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JP3305445B2 - Current detector for line current detection - Google Patents

Current detector for line current detection

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Publication number
JP3305445B2
JP3305445B2 JP20874493A JP20874493A JP3305445B2 JP 3305445 B2 JP3305445 B2 JP 3305445B2 JP 20874493 A JP20874493 A JP 20874493A JP 20874493 A JP20874493 A JP 20874493A JP 3305445 B2 JP3305445 B2 JP 3305445B2
Authority
JP
Japan
Prior art keywords
current
magnetic core
line
magnetization state
magnetic
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.)
Expired - Fee Related
Application number
JP20874493A
Other languages
Japanese (ja)
Other versions
JPH0743389A (en
Inventor
秀夫 鈴木
道夫 根本
Original Assignee
エヌイーシートーキン株式会社
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 エヌイーシートーキン株式会社 filed Critical エヌイーシートーキン株式会社
Priority to JP20874493A priority Critical patent/JP3305445B2/en
Publication of JPH0743389A publication Critical patent/JPH0743389A/en
Application granted granted Critical
Publication of JP3305445B2 publication Critical patent/JP3305445B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、電話機、ファックス等
の回線電流検出用電流検出器であって、電流検出器の構
成部品である磁性体コアの磁化状態を初期化することに
よって、検出精度を向上させた電流検出器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a current detector for detecting a line current of a telephone, a facsimile, or the like. The present invention relates to a current detector in which is improved.

【0002】[0002]

【従来の技術】図4に従来の回線電流検出用電流検出器
のブロック図を示す。磁性体コア11の磁路の一部には
空隙31が設けられ、その空隙31内にホール素子41
が設置されており、該ホール素子41の出力電圧が差動
増幅器44を通して増幅され、ついでコンパレータ42
に入力され、前もって設定した被検出電流に対応させた
基準電圧43と差動増幅器44からの出力電圧の比較に
よって、回線電流I1を検出する。図5は、その検出の
原理を示したものである。図5に示すヒステリシス曲線
にて磁性体コア11がB−Hヒステリシス曲線のほぼ原
点に初期化されている。回線に被検出の直流電流が流
れると、それにより磁性体コア11内に起磁力が発生
し、その印加磁場が磁性体コア11の空隙31内に磁場
を発生させる。磁性体コア11の動作点はB−Hヒステ
リシス曲線上を移動し、例えば図5における回線電流I
1にて発生する磁場H1によるホール素子31からの出力
電圧をしきい値としてコンパレータ42の基準電圧43
を設定すれば、図5のヒステリシス曲線のA点にて回線
電流が電流値I1となったことが検出される。一般に、
回線電流は最大で±100mA前後まで流れ、この範囲
内では強磁性体コアの磁化状態、即ちB−Hヒステリシ
ス曲線特性がほぼ直線範囲にある。もし、大きな回線電
流が流れ、動作点が飽和磁化状態のまで達した後、回
線電流が遮断されると、動作点はヒステリシス曲線に沿
って残留磁化状態のへ達して保持される。このの状
態は明かに前の初期のの状態とは異なる。従って、再
度前記と同方向の回線電流が流れた場合には、残留磁化
状態のより動作が開始し、ヒステリシス曲線に沿って
磁束Bが増加する。従って、前記のコンパレータ42の
設定点B点で電流検出の出力が得られるが、実際の電流
値は印加磁場H2に相当する回線電流値I2である。よっ
て、図のごとく△H=H1−H2の印加磁場の差に相当す
る電流値△Iが誤差として発生する。本発明は、この誤
差を解消することにある。
2. Description of the Related Art FIG. 4 is a block diagram of a conventional line current detecting current detