JPH02194363A - Current sensor - Google Patents
Current sensorInfo
- Publication number
- JPH02194363A JPH02194363A JP1446889A JP1446889A JPH02194363A JP H02194363 A JPH02194363 A JP H02194363A JP 1446889 A JP1446889 A JP 1446889A JP 1446889 A JP1446889 A JP 1446889A JP H02194363 A JPH02194363 A JP H02194363A
- Authority
- JP
- Japan
- Prior art keywords
- current
- coil
- magnetic
- pair
- magnetic field
- 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.)
- Pending
Links
- 238000001514 detection method Methods 0.000 claims abstract description 26
- 230000010355 oscillation Effects 0.000 claims description 7
- 239000000696 magnetic material Substances 0.000 claims description 2
- 239000004020 conductor Substances 0.000 abstract description 11
- 238000004804 winding Methods 0.000 abstract description 7
- 230000035945 sensitivity Effects 0.000 abstract description 4
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 abstract 2
- 230000015556 catabolic process Effects 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 5
- 238000012935 Averaging Methods 0.000 description 4
- 239000003990 capacitor Substances 0.000 description 4
- 230000005284 excitation Effects 0.000 description 3
- 235000014676 Phragmites communis Nutrition 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R19/00—Arrangements for measuring currents or voltages or for indicating presence or sign thereof
- G01R19/0092—Arrangements for measuring currents or voltages or for indicating presence or sign thereof measuring current only
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Current Or Voltage (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は、主として、直流電流を検出する電流センサに
関し、コイルを巻装した対の磁性線を間隔を隔てて配置
し、対の磁性線の各コイルはコイル電流の磁界方向が互
いに同一方向となるように巻装し、対の磁性線の間隔内
に電流検出部を設けることにより、直流電流を、外部磁
場の影響を受けることなく、高耐圧を確保して、高感度
で検出できるようにしたものである。[Detailed Description of the Invention] <Industrial Application Field> The present invention mainly relates to a current sensor for detecting direct current, in which a pair of magnetic wires wrapped around a coil are arranged at a distance, and a pair of magnetic wires is arranged at a distance. Each coil is wound so that the magnetic field direction of the coil current is in the same direction, and by providing a current detection section within the interval between the paired magnetic wires, DC current can be detected without being affected by external magnetic fields. It ensures high voltage resistance and enables detection with high sensitivity.
〈従来の技術〉
直流電流センサは、交流電流センサと異なって、検出部
にトランスを使用することができないノテ、その構成が
比較的複雑になる傾向にある。<Prior Art> Unlike alternating current sensors, direct current sensors cannot use a transformer in the detection section, and their configurations tend to be relatively complex.
第4図〜第6図は何J]も従来の直流電流センサな示し
・ている。まず、第4図は、検出しようとする電流11
の流ねているラインに031列に検出抵抗1を挿入1.
・、検出抵抗1の両端に現われる電位差を増幅回路A等
を通して検出する回路構成である。4 to 6 show conventional DC current sensors. First, FIG. 4 shows the current 11 to be detected.
Insert detection resistor 1 in column 031 to the flowing line.1.
・This is a circuit configuration in which the potential difference appearing across the detection resistor 1 is detected through an amplifier circuit A or the like.
第5区は、電流検出コイル2を巻回したコア3の一部に
:ギャ・・・ブG1を設け、このキャップG1内にホー
ル素子−または磁気抵抗素子等の磁電変換素−f4を配
置し・、1i11電変換素子4の出力を増幅回路A゛τ
τ増幅で出力するようになっている。In the fifth section, a gap G1 is provided in a part of the core 3 around which the current detection coil 2 is wound, and a magnetoelectric transducer f4 such as a Hall element or a magnetoresistive element is arranged in this cap G1.・The output of the 1i11 electric conversion element 4 is sent to the amplifier circuit A゛τ
It is designed to output by τ amplification.
次に第6図は、電話通信回線に多用されている電流セン
サを示し・、検出しようとする電流■1の流れる通イ言
線にリードリレー5を挿入する構成となっている。リー
トリレー5は、通信線に直列:ζ入る励磁巻線51と、
励磁巻線51の生じる磁界の作用を受け°Cオン、オフ
動作をするリード接点52とを備える。通信線には、音
声電流等の交流成分を重畳した直流電流が流れる。リー
トリレー5の巻線部のインピーダンスがこの交流成分な
阻1トしないようにするため、リートりし〜 5の1乃
力磁巻線51とMI列に、交流成分をバイパスするコン
デンサC4か接続されている。R,l:iサージ吸14
5+用のバリスタである。Next, FIG. 6 shows a current sensor that is often used in telephone communication lines, and has a configuration in which a reed relay 5 is inserted into the communication line through which the current 1 to be detected flows. The REIT relay 5 includes an excitation winding 51 that is connected in series with the communication line.
It is provided with a lead contact 52 that turns on and off under the action of the magnetic field generated by the excitation winding 51. A DC current on which an AC component such as a voice current is superimposed flows through the communication line. In order to prevent the impedance of the winding part of the relay relay 5 from interfering with this alternating current component, a capacitor C4 is connected to the magnetic winding 51 of the relay relay 5 and the MI column to bypass the alternating current component. has been done. R, l: i surge suction 14
This is a barista for 5+.
〈発明か解決しようとする問題点〉
しかしなから、第4図に示した電流センサl、j、検出
しようとする電流I、の流ねる電気回路と、検出回路と
を電気的に絶縁することカシCきないこと、電流11の
流れているラインの電位によつCは、検出部の耐圧保持
が困難になること、検出抵抗R1による損失を招くこと
等の問題点かある。<Problem to be solved by the invention> However, it is necessary to electrically insulate the detection circuit from the electric circuit through which the current sensors l and j shown in FIG. 4 and the current I to be detected flows. There are problems such as the fact that the current 11 does not change due to the potential of the line through which the current 11 flows, making it difficult to maintain the withstand voltage of the detection section, and causing loss due to the detection resistor R1.
第5図のN流センサは、微小電流を検出しようとすると
、検出コイル2の巻き数を増大さ世なけれはならず、検
出コイル2の抵抗分及びインダクタンス分か増えること
、検出コイル2か電tlの流れるラインと等電位となる
ため、ライン電位によっては耐圧保持が困難になること
等の問題点かある。In the N-flow sensor shown in Fig. 5, in order to detect a minute current, the number of turns of the detection coil 2 must be increased, which increases the resistance and inductance of the detection coil 2, and increases the current Since it has the same potential as the line through which tl flows, there are problems such as difficulty in maintaining a withstand voltage depending on the line potential.
第6図に示した電流センサは、検出端であるリードリレ
ー5の励磁巻線が通信回線に直列に入るため、交流成分
をバイパスするための大容量コンデンサC1や、サージ
吸収用のバリスタR5が必要になること等の問題点があ
る。In the current sensor shown in Fig. 6, the excitation winding of the reed relay 5, which is the detection end, is connected in series to the communication line, so a large capacity capacitor C1 to bypass the AC component and a varistor R5 for surge absorption are installed. There are problems such as the necessity of
そこで、本発明の課題は、上述する従来の問題へを解決
し、直流電流を、外部磁場の影響を受けることなく、高
耐圧を確保して、高感度で検出し得る電流センサを提供
することである。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a current sensor capable of solving the above-mentioned conventional problems and detecting direct current with high sensitivity while ensuring high withstand voltage without being affected by external magnetic fields. It is.
〈問題点を解決するための手段〉
上述する従来の問題点を解決するため、本発明は、コ、
イルを巻装した対の磁性線と、検出しようとする電流に
よる前記コイルのインダクタンス値変化に対応した出力
を生じる回路とを備える電流センサであって、
前記対の磁性線は、間隔を隔てて互いに平行となるよう
に配置されており、
前記対の磁性線の各コイルは、コイル電流による磁界の
方向が互いに同一方向となるように巻装さねており、
前記対の磁性線の間隔内に電流検出部を有すること
を特徴とする。<Means for solving the problems> In order to solve the above-mentioned conventional problems, the present invention provides the following:
A current sensor comprising: a pair of magnetic wires wrapped with a coil; and a circuit that generates an output corresponding to a change in inductance value of the coil due to a current to be detected, the pair of magnetic wires are spaced apart from each other. They are arranged so that they are parallel to each other, and each coil of the pair of magnetic wires is wound so that the direction of the magnetic field due to the coil current is in the same direction, and within the interval between the magnetic wires of the pair. It is characterized in that it has a current detection section.
く作用〉
電流検出に当っては、対の磁性線の間隔内に設けられた
電流検出部に、検出しようとする電流の流れている導線
を配置する。導線の周りには、電流の方向に依存した磁
界が発生ずる。対の磁性線は、間隔を隔てて平行となる
ように配置されているから、対の磁性線間の間隔内に設
定された電流検出部内の導線のまわりに発生した磁界は
、対の磁性線に巻かれたコイルと鎖交する。Effect> For current detection, a conductor wire through which the current to be detected is flowing is placed in the current detection section provided within the interval between the pair of magnetic wires. A magnetic field is generated around the conductor, which depends on the direction of the current. Since the magnetic wires of the pair are arranged parallel to each other with an interval between them, the magnetic field generated around the conductor wire in the current detection section that is set within the interval between the magnetic wires of the pair is It interlinks with the coil wound on.
対の磁性線の各コイルは、コイル電流による磁界の方向
が互いに同一方向となるように巻装されているから、導
線のまわりに発生した磁界は、方のコイルの生じる磁界
に対しては加算的に、他方のコイルの生じる6n界に対
しては差動的に作用する。このため、対の磁性線の各コ
イルのインダクタンス値が、検出電涜値に対応して、互
いに異なるようになる。従って、両コイルのインダクタ
ンス値の差を検出することにより、Tl ?mを検出て
きる。Each coil of a pair of magnetic wires is wound so that the direction of the magnetic field due to the coil current is in the same direction, so the magnetic field generated around the conductor wire is added to the magnetic field generated by the other coil. In other words, it acts differentially on the 6n field generated by the other coil. Therefore, the inductance values of the respective coils of the pair of magnetic wires become different from each other depending on the detected electric discharge value. Therefore, by detecting the difference between the inductance values of both coils, Tl? m can be detected.
本発明に係る電流センサは、検出しようとする電流の流
れている導線が外部回路となるから、センサとしての耐
圧は、導線の耐圧によって保証される。しかも、対の磁
性線に同一方向から加わる地球磁場等の外部磁界に対し
ては、各コイルのインダクタンス値は同一方向に同量だ
け変化し、差を生しない。従って、インダクタンス値の
差から電流を検出する本発明においては、外部磁界の影
響を受けることがなくなり、微小磁界を高精度で検知す
ることが可能になる。In the current sensor according to the present invention, since the conductor through which the current to be detected flows is an external circuit, the withstand voltage as a sensor is guaranteed by the withstand voltage of the conductor. Moreover, in response to an external magnetic field such as the earth's magnetic field that is applied to the pair of magnetic wires from the same direction, the inductance value of each coil changes by the same amount in the same direction and does not make any difference. Therefore, in the present invention, which detects current from the difference in inductance values, there is no influence of external magnetic fields, and it is possible to detect minute magnetic fields with high precision.
〈実施例〉
第1図は本発明に係る電流センサの実施例を示す。図に
おいて、6及び7は磁性線、8及び9はコイル、IOは
発振回路、11は平均化回路、12は差動増幅回路であ
る。<Example> FIG. 1 shows an example of a current sensor according to the present invention. In the figure, 6 and 7 are magnetic wires, 8 and 9 are coils, IO is an oscillation circuit, 11 is an averaging circuit, and 12 is a differential amplifier circuit.
