.Figure 20
Effect of distance between transmitting and receiving antennas,X = frequency, Y = A.U.The sensitivity distribution, in horizontal direction, was investigated by gradually covering the antenna along the midline between transmitting antenna and receiving antenna with test metal plate. The measured data showed fairly good horizontal linearity, only 6.5% nonlinearity. The sensitivity variation, in vertical direction, was measured as ~13% along the 20~80% line connecting between transmitting antenna and receiving antenna. This implies that the loop antenna configuration facing each other provides more uniform distribution in sensitivity.Following the single channel experiment, two receiving antennas were connected in differential mode, and the gain was increased accordingly. The CMRR was measured in a similar way to the former sensor channel and was calculated as –52 dB, less than 22 dB in comparison to the former sensor. Thus this sensor channel is regarded as adequate for metal object having dimension in cm scale. Ferrous test sample balls having dimension of10×5×5 (mm) were tested to find the sensitivity in 3 axes. And the result is summarized in Table 1. If we extend the concept of antenna configuration in horizontal direction instead of the present vertical direction, then we can obtain rotated sensitivity distribution. In case we cascade these two antenna configurations, then we are able to obtain more uniform sensitivity distribution by compensating the sensitivity to each other.Table 1
Sensitivity comparison along with test sample laying direction.
Sensitivity
Direction
X direction(mV)
Y direction(mV)
Z direction(mV)
Peak output voltage (A.U.)
110
80
210


### 5.3. Simultaneous Operation of Two Sensors

The objective of this research is to obtain wide range of sensor responses throughout the object from mm scale to cm scale by cascading two sensors having different sensitivity and distribution. However metal detection sensor, operating in differential mode, maintains extremely high gain to increase sensitivity; thus it is strongly influenced by nearby electromagnetic waves. Therefore the effect from the other sensor is mainly investigated through measurement using the present experimental setup to examine the feasibility of this concept. Since the experimental setup was extremely sensitive to outside vibration and electromagnetic waves, all antennas were firmly mounted, adjusted, and fixed using epoxy resin; thus it was not feasible to change parameters such as dimensions and distances. The response from the sensor having sensitivity in mm scale showed lower response of ~30% as shown in Figure21, while in simultaneous operation with the sensor having sensitivity in cm scale, in comparison to standalone operation. This is considered from the characteristics of PSD because the output from PSD has the tendency of decreasing along with the increasing outside noise. However it was not possible to decouple each effect individually, such as BPF effect, shielding effect, and PSD effect, due to the delicately integrated sensor system.Figure 21
Effect of simultaneous operation of two sensors.On the contrary case, the response from the sensor having sensitivity in cm scale showed a little less response of ~85%, while in simultaneous operation with the sensor having sensitivity in mm scale, in comparison to standalone operation. This is considered also from the characteristics of PSD, but with less effect due to lower gain level of the sensor having sensitivity in cm scale.


## 5.1. Metal Detection Sensor Having Sensitivity in mm Scale

For this sensing channel, the sensitivity is the key part of the sensor. The minimum size of detectable metal piece is related to the degree of canceling signals from receiving antenna pair, because this limits the maximum amplification ratio. And this figure of merit (FOM) is represented by CMRR, which is the logarithmic value of differential output, 2 mVpp (before amplification), over single channel output, 10 Vpp. The measured CMRR was −74 dB as shown in
(17)CMRR[dB]=20log⁡(0.2V/gain10V)=-74[dB].The dependency of output voltage on ferrous metal size was investigated, using ferrous test balls having diameter of 0.8 mm, 1.0 mm, and 1.2 mm at 50 kHz exciting frequency and 33 Hz LPF (low-pass filter) cutoff frequency after PSD (phase sensitive detector). Measurement data showed that output voltage was almost linearly proportional to the volume as in Figure13. The minimum detectable size was up to the diameter of 0.8 mm using 33 Hz LPF (low-pass filter) cutoff frequency.Figure 13
Signal output versus Fe ball volume.The dependency of output voltage on applying frequency (50 kHz, 200 kHz, and 400 kHz) was investigated using Fe ball of 1.2 mm diameter as shown in Figure14. Measurement data showed that output voltage was increasing with applying frequency, and this was closely matched if we multiplied the frequency characteristics of antenna matching circuit to the theoretically expected value.Figure 14
Signal output versus applying frequency using Fe ball,D=1.2 mm.The metal detection sensor using differential loop antennas usually suffers a nonuniform sensitivity distribution inside hollow center area of coil which is used for sample passage due to the nature of loop coil. It is necessary, ideally, to maintain equal sensitivity throughout sensing area. Otherwise the sample metal ball will be undetectable when passing the center area, even if it was detectable when passing edge area. Therefore it is necessary to compensate sensitivity distribution for close to equal sensitivity as possible. The sensitivity distribution was measured for the above sensing entry,W300mm×H100 mm, by applying 50 kHz and using Fe test ball of 1.2 mm diameter as shown in Figure 15(a). Two small copper plates on center of receiving antenna coil, in horizontal direction, were patched to compensate sensitivity in sensing entry by providing more electromagnetic flux linkages. Measurement data showed that the sensitivity was −6 dB at the center of sensing entry as shown in Figure 15(b), which was +4 dB enhancement in comparison to the case without patches.Sensitivity plot of sensing entry (output voltage versus position in sensing entry using FeD=1.2 mm ball): (a) before patching and (b) after patching.
(a)
(b)The bandwidth of LPF after PSD is critical for sensitivity enhancement. In the conventional LPF, the narrower the bandwidth is, the lower the noise level is. However, for the metal sensor for moving object detection, the sensitivity is degraded if the bandwidth of LPF is too narrow, because frequency component due to moving object is attenuated. On the contrary, the noise level soars if the bandwidth of LPF is too wide, resulting in degraded SNR (signal to noise ratio). Also the improved SNR by narrowing the bandwidth of LPF does not mean increasing sensitivity unless it is amplified. Therefore the signal of this ultrahigh sensitivity metal sensor, operating close to detection limit, is only able to be amplified after lowering noise level without sacrificing usable frequency component of moving object. The effect of LPF bandwidth was measured, by varying cutoff frequency, to find optimum sensitivity when exciting frequency of 50 kHz is applied. During the experiment, the signal was amplified for the level which was equivalent to decreasing noise floor, while keeping overall system gain, because there did not exist a margin for signal amplification due to inherent noise level for ultrahigh sensitivity metal sensor operating close to detection limit. The cutoff frequencies of LPF, from 33 Hz to lower than 11 Hz, were attempted, and the frequency below 11 Hz resulted in weaker signal output due to too deep attenuation of signal frequency component. The cutoff frequency of 11 Hz showed the best performance for the moving object which was similar to practical application. The signal responses at 11 Hz cutoff frequency together with 33 Hz cutoff frequency are shown in Figure16 for comparison purpose.Figure 16
The effect of cutoff frequency of LPF forD=1.2 mm ferrous test ball, Y=200 mV/div, X=100 ms/div.Further test is conducted by applying 50 kHz for ferrous test sample ball having 0.8 mm and 0.7 mm diameter using the same LPFfco⁡=11 Hz to find detection limit as shown in Figure 17. Measurement showed that this metal sensor was able to detect ferrous test sample ball down to 0.7 mm diameter. Thus the minimum detectable size of Fe ball was extended from 0.8 mm diameter to 0.7 mm diameter by optimizing the cutoff frequency of LPF.Detection limit of metal sensor: (a)D=0.8 mm ferrous test ball (Y=50 mV/div, X=200 ms/div), (b) D=0.7 mm ferrous test ball (Y=20 mV/div, X=200 ms/div).
(a)
(b)


## 5.2. Metal Detection Sensor Having Sensitivity in cm Scale

Measured data showed that the previous ultrahigh sensitivity metal sensor had the linear response range of about 0.7 mm~4 mm of Fe ball diameter when the exciting frequency was 50 kHz and cutoff frequency of LPF was 11 Hz. Over this size limit, the sensor detects the presence of metal, but the output response becomes saturated and unable to set further threshold point for different size of Fe test ball. Of course, the detectable size can be altered by varying the sensor gain; however the detection range remains similar to the above. The metal sensor having sensitivity in cm scale was devised with the flexibility to locate the other sensor in adjacent axis to compensate direction dependent sensitivity. Thus this sensor enables sensing throughout wide range of metal sizes from mm to cm scale, if it is combined with the previous ultrahigh sensitivity metal sensor.The single channel response was measured, with reduced gain, to characterize the frequency characteristics of sensor by using TX antenna #2 and RX antenna #3, as shown in Figure18. In the experiment test metal plate occupying 66% of antenna surface was inserted to find the effect of metal in sensitivity through projected frequency range. The high peak around 50 kHz was observed, and this was regarded as frequency matching characteristics between antenna and transmitter. However the effect of metal piece was similar within the range 40~60%, which was defined as output voltage after inserting versus output voltage before inserting, as shown in Figure 19. It is noted that the sensitivity is increasing along with the frequency increase as expected, even if the absolute value of output voltage is decreasing in higher frequency region due to frequency matching characteristics.Figure 18
Signal output of receiver #2 for single channel using RX antenna #3,X = frequency, Y = A.U.Figure 19
Effect of frequency in metal sensing, output voltage after inserting versus before inserting,X = frequency, Y = A.U.The effect of distance “d” between transmitting antenna and receiving antenna was investigated by separating the distance by two times, and the ratio was calculated, the output voltage at L=2d over the output voltage at L=d, as shown in Figure 20. The measured result shows the tendency, close to the rule of ∝1/d2. The deviation between the ideal data and measured data is regarded due to leaked electromagnetic fluxes as the distance is farther.Figure 20
Effect of distance between transmitting and receiving antennas,X = frequency, Y = A.U.The sensitivity distribution, in horizontal direction, was investigated by gradually covering the antenna along the midline between transmitting antenna and receiving antenna with test metal plate. The measured data showed fairly good horizontal linearity, only 6.5% nonlinearity. The sensitivity variation, in vertical direction, was measured as ~13% along the 20~80% line connecting between transmitting antenna and receiving antenna. This implies that the loop antenna configuration facing each other provides more uniform distribution in sensitivity.Following the single channel experiment, two receiving antennas were connected in differential mode, and the gain was increased accordingly. The CMRR was measured in a similar way to the former sensor channel and was calculated as –52 dB, less than 22 dB in comparison to the former sensor. Thus this sensor channel is regarded as adequate for metal object having dimension in cm scale. Ferrous test sample balls having dimension of10×5×5 (mm) were tested to find the sensitivity in 3 axes. And the result is summarized in Table 1. If we extend the concept of antenna configuration in horizontal direction instead of the present vertical direction, then we can obtain rotated sensitivity distribution. In case we cascade these two antenna configurations, then we are able to obtain more uniform sensitivity distribution by compensating the sensitivity to each other.Table 1
Sensitivity comparison along with test sample laying direction.
Sensitivity
Direction
X direction(mV)
Y direction(mV)
Z direction(mV)
Peak output voltage (A.U.)
110
80
210


## 5.3. Simultaneous Operation of Two Sensors

The objective of this research is to obtain wide range of sensor responses throughout the object from mm scale to cm scale by cascading two sensors having different sensitivity and distribution. However metal detection sensor, operating in differential mode, maintains extremely high gain to increase sensitivity; thus it is strongly influenced by nearby electromagnetic waves. Therefore the effect from the other sensor is mainly investigated through measurement using the present experimental setup to examine the feasibility of this concept. Since the experimental setup was extremely sensitive to outside vibration and electromagnetic waves, all antennas were firmly mounted, adjusted, and fixed using epoxy resin; thus it was not feasible to change parameters such as dimensions and distances. The response from the sensor having sensitivity in mm scale showed lower response of ~30% as shown in Figure21, while in simultaneous operation with the sensor having sensitivity in cm scale, in comparison to standalone operation. This is considered from the characteristics of PSD because the output from PSD has the tendency of decreasing along with the increasing outside noise. However it was not possible to decouple each effect individually, such as BPF effect, shielding effect, and PSD effect, due to the delicately integrated sensor system.Figure 21
Effect of simultaneous operation of two sensors.On the contrary case, the response from the sensor having sensitivity in cm scale showed a little less response of ~85%, while in simultaneous operation with the sensor having sensitivity in mm scale, in comparison to standalone operation. This is considered also from the characteristics of PSD, but with less effect due to lower gain level of the sensor having sensitivity in cm scale.


## 6. Conclusion

The characteristics of metal detection sensor having two sets of perpendicularly oriented sensor antennas were investigated to extend the sensing range from mm scale to cm scale with less interference by cascading two sensors. Metal detection sensor having sensitivity in mm scale had superior sensitivity to ferrous sphere with diameter down to 0.7 mm using 50 kHz exciting frequency in standalone operation. Sensor response was proportional to the exciting frequency and the volume of ferrous test sample as expected. The sensitivity distribution at the object passage showed enhanced uniformity by attaching copper patch on the winding coil. The bandwidth, around 11 Hz, of LPF after phase sensitive detector was found to be optimum for sensitivity enhancement. Metal detection sensor having sensitivity in cm scale showed more uniform sensitivity distribution, but with order of lower sensitivity, which was suited to extend sensing range to cm scale with minimum interference. This antenna structure, facing each other, has the advantage of adding more axes in a simple way; thus it enables modular construction to achieve near uniform sensitivity distribution without direction dependent sensitivity. The effect of interference while in simultaneous operation of two sensors was investigated, and the measured result showed reduced output response but still within usable detection range. Thus it was feasible to operate two sensors, having different sensitivity range, simultaneously and to extend detection range from mm to cm scale, within practically acceptable interference.



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*Source: 412621-2014-07-10.xml*