JPS58100768A - metal detector - Google Patents

metal detector

Info

Publication number
JPS58100768A
JPS58100768A JP56200389A JP20038981A JPS58100768A JP S58100768 A JPS58100768 A JP S58100768A JP 56200389 A JP56200389 A JP 56200389A JP 20038981 A JP20038981 A JP 20038981A JP S58100768 A JPS58100768 A JP S58100768A
Authority
JP
Japan
Prior art keywords
coil
magnetic field
excitation
metal detector
metal
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.)
Granted
Application number
JP56200389A
Other languages
Japanese (ja)
Other versions
JPH0429035B2 (en
Inventor
Kazuo Watabe
一雄 渡部
Yoshiaki Matsumoto
松本 好秋
Yasuharu Yamada
康晴 山田
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.)
Shimadzu Corp
Technical Research and Development Institute of Japan Defence Agency
Shimazu Seisakusho KK
Original Assignee
Shimadzu Corp
Technical Research and Development Institute of Japan Defence Agency
Shimazu Seisakusho KK
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Shimadzu Corp, Technical Research and Development Institute of Japan Defence Agency, Shimazu Seisakusho KK filed Critical Shimadzu Corp
Priority to JP56200389A priority Critical patent/JPS58100768A/en
Publication of JPS58100768A publication Critical patent/JPS58100768A/en
Publication of JPH0429035B2 publication Critical patent/JPH0429035B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01VGEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
    • G01V3/00Electric or magnetic prospecting or detecting; Measuring magnetic field characteristics of the earth, e.g. declination, deviation
    • G01V3/08Electric 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
    • G01V3/10Electric 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
    • G01V3/104Electric 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
    • G01V3/105Electric 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 forming directly coupled primary and secondary coils or loops
    • G01V3/107Electric 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 forming directly coupled primary and secondary coils or loops using compensating coil or loop arrangements

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Electromagnetism (AREA)
  • Environmental & Geological Engineering (AREA)
  • Geology (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Geophysics (AREA)
  • Geophysics And Detection Of Objects (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 この発明は、たとえば地中等に埋設されている金属物体
を探知する金属探知器に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a metal detector for detecting metal objects buried underground, for example.

従来より、地中の金属物体を探知する金属探知器として
は、励振電源よりの信号を受けて探知すべき金属片に励
振磁界を加える励振コイルと、励振磁界が加えられるこ
とによフ金属片から発生される信号磁界を検出して電気
信号に変換する受はコイルとから構成されるものがある
。この種金属探知器を用いて地中に埋設された金属物体
を探知する場合には、金属物体が形状的に非常に小さい
ものもあり、また埋設されている点が地中深くであった
シ、探知方向から離れていることもあって。
Conventionally, metal detectors that detect metal objects underground have been equipped with an excitation coil that receives a signal from an excitation power source and applies an excitation magnetic field to the metal piece to be detected, and a metal detector that detects metal objects by applying the excitation magnetic field. A receiver that detects a signal magnetic field generated by a magnetic field and converts it into an electric signal is sometimes composed of a coil. When detecting metal objects buried underground using this type of metal detector, it is important to note that some metal objects may be very small in shape, or that the buried point is deep underground. , partly because it is far away from the detection direction.

金属探知器は出来るだけ感度の良いものが望ましい。し
かし、従来の金属探知器において、感度を向上させるた
め余9励振磁界を大きくすると、励振磁界が受信コイル
にも影響を与えるので感度を良くするにも限界があった
It is desirable that the metal detector be as sensitive as possible. However, in conventional metal detectors, if the excitation magnetic field is increased in order to improve sensitivity, the excitation magnetic field also affects the receiving coil, so there is a limit to how much sensitivity can be improved.

この発明の目的は、上記従来の金属探知器の欠点を解消
し、感度の良いすなわち探知性能の良いまた。同じ感度
のものであれば従来のものよりコンパクトな金属探知器
を提供するにある。
The object of the present invention is to eliminate the drawbacks of the conventional metal detectors mentioned above, and to provide a metal detector with good sensitivity, that is, good detection performance. The purpose is to provide a metal detector that is more compact than conventional metal detectors with the same sensitivity.

以上の目的を達成するために、この発明の金属探知器は
、励振磁界による受はコイルへの影響を打消すだめの打
消コイルを設け、この打消コイルに、受信コイルを内包
するようにしている。
In order to achieve the above object, the metal detector of the present invention is provided with a canceling coil for canceling the influence of the excitation magnetic field on the coil, and the receiving coil is enclosed in the canceling coil. .

以下2図面に示す実施例により、この発明の詳細な説明
する。
The present invention will be described in detail with reference to embodiments shown in the following two drawings.

第1図はこの発明の一実施例を示す金属探知器のコイル
の配置を示す図であフ、第2図は第1図に示す金属探知
器の接続図を示している。
FIG. 1 is a diagram showing the arrangement of coils of a metal detector showing an embodiment of the present invention, and FIG. 2 is a diagram showing the connections of the metal detector shown in FIG. 1.

第1図に示すように、大径の励振コイμm内に。As shown in Fig. 1, inside the large-diameter excited carp μm.

励振コイ/L/1の中心Co f対称にして1対の受信
コイ/l/2m、2bが配置されており、さらにこの受
信コイlv2m、2b″f:内包する1対の打消コイ/
l/3g、5bが受信コイ/I/2a、2bと同心円的
に配置されている。なお、受信コイ/I/2a、2bは
高透磁率の磁芯4a、4bに巻回されている。
A pair of receiving coils/l/2m, 2b are arranged symmetrically with the center Co f of the excitation coil/L/1, and furthermore, this receiving coil lv2m, 2b″f: a pair of canceling coils/
1/3g, 5b are arranged concentrically with receiving coils/I/2a, 2b. The receiving coils /I/2a and 2b are wound around magnetic cores 4a and 4b having high magnetic permeability.

また、同じく励振コイ/v1内には1対の補償コイ/L
158.5bも配置されている。補償コイ/L15a。
Similarly, a pair of compensation coils/L are included in the excitation coil/v1.
158.5b is also located. Compensation Carp/L15a.

5bは励振コイル1の略中心を通り、受信コイル2a、
2bを結ぶ線とは垂直の線上に設けられるガイド孔6に
摺動自在に配されている。
5b passes approximately through the center of the excitation coil 1, and the receiving coil 2a,
It is slidably disposed in a guide hole 6 provided on a line perpendicular to the line connecting 2b.

これら各コイルは第2図に示すように接続されている。These coils are connected as shown in FIG.

励振コイ/l/1と打消コイ/l/3a、3bは直列接
続され、励振信号発生用の発振器7に接続されており、
受信コイ/l/2a、2b及び補償コイル5a、5bは
直列接続され増幅器8に接続されている。
The excitation coil/l/1 and the canceling coil/l/3a and 3b are connected in series and connected to an oscillator 7 for generating an excitation signal,
The receiving coils/l/2a, 2b and the compensation coils 5a, 5b are connected in series to an amplifier 8.

今2発振器7より打消コイtv5a、励振コイル1、打
消コイル3bに電流を流すと、励振コイル1によって励
振磁界H1が発生する。もし励振磁界H1の軸方向に探
知すべき金属片9が存在すると、励振磁界H1によって
金属片9に誘導電流が発生し、金属片9より微弱な信号
磁界H9が発生する。一方、打消コイル3a、3bにも
発振器7よシの電流が流れるので打消磁界H3a、H3
bが生じるが、これらの磁界の方向は励振磁界H1とは
逆方向となるように構成されているので励振磁界H1は
打消磁界H3a、Hubによって打消される。そのため
受はコイtv2h、2bは信号磁界H9のみを検知して
検知信号を発生させる。受信コイ/I/2a、2bは増
幅器8に差動的に接続されており、増幅器8は受信コイ
/1/2aの検知信号と受信コイ/l/2bの検知信号
の差の出力を導出する。そのため、金属片9が第2図の
現位置にあり。
Now, when current is passed from the second oscillator 7 to the canceling coil tv5a, the excitation coil 1, and the canceling coil 3b, the excitation coil 1 generates an excitation magnetic field H1. If a metal piece 9 to be detected exists in the axial direction of the excitation magnetic field H1, an induced current is generated in the metal piece 9 by the excitation magnetic field H1, and a signal magnetic field H9 weaker than the metal piece 9 is generated. On the other hand, since the current from the oscillator 7 also flows through the canceling coils 3a and 3b, the canceling magnetic fields H3a and H3
However, since the directions of these magnetic fields are configured to be opposite to the excitation magnetic field H1, the excitation magnetic field H1 is canceled by the canceling magnetic fields H3a and Hub. Therefore, the receiver is Koi tv2h, and the receiver 2b detects only the signal magnetic field H9 to generate a detection signal. The receiving coils/I/2a and 2b are differentially connected to an amplifier 8, and the amplifier 8 derives an output of the difference between the detection signal of the receiving coil/1/2a and the detection signal of the receiving coil/1/2b. . Therefore, the metal piece 9 is in its current position in FIG.

金属探知器が図面の下方より上方に向けて移動して探査
されるとすれば励振コイル1が金属片9に近ずくにつれ
、受信コイ/1/2mの検知信号が増加し、あるピーク
値を検出した後減少する。励振コイA/1の中央が金属
片9を通過する頃から今度は受信コイ/I/2bの検知
信号が増加し、励振コイル1の移動につれてやはりある
ピーク値を検出した後減少する。その結果、増幅器8は
一種の8字特性出力を得るので金属片9の存在を知るこ
とができる。すなわち探知ができる。
If the metal detector moves from the bottom to the top of the drawing for exploration, as the excitation coil 1 approaches the metal piece 9, the detection signal of the receiving coil/1/2m will increase and reach a certain peak value. Decrease after detection. From the time when the center of the excitation coil A/1 passes the metal piece 9, the detection signal of the reception coil I/2b increases, and as the excitation coil 1 moves, it also detects a certain peak value and then decreases. As a result, the amplifier 8 obtains a kind of figure-8 characteristic output, so that the presence of the metal piece 9 can be known. In other words, it can be detected.

なお、受信コイ/I/2m、2bは信号磁界H9の検知
感度を上げるために高透磁率の磁芯4a、4bを組込ん
でいるが、もしこの場合打消コイ)tz3a+3bがな
いと受信コイ7L/2a、2bは強大な励振磁界H1に
さらされることになり、検知感度向上のために設けた磁
芯4 a @ 4 bは磁気的に飽和してしまい、その
機能を果さなくなる。また、受信コイル2a、2bに磁
芯4a、4bを組込むことにより同一感度を得るとする
と受信コイ/v2a。
In addition, the receiving coil /I/2m, 2b incorporates magnetic cores 4a, 4b with high magnetic permeability in order to increase the detection sensitivity of the signal magnetic field H9, but in this case, if there is no canceling coil) tz3a+3b, the receiving coil 7L /2a and 2b will be exposed to the strong excitation magnetic field H1, and the magnetic core 4a @ 4b provided to improve detection sensitivity will be magnetically saturated and will no longer perform its function. Further, if the same sensitivity is obtained by incorporating the magnetic cores 4a and 4b into the receiving coils 2a and 2b, the receiving coil/v2a.

2bの断面積と巻数を縮小することができるので金属探
知器全体を小型化できる。
Since the cross-sectional area of 2b and the number of turns can be reduced, the entire metal detector can be made smaller.

次に補償コイ/L15a、’5bの作用について説明す
る。
Next, the action of the compensation coils /L15a and '5b will be explained.

上記実施例において、受信コイ/v2a、2bの特性が
理想的であり、バランスがとれていれば。
In the above embodiment, if the characteristics of the receiving carp/v2a, 2b are ideal and balanced.

金属片9の存在しない場合や金属片が存在する場合で金
属探知器の励振コイ/l/1の中央部が金属片9に達し
た時は増幅器8の出力が0となるはずであるが、受信コ
イ/L/2a、2bのひずみ等で増幅器8の出力が0に
ならず誤差分を出力することがある。この誤差分を補償
するために補償コイル5a。
When the metal piece 9 is not present or when a metal piece is present, when the center of the excitation coil /l/1 of the metal detector reaches the metal piece 9, the output of the amplifier 8 should be 0. The output of the amplifier 8 may not become 0 due to distortion of the receiving coil/L/2a, 2b, etc., and an error amount may be output. A compensation coil 5a is provided to compensate for this error.

5bf設けている。補償コイl 5 a + 5 bは
ガイド孔6に沿って摺動自在でアリ、その位置を励振コ
イ/L/1の中心COから励振コイ/I/1の巻回面C
1近くまで移動することができる。また、その時に補償
コイル5a、5bに発生する補償磁界H5a。
5bf is provided. The compensation coil 5a + 5b is slidable along the guide hole 6, and its position is changed from the center CO of the excitation coil/L/1 to the winding surface C of the excitation coil/I/1.
You can move up to 1. Also, at that time, a compensation magnetic field H5a is generated in the compensation coils 5a and 5b.

H5bの磁界の強さH5は第6図に示すように励振コイ
/L/1の中心CDよυ励振コイル1の巻回面C1に向
って増加するので補償磁界H5a 、 H5bを自由に
選択でき、精度の高い補償を行うことができる。なお補
償コイル5a、5bはガイド孔6を摺動自在にする代り
に適宜な複数の穴を上記ガイド孔6を設けたと同様の線
上に設け、補償コイル5a、5bt−その穴に抜差自在
とし位置を調整するようにしてもよい。
As shown in Fig. 6, the magnetic field strength H5 of H5b increases from the center CD of the excitation coil/L/1 toward the winding surface C1 of the excitation coil 1, so the compensation magnetic fields H5a and H5b can be freely selected. , it is possible to perform highly accurate compensation. In addition, instead of making the guide hole 6 slidable, the compensation coils 5a, 5b are provided with a plurality of appropriate holes on the same line as the guide hole 6, and the compensation coils 5a, 5b can be freely inserted into and removed from the holes. The position may also be adjusted.

また、上記実施例において打消コイlL/3a、3bは
励振コイ/l/1に直列に、補償コイ1L15a、5b
は受信コイAz2a、2bに直列に、接続した場合を示
したが、これに限ることなく打消コイルは励振磁界の打
消を、補償コイμは受信コイルの補償をなすものである
なら他の接続方法であってもよい。
Further, in the above embodiment, the canceling coils 1L/3a, 3b are connected in series with the excitation coil/1/1, and the compensation coils 1L15a, 5b
shows the case where the receiving coils Az2a and 2b are connected in series, but the invention is not limited to this, and other connection methods may be used as long as the canceling coil cancels the excitation magnetic field and the compensation coil μ compensates for the receiving coil. It may be.

以上のようにこの発明の金属探知器によれば。According to the metal detector of the present invention as described above.

受信コイルを内包するように配置した打消コイルを設け
、この打消コイルにより発生される打消磁界により受部
コイルへの励振磁界を打消すようにしたから受信コイル
は探知すべき金属物体よりの信号磁界のみを検知すれば
よく高探知性能の金属探知器を得ることができる。
A canceling coil is arranged to enclose the receiving coil, and the canceling magnetic field generated by this canceling coil cancels the excitation magnetic field to the receiving coil, so that the receiving coil receives the signal magnetic field from the metal object to be detected. A metal detector with high detection performance can be obtained by detecting only the metal.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例を示す金属探知器のコイル
の配置を示す図、第2図は第1図に示す金属探知器の電
気的接続図、第6図は第1図、第2図に示す実施例に使
用される補償コイルの磁界分布を示す図である。 1:励振コイル、   2a・2b:受信コイル。 3g−3b:打消コイルl  4a−4b:磁芯。 5B・5b:補償コイル、  6:ガイド孔。 7:発振器、 8:増幅器、 9:金属片。 Hl:励振磁界、  H2a−H2b:信号磁界。 H3a−H3b:打消磁界、  H5a−H5b:補償
磁界、 H9:信号磁界1 H5:磁界の強さ、 CO:励振コイルの中心。 C1:励振コイμの巻回面  。 特許出願人  防衛庁技術研究本部長 大森幸衛(ほか
1名) 代理人  弁理士  中 村 茂 信 第1図 第2図 第3図
FIG. 1 is a diagram showing the coil arrangement of a metal detector showing an embodiment of the present invention, FIG. 2 is an electrical connection diagram of the metal detector shown in FIG. 1, and FIG. FIG. 2 is a diagram showing the magnetic field distribution of the compensation coil used in the embodiment shown in FIG. 2; 1: Excitation coil, 2a/2b: Receiving coil. 3g-3b: Cancellation coil l 4a-4b: Magnetic core. 5B/5b: Compensation coil, 6: Guide hole. 7: Oscillator, 8: Amplifier, 9: Metal piece. Hl: excitation magnetic field, H2a-H2b: signal magnetic field. H3a-H3b: Cancellation magnetic field, H5a-H5b: Compensation magnetic field, H9: Signal magnetic field 1 H5: Strength of magnetic field, CO: Center of excitation coil. C1: Winding surface of excitation coil μ. Patent applicant Yukie Omori, director of the Technology Research Headquarters, Defense Agency (and one other person) Agent: Shigeru Nakamura, patent attorney Figure 1 Figure 2 Figure 3

Claims (3)

【特許請求の範囲】[Claims] (1)励振用信号を発生する発振器と、この発振器より
の信号を受けて探知すべき金属片に励振磁界を加える励
振コイルと、励振磁界が加えられることにより金属片か
ら発生される信号磁界を検出して電気信号に変換する受
信コイルとより構成される金属探知器において、前記受
信コイルを内包するように配置され、前記励振磁界によ
る受信コイルへの影響を打消す磁界を発生する打消コイ
ルを設けたことを特徴とする金属探知器。
(1) An oscillator that generates an excitation signal, an excitation coil that receives the signal from this oscillator and applies an excitation magnetic field to the metal piece to be detected, and a signal magnetic field that is generated from the metal piece by applying the excitation magnetic field. A metal detector comprising a receiving coil that detects and converts into an electric signal, a canceling coil that is arranged to enclose the receiving coil and generates a magnetic field that cancels the influence of the excitation magnetic field on the receiving coil. A metal detector characterized by the following:
(2)前記打消コイμに内包される受信コイルは。 高透磁率磁芯に巻回したものであることを特徴とする特
許請求の範囲第1項記載の金属探知器。
(2) What is the receiving coil included in the canceling coil μ? The metal detector according to claim 1, wherein the metal detector is wound around a high magnetic permeability magnetic core.
(3)前記打消コイルに内包される受信コイルは。 差動的に動作する1対のコイルであり、これら1対のコ
イルに、コイルひずみ、ノイズ等により生じる誤差を補
償する補償コイ)Vf付設してなることを特徴とする特
許請求の範囲第1項または第2項記載の金属探知器。
(3) What is the receiving coil included in the cancellation coil? Claim 1: A pair of coils that operate differentially, and a compensation coil Vf that compensates for errors caused by coil distortion, noise, etc. is attached to the pair of coils. The metal detector described in paragraph 2 or paragraph 2.
JP56200389A 1981-12-11 1981-12-11 metal detector Granted JPS58100768A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56200389A JPS58100768A (en) 1981-12-11 1981-12-11 metal detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56200389A JPS58100768A (en) 1981-12-11 1981-12-11 metal detector

Publications (2)

Publication Number Publication Date
JPS58100768A true JPS58100768A (en) 1983-06-15
JPH0429035B2 JPH0429035B2 (en) 1992-05-15

Family

ID=16423509

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56200389A Granted JPS58100768A (en) 1981-12-11 1981-12-11 metal detector

Country Status (1)

Country Link
JP (1) JPS58100768A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1992000534A1 (en) 1990-06-29 1992-01-09 Safeline Limited Metal detector
GB2261073A (en) * 1990-06-29 1993-05-05 Safeline Ltd Metal detector
WO2001071387A3 (en) * 2000-03-22 2002-06-06 Univ Johns Hopkins Electromagnetic target discriminator sensor system and method for detecting and identifying metal targets

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011127452A (en) 2009-12-15 2011-06-30 Mitsubishi Heavy Ind Ltd Heat exchange module for vehicle

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1992000534A1 (en) 1990-06-29 1992-01-09 Safeline Limited Metal detector
GB2261073A (en) * 1990-06-29 1993-05-05 Safeline Ltd Metal detector
GB2261073B (en) * 1990-06-29 1994-02-16 Safeline Ltd Metal detector
WO2001071387A3 (en) * 2000-03-22 2002-06-06 Univ Johns Hopkins Electromagnetic target discriminator sensor system and method for detecting and identifying metal targets

Also Published As

Publication number Publication date
JPH0429035B2 (en) 1992-05-15

Similar Documents

Publication Publication Date Title
US4243839A (en) Transducer with flux sensing coils
EP0356171A2 (en) Direct-coupled fluxgate current sensor and sensing method using the same
ATE40604T1 (en) CURRENT DETECTOR CIRCUIT.
US4967145A (en) Active current transformer
US2856581A (en) Magnetometer
US5130655A (en) Multiple-coil magnetic field sensor with series-connected main coils and parallel-connected feedback coils
US4864232A (en) Temperature compensation for displacement transducer
CN110068390B (en) Piezoelectric and electromagnetic coupling vibration sensor
JPS58100768A (en) metal detector
US3286169A (en) Combined magnetometer and gradiometer
US4272724A (en) Magnetic modulator for magnetic field detection differentially outputting magnetic core noise
JP6974898B2 (en) Current converter
JP2025512134A5 (en)
JPH0618568A (en) Current sensor
JP3300496B2 (en) Radiation measurement system
CN111929735A (en) Transient electromagnetic exploration device and system with shielding function
US3353130A (en) High ratio vacuum tube input transformer
GB1003872A (en) A magnetic field detecting device
JPH073345Y2 (en) DC current detector
JPS5946340B2 (en) Accelerometer
US4495601A (en) Magnetic bubble memory apparatus
JP3126754B2 (en) Reactor device for line filter
GB2027319A (en) Public address system
JP2674012B2 (en) Metal detector
JP2514338B2 (en) Current detector