磁性線6及び7は保磁力Heの小さな磁性材、例えばア
モルファス磁性線材による長さのほぼ等しい独立する線
材となっている。これらの磁性線6.7のそれぞれは、
コイル8及び9を巻回したうえて、間隔d、を隔ててほ
ぼ平行となるように配置されている。対のlin性線6
−7間の間隔d。The magnetic wires 6 and 7 are made of a magnetic material having a small coercive force He, for example, an amorphous magnetic wire, and are independent wires having substantially the same length. Each of these magnetic lines 6.7 is
The coils 8 and 9 are wound and arranged so as to be substantially parallel to each other with a distance d between them. paired lin sex line 6
The interval d between -7.
内には電流検出部S1を設けである。電流検出に当って
は、この電流検出部S1内に検出しようとする電流■1
の流れる導線13を配置する。A current detection section S1 is provided inside. When detecting current, the current to be detected (■1) is stored in this current detection section S1.
A conducting wire 13 is arranged through which the flow of the current occurs.
コイル8及び9は、コイル電流I8、IOによる磁界φ
8、φ9の方向が互いに同一方向となるように巻装され
ている。コイル8.9は、その端を直流電源端子14に
共通に接続すると共に、他端を発振回路10に接続しで
ある。Coils 8 and 9 have a magnetic field φ caused by coil currents I8 and IO.
8 and φ9 are wound in the same direction. The coils 8.9 have their ends commonly connected to the DC power supply terminal 14, and the other ends connected to the oscillation circuit 10.
実施例に示す発振回路10は、非安定マルチバイブレー
タで構成されており、トランジスタ101.102のコ
レクタに、コイル8.9を接続しである。トランジスタ
101.102のエミッタは、それぞれ抵抗103.1
04を介してアースし、一方のトランジスタ101 (
または102)のベースを、他方のトランジスタ102
(または101)のコレクタに、コンデンサと抵抗の並
列回路105(または106)を介して接続することに
より、非安定マルチバイブレータを構成しである。そし
て、トランジスタ101.102のエミッタ電圧を平均
化回路11で直流電圧に変換し、その直流電圧を差動増
幅回路12に入力し、出力端子15より差動出力電圧を
得るようになっている。111.112は抵抗、113
.114はコンデンサである。The oscillation circuit 10 shown in the embodiment is composed of an unstable multivibrator, and has a coil 8.9 connected to the collector of a transistor 101.102. The emitters of transistors 101.102 are connected to resistors 103.1 and 103.1, respectively.
04, and one transistor 101 (
or 102) to the base of the other transistor 102
(or 101) via a parallel circuit 105 (or 106) of a capacitor and a resistor, an astable multivibrator is constructed. Then, the emitter voltages of the transistors 101 and 102 are converted into a DC voltage by an averaging circuit 11, and the DC voltage is input to a differential amplifier circuit 12 to obtain a differential output voltage from an output terminal 15. 111.112 is resistance, 113
.. 114 is a capacitor.
次に、第2図を参照して動作を説明する。電流検出部S
1に配置された導線13に、矢印a方向の電流11が流
れているとすると、導線13の周りには、右ネジの法則
に従って、電流11の方向に依存した磁界φ1が発生す
る。Next, the operation will be explained with reference to FIG. Current detection part S
If a current 11 in the direction of arrow a is flowing through the conductor 13 disposed at 1, a magnetic field φ1 that depends on the direction of the current 11 is generated around the conductor 13 according to the right-handed screw rule.
対の磁性線6.7は、間隔d、を隔てて平行となるよう
に配置されているから、その間隔d、内に設定された電
流検出部S1内の導線13のまわりに発生した磁界φ8
は、対の磁性線6.7に巻かれたコイル8.9と鎮交す
る。Since the pair of magnetic wires 6.7 are arranged parallel to each other with an interval d, a magnetic field φ8 generated around the conductive wire 13 in the current detection unit S1 set within the interval d.
intersect with a coil 8.9 wound around a pair of magnetic wires 6.7.
ここで、対の磁性線6.7の各コイル8.9は、コイル
電流■8、IOによる磁界φ8、φ9の方向が互いに同
一方向となるように巻装されているから、導線13のま
わりに発生した磁界φ8は、コイル9の生じる磁界φ9
に対しては加算的に、コイル8の生じる磁界φ8に対し
ては差動的に作用する。このため、コイル9側では磁性
線7がほぼ磁気飽和し、インダクタンス値が著しく小さ
くなるので、コイル8のインダクタンス値とコイル9の
インダクタンス値との間に大きな差が生じる。非安定マ
ルチバイブレータ10はインダクタンス値の差が大きく
なる程、動作周波数が高くなり、かつ、各エミッタ間の
電圧も高くなる発振動作をする。従って、トランジスタ
101.102の出力を平均化回路11で平均化し、差
動増幅器12でその差分を増幅して取り出すことにより
、導線13に流れる電流■、を検出できる。Here, each coil 8.9 of the pair of magnetic wires 6.7 is wound so that the directions of the magnetic fields φ8 and φ9 due to the coil current 8 and IO are in the same direction. The magnetic field φ8 generated in the coil 9 is the magnetic field φ9 generated by the coil 9.
It acts additively on the magnetic field φ8 generated by the coil 8, and differentially acts on the magnetic field φ8 generated by the coil 8. Therefore, the magnetic wire 7 is almost magnetically saturated on the coil 9 side, and the inductance value becomes significantly small, so that a large difference occurs between the inductance value of the coil 8 and the inductance value of the coil 9. The unstable multivibrator 10 performs an oscillation operation in which the larger the difference in inductance values, the higher the operating frequency and the higher the voltage between each emitter. Therefore, by averaging the outputs of the transistors 101 and 102 in the averaging circuit 11 and amplifying and extracting the difference in the differential amplifier 12, it is possible to detect the current 2 flowing in the conducting wire 13.
導線13に流れる電流■1の方向が逆になった場合には
、コイル8.9の役割が逆になる。When the direction of the current (1) flowing through the conducting wire 13 is reversed, the role of the coil 8.9 is reversed.
本発明に係る電流センサは、検出しようとする電流■、
の流れている導線13が回路外部にあるから、導線13
による回路上の影響を受けることがない。また、電流セ
ンサとしての耐圧は、導線13の耐圧によって保証され
る。しかも、対の磁付線6.7に対して同一方向から加
わる地球磁場等の外部磁界φbは、各コイル8.9に対
して同様に作用し、インダクタンス値に変化を生じさせ
ない。従って、外部磁界φbの影響を受けることがなく
なり、導線13に流れる電流11だけを高精度で検知す
ることが可能になる。The current sensor according to the present invention has a current to be detected;
Since the conductor 13 flowing through it is outside the circuit, the conductor 13
The circuit is not affected by Further, the withstand voltage as a current sensor is guaranteed by the withstand voltage of the conducting wire 13. Moreover, the external magnetic field φb such as the earth's magnetic field applied from the same direction to the pair of magnetized wires 6.7 acts on each coil 8.9 in the same way and does not cause a change in the inductance value. Therefore, it is no longer affected by the external magnetic field φb, and only the current 11 flowing through the conducting wire 13 can be detected with high precision.
検出すべき電流I、が小さいときは、第3図に示すよう
に、導線13のターン数を増やすことにより、容易に検
知できる。導線13は磁性線6及びコイル8の組を包囲
するように巻回するか、磁性線7とコイル9の組を包囲
するように巻回する。When the current I to be detected is small, it can be easily detected by increasing the number of turns of the conducting wire 13, as shown in FIG. The conducting wire 13 is wound so as to surround the set of the magnetic wire 6 and the coil 8, or the set of the magnetic wire 7 and the coil 9.
〈発明の効果〉
以上述べたように、本発明は、コイルを巻装した対の磁
性線と、検出しようとする電流による前記コイルのイン
ダクタンス値変化に対応した出力を生じる回路とを備え
る電流センサであって、対の磁性線は、間隔を隔てて互
いに平行となるように配置されており、対の磁性線の各
コイルは、コイル電流による磁界の方向が互いに同一方
向となるように巻装されており、対の磁性線間の間隔内
に電流検出部を有するから、直流電流を、外部磁場の影
響を受けることなく、高耐圧を確保して、高感度で検出
し得る電流センサを提供できる。<Effects of the Invention> As described above, the present invention provides a current sensor comprising a pair of magnetic wires around which a coil is wound, and a circuit that generates an output corresponding to a change in the inductance value of the coil due to a current to be detected. The pairs of magnetic wires are arranged parallel to each other with a gap between them, and each coil of the pair of magnetic wires is wound so that the direction of the magnetic field due to the coil current is in the same direction. Since it has a current detection part within the interval between the paired magnetic wires, it provides a current sensor that can detect DC current with high sensitivity without being affected by external magnetic fields, ensuring high withstand voltage. can.
【図面の簡単な説明】
第1図は本発明に係る電流センサの実施例を示す回路図
、第2図は電流検出の基本動作を示す図、第3図は別の
実施例における要部の構成を示す図、第4図〜第6図は
従来の電流センサを示す図である。
6.7・・・磁性線 8.9・・・コイルS、
・・・電流検出部[Brief Description of the Drawings] Fig. 1 is a circuit diagram showing an embodiment of the current sensor according to the present invention, Fig. 2 is a diagram showing the basic operation of current detection, and Fig. 3 is a diagram showing the main parts of another embodiment. The diagrams showing the configuration, FIGS. 4 to 6, are diagrams showing a conventional current sensor. 6.7...Magnetic wire 8.9...Coil S,
...Current detection section
Claims (4)
る電流による前記コイルのインダクタンス値変化に対応
した出力を生じる回路とを備える電流センサであって、 前記対の磁性線は、間隔を隔てて互いに平行となるよう
に配置されており、 前記対の磁性線の各コイルは、コイル電流による磁界の
方向が互いに同一方向となるように巻装されており、 前記対の磁性線間の間隔内に電流検出部を有すること を特徴とする電流センサ。(1) A current sensor comprising a pair of magnetic wires wrapped around a coil and a circuit that generates an output corresponding to a change in the inductance value of the coil due to a current to be detected, the pair of magnetic wires having an interval between them. The coils of the pair of magnetic wires are wound so that the direction of the magnetic field due to the coil current is in the same direction, and the magnetic wires of the pair are arranged parallel to each other with a distance between them. A current sensor comprising a current detection section within an interval of.
により発振出力特性が変化する発振回路を含むことを特
徴とする特許請求の範囲第1項に記載の電流センサ。(2) The current sensor according to claim 1, wherein the circuit includes an oscillation circuit whose oscillation output characteristics change according to changes in the inductance value of the coil.
を特徴とする特許請求の範囲第2項に記載の電流センサ
。(3) The current sensor according to claim 2, wherein the oscillation circuit is a multivibrator.
特徴とする特許請求の範囲第1項、第2項または第3項
に記載の電流センサ。(4) The current sensor according to claim 1, 2, or 3, wherein the magnetic wire is made of an amorphous magnetic material.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1446889A JPH02194363A (en) | 1989-01-24 | 1989-01-24 | Current sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1446889A JPH02194363A (en) | 1989-01-24 | 1989-01-24 | Current sensor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02194363A true JPH02194363A (en) | 1990-07-31 |
Family
ID=11861891
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1446889A Pending JPH02194363A (en) | 1989-01-24 | 1989-01-24 | Current sensor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02194363A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013077483A (en) * | 2011-09-30 | 2013-04-25 | Sankosha Corp | Lightning surge detector, surge protection device and management system for surge protection device |
-
1989
- 1989-01-24 JP JP1446889A patent/JPH02194363A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013077483A (en) * | 2011-09-30 | 2013-04-25 | Sankosha Corp | Lightning surge detector, surge protection device and management system for surge protection device |
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