The present application is a national phase entry under 35 U.S.C. § 371 of International Application No. PCT/EP2018/085038 filed Dec. 14, 2018, which claims priority from French Application No. 1762289, filed Dec. 15, 2017, all of which are incorporated herein by reference.
The invention relates to the field of the detection of target objects, and more particularly to the detection of explosive charges such as landmines buried in the ground.
In order to detect explosive charges, it is known to use dual technology detectors (“dual detectors”) comprising a detection head housing an inductive sensor and a ground-penetrating radar, insofar as these technologies are complementary as for the types of detected materials (metals for the inductive sensor vs. differences in dielectric constants of the materials and relative position for the radar).
In use, the Applicant has however noticed that the ground was not neutral from an electromagnetic point of view and can therefore disturb the coupling between the windings. In addition, the ground is rarely uniformly magnetic so that, during the scanning of the ground with the detector by an operator, the detected signal can vary only due to the presence of metal debris or to the very composition of the ground, or even trigger false alarms.
In addition, the operators using these detectors may be inadequately trained and may not hold the detector properly or perform an inappropriate scanning motion. The detection head can then form a lateral angle with the ground, so that one of the coils is closer to the ground than the other of the coils, which creates a strong modulation of the signal and therefore risks triggering false alarms. And even if the operator were well trained and tried to keep the detection head substantially parallel to the ground at any point in the scanning motion, he cannot locally modify its inclination to take into account the unevenness in the ground.
In order to overcome these difficulties, manufacturers tend to reduce the sensitivity of these detectors. The risk, however, is that they will no longer be able to detect targets buried in the ground and therefore put the lives of the operators in danger.
Document U.S. Pat. No. 3,758,849 describes a method for detecting a target object using a detector comprising a detection head comprising a inductive sensor comprising a transmitting coil and a receiving coil distinct from each other. The transmitting coil and the receiving coil form a coupling area.
However, the detector is fixed and it is the object to be scanned that moves in front of it along a scanning direction. The detector therefore does not scan the ground. In addition, it is not a dual detector, that is to say a detector comprising an additional detection means in addition to the inductive sensor.
Document U.S. Pat. No. 9,733,353 describes a detector comprising a single detection loop.
Document WO 2012/024133 describes a detector comprising an inductive sensor formed by a receiving coil and a transmitting coil positioned so as to form a through bar and V-shaped radar antennas.
An object of the invention is therefore to propose a dual detector comprising a detection head housing an inductive sensor and another sensor, such as a ground penetrating radar, which is capable of reducing the false alarms likely to be generated during the scanning of a ground with the detector while having higher sensitivity.
For this, the invention proposes a method for detecting a target object using a dual detector, said detector comprising a detection head comprising an inductive sensor comprising a transmitting coil and a receiving coil distinct from each other, the transmitting coil and the receiving coil each forming a loop, the loop of the transmitting coil at least partially overlapping the loop of the receiving coil so as to form a coupling area, the coupling area being elongated along a first longitudinal direction defining a first axis. The detector is moved along a scanning direction defining a scanning axis and in that, during this movement, the detection head is oriented so that the first axis of the coupling area is substantially parallel to the scanning axis.
According to a second aspect, the invention proposes a dual detector suitable for use in a detection method as described above, said detector comprising a detection head fixed to a handle by means of a mechanical link, the detection head comprising:
Some preferred but nonlimiting characteristics of the dual detector described above are the following, taken individually or in combination:
The detector further comprises a grip configured to be grasped by an operator, said grip extending in the plane.
The detector further comprises a ground-penetration radar comprising a transmitting antenna and a receiving antenna, the transmitting antenna and the receiving antenna each being housed in the center of one of the loops of the transmitting and receiving coils.
Other characteristics, aims and advantages of the present invention will become more apparent upon reading the following detailed description, and in relation to the appended drawings given by way of nonlimiting examples and wherein:
A dual detector 1 according to the invention comprises a detection head 10 fixed to a handle 20 by means of a mechanical link 30.
The detection head 10 corresponds to the portion intended to come close to the ground in order to detect target products. To this end, it comprises:
The transmitting coil 12 and the receiving coil 13 are homopolar windings. In a manner known per se, they are configured to transmit and receive waves having a frequency comprised between 300 Hz and 180 kHz. They each form a loop and are shaped so that the loop of the transmitting coil 12 at least partially overlaps the loop of the receiving coil 13 so as to form a coupling area 14. This configuration allows obtaining an inductive sensor in which mutual inductance is minimal.
By way of comparison, compared to an inductive sensor comprising a single coil constituting the transmitter and the receiver and formed of two loops in series of opposite directions in order to neutralize the effects of external interferences, the use of two distinct coils 12, 13 for the transmitting coil 12 and the receiving coil 13 makes it possible to amplify the signal, and therefore does not require decreasing the detection threshold to avoid the risks of false alarms.
The coupling area is elongated along a first longitudinal direction which defines a first axis X1. In order to further reduce the risks of false alarms and to simultaneously increase the sensitivity of the detector 1, the inductive sensor is positioned so that, in use, the handle 20 extends in a plane P1 normal to the platform 11 on which the transmitting and receiving coils 12, 13 are fixed and the first axis X1 of the coupling area 14 is transverse to said plane P1.
By “transverse” it will be understood here that the first axis X1 forms an angle comprised between 70° and 110° with the plane P1, preferably on the order of 90°. Furthermore, the loop of the transmitting coil 12 and the loop of the receiving coil 13 being of symmetrical shape, the first axis X1 passes through the points 14a, 14b of intersections of the two loops.
By “longitudinal direction” of a part or an element, it will be understood here the direction along which the part or the element has its largest dimension.
In other words, during the scanning of the ground by an operator, which is done following a right/left scanning motion defining a scanning axis X0, that is to say perpendicular to the direction of advance of the operator, the detection head 10 is oriented so that the coupling area 14 is substantially aligned with the direction of the scanning motion. In this way, at all times, the transmitting coil 12 and the receiving coil 13 are at a substantially equal distance from the ground, even in the event of inclination of the detection head 10 and/or of unevenness in the ground, which significantly reduces the risks of false alarms. In addition, thanks to this new orientation, the metal debris on the ground do not necessarily pass through the coupling area 14, unlike the case of the traditional detector (
The loop of the transmitting coil 12 and the loop of the receiving coil 13 are both elongated along a second longitudinal direction which defines a second axis X2. This second axis X2 is substantially parallel to the first axis X1. In other words, the loop of the transmitting coil 12, the coupling area 14 and the loop of the receiving coil 13 have the same longitudinal direction and extend next to each other.
Furthermore, the shape of the detection head 10 is adapted to the configuration and to the spatial orientation of the transmitting and receiving coils 12, 13. It is therefore elongated along the same direction as the loops and extends along a longitudinal direction which is substantially parallel to the first axis X1.
In a first embodiment, the transmitting coil 12 and the receiving coil 13 are directly printed on the platform 11. The platform 11 and the transmitting and receiving coils 12, 13 therefore form a printed circuit. This embodiment has the advantage of reducing the compactness of the inductive sensor in the detection head 10 as well as the overall weight of the detector 1. Its cost is however substantial. Consequently, in a second embodiment, which is illustrated in
The mechanical link 30 may comprise a built-in, pivot or ball-joint type link. Preferably, the mechanical link 30 is fixed in rotation about a third axis X3 which is comprised in the plane P1 and is perpendicular to the first axis X1. By blocking the rotation about the third axis X3, the operator is encouraged to grasp the detector 1 so that the coupling area 14 is substantially parallel to the scanning axis X0 during a detection sequence.
Optionally, the detector 1 further comprises means 40 for the gripping of the detector 1 by an operator. Usually, the gripping means 40 may comprise a hoop 41 configured to slidably receive the operator's arm and a grip 42 configured to be grasped by the operator.
In one embodiment, the grip 42 extends in the plane P1 in order to structurally force the operator to position the detector 1 so that the coupling area 14 is oriented so as to extend substantially parallel to the scanning axis X0 during a detection sequence.
The handle 20 can be telescopic and/or comprise several distinct portions configured to be assembled with each other before being fixed together, for example by screwing.
In a manner known per se, the detector 1 also comprises processing means 50 comprising in particular a microprocessor configured to process the signal detected by the inductive sensor 12, 13, such as one or more electronic cards, a memory and when appropriate alert means and/or a display device 51.
The processing means 50 can be housed in whole or in part at the gripping means 40.
These tests were carried out on a magnetic ground. In a first case (
The detection head 10 has been passed along a right/left scanning motion according to the motion recommended to the operators in the field. By right/left scanning motion, it will be understood here a lateral motion, that is to say along a scanning axis X0 which is perpendicular to the plane P1 in which the handle 20 extends.
In this first series of tests, during the scanning motion, the detection head 10 is placed in contact with the ground (0 cm—
The results of the measurements carried out for the three cases, with the traditional detector and the detector 1 according to the invention, at 0 cm and 5 cm, are summarized in the table below:
It therefore appears from this series of comparative tests that by modifying the orientation of the transmitting coil 12 and of the receiving coil 13 relative to the scanning axis X0, the ratio between the amplitude of the signal at 0 cm (in contact with the ground) and at 5 cm from the ground is significantly decreased. In other words, the influence of the ground type and of the metal debris or comprising oxides laid on the ground is significantly decreased when the scanning direction is parallel to the first axis X1 (and therefore to the longitudinal direction of the coupling area 14).
This configuration therefore makes it possible to significantly increase the detection sensitivity of the detector 1 according to the invention, since the type of ground and any debris have less influence on the detection and therefore generate fewer false alarms.
During this second series of tests, the detection head 10 of the traditional detector and of the detector 1 of the invention was passed over the magnetic ground, at 5 cm from the ground. The gain of the two detectors was equalized such that they provide the same intensity for the same gain. However, in a first case, the detection head 10 was tilted at an angle of 20° relative to the ground, statically (no scanning motion—
The results of the measurements carried out for the two cases, with the traditional detector and the detector 1 according to the invention, are summarized in the table below:
It appears from this second series of comparative tests that by modifying the orientation of the transmitting coil 12 and of the receiving coil 13 relative to the scanning axis X0, there is a significant decrease in the amplitude of the signal resulting from the simple inclination of the detector 1. Indeed, in the case of the traditional detector, the difference in amplitude of the signal due to the simple inclination, statically, of the detection head, is of 350 mV, against 200 mV in the case of the detector 1 of the invention. Similarly, the amplitude of the signal due to the simple scanning with inclination is of 400 mV for the traditional detector, against 250 mV for the detector 1 of the invention.
The detector 1 comprises an additional sensor, preferably a ground-penetration radar 60.
In this case, the radar 60 comprises a transmitting antenna 61 and a receiving antenna 62 configured to transmit and receive electromagnetic waves in the ground, for example at a frequency comprised between 100 MHz and 8 GHz. When these waves encounter medium changes, part of the waves is returned to the surface and recorded by the receiving antenna 62.
Advantageously, thanks to the orientation of the transmitting and receiving coils 12, 13 relative to the scanning axis X0, the surface available within each of the loops is greater. The transmitting antenna 61 and the receiving antenna 62 can therefore each be housed in the center of one of the loops of the transmitting coil 12 and of the receiving coil 13. In this way, the maximum sensitivity of the radar 60 is in the same area as the maximum sensitivity of the inductive sensor, that is to say at the coupling area 14. In other words, the microwave detection lobes of the radar 60 and the magnetic detection lobes of the inductive sensor match, so that it becomes possible for an operator to consider that the detection of a target takes place in the central area of the detection head 10 during pointing.
The loops of the transmitting coil 12 and of the receiving coil 13 having an elongated shape, the transmitting and receiving 12, 13 antennas 61, 62 can be elongated along a fourth axis X4 parallel to the second axis X2 in order to maximize the radiation surface and therefore the transmission capacity. For example, the transmitting antenna 61 and the receiving antenna 62 can have the shape of a logarithmic spiral which has been lengthened in order to maximize the radiation surface and the gain of the antennas while minimizing the length of each strand 63 forming the spiral of the antennas 61, 62 so as not to increase the pulse. In an elongated logarithmic spiral antenna, the spacing between the strands 63 of the spiral is indeed greater and increases logarithmically.
For example, the elongated logarithmic spiral forming the antennas 61, 62 can have a height of about 150 mm for 80 mm.
As a variant, the transmitting antenna 61 and the receiving antenna 62 of the radar 60 can be of one of the following types: quad-ridged horn radio antenna, bow tie antenna, rectangular bow tie antenna, Archimedean spiral antenna, logarithmic spiral antenna, Vivaldi antenna.
In a manner known per se, the transmitting antenna 61 and the receiving antenna 62 can be made of copper, which is a good electrical conductor.
However, in order to reduce the risks of oxidation of the antennas, the transmitting and receiving 12, 13 antennas 61, 62 can be partly made of nickel and/or chromium and partly made of copper. Nickel and chromium indeed have the advantage of not oxidizing over time while being electrically conductive.
For example, the center 64 of each antenna 61, 62 can be made of copper and protected by a layer comprising gold, while the rest 65 of the antennas 61, 26 is made of nickel and/or chromium. Between the central portion of each antenna 61, 26 and the rest of the antenna 61, 62 can be made of copper and covered with a layer of nickel (and/or chromium).
Furthermore, in order to limit the interactions with the transmitting and receiving coils 12, 13, a thickness of the transmitting antenna 61 and of the receiving antenna 62 is smaller than a depth of absorption of the coils 12, 13. In this way, the antennas 61, 62 become invisible to the magnetic field of the inductive sensor. It will however be noted that the thickness of the transmitting and receiving antennas 12, 13 must remain greater than a threshold thickness to guarantee sufficient mechanical robustness of the antennas 61, 62 and avoid any risk of breakage. The thickness of the transmitting and receiving antennas 61, 62 is therefore chosen so as to be comprised between a hundred nanometers and a micron. For example, the transmitting antenna 61 and the receiving antenna 62 may have a thickness on the order of 200 nm (to within 10%).
In order to produce antennas 61, 62 of this thickness, it is possible in particular to use a Physical Vapor Deposition (PVD) technique. This technique indeed makes it possible to obtain antennas 61, 62 of very small thickness with high dimensional accuracy and to produce several antennas at a time.
Number | Date | Country | Kind |
---|---|---|---|
1762289 | Dec 2017 | FR | national |
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/EP2018/085038 | 12/14/2018 | WO |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2019/115798 | 6/20/2019 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3758849 | Susman | Sep 1973 | A |
5119028 | Mooney et al. | Jun 1992 | A |
5148151 | Podhrasky | Sep 1992 | A |
5214378 | Hore | May 1993 | A |
5323114 | Nagamune | Jun 1994 | A |
5844140 | Seale | Dec 1998 | A |
6951133 | Passarelli, Jr. | Oct 2005 | B2 |
7336078 | Merewether | Feb 2008 | B1 |
7550734 | Lee | Jun 2009 | B1 |
7733077 | Merewether | Jun 2010 | B1 |
8072310 | Everhart | Dec 2011 | B1 |
8269479 | Krapf | Sep 2012 | B2 |
9703002 | Olsson | Jul 2017 | B1 |
9733353 | Carlson | Aug 2017 | B1 |
9835752 | Reime | Dec 2017 | B2 |
9997845 | Schantz | Jun 2018 | B2 |
10069336 | Fackelmeier | Sep 2018 | B2 |
10082572 | Duvoisin, III | Sep 2018 | B2 |
10587308 | Henry | Mar 2020 | B2 |
11238670 | Six | Feb 2022 | B2 |
20010014520 | Usui | Aug 2001 | A1 |
20030205088 | Passarelli, Jr. | Nov 2003 | A1 |
20060006874 | Nelson | Jan 2006 | A1 |
20070085427 | Sivasubramaniam | Apr 2007 | A1 |
20090174396 | Howard | Jul 2009 | A1 |
20110148392 | Krapf | Jun 2011 | A1 |
20120092206 | Etebari | Apr 2012 | A1 |
20120280849 | Chang | Nov 2012 | A1 |
20130113648 | Duvoisin, III et al. | May 2013 | A1 |
20130113649 | Trishaun | May 2013 | A1 |
20130154649 | Candy | Jun 2013 | A1 |
20140111208 | Olsson | Apr 2014 | A1 |
20140139210 | Walsh | May 2014 | A1 |
20140145704 | Krapf | May 2014 | A1 |
20140191750 | Reime | Jul 2014 | A1 |
20140270051 | Smithanik | Sep 2014 | A1 |
20150369910 | Griebeler | Dec 2015 | A1 |
20160012966 | Davis | Jan 2016 | A1 |
20160259047 | Blech | Sep 2016 | A1 |
20160322852 | Yeh | Nov 2016 | A1 |
20170060291 | Chevrier | Mar 2017 | A1 |
20170115424 | Olsson | Apr 2017 | A1 |
20170222321 | Caratelli | Aug 2017 | A1 |
20180011212 | Kang | Jan 2018 | A1 |
20180164429 | Tasovac | Jun 2018 | A1 |
20200055417 | Pachler | Feb 2020 | A1 |
20200408893 | Wang | Dec 2020 | A1 |
Number | Date | Country |
---|---|---|
H0933194 | Feb 1997 | JP |
2012-527603 | Nov 2012 | JP |
2014-527628 | Oct 2014 | JP |
WO-2006082334 | Aug 2006 | WO |
WO-2012024133 | Feb 2021 | WO |
Entry |
---|
French Search Report for Application No. 1762289 dated Sep. 13, 2018, 2 pages. |
International Search Report for Application No. PCT/EP2018/085038 mailed Jan. 29, 2019, 2 pages. |
Number | Date | Country | |
---|---|---|---|
20210080608 A1 | Mar 2021 | US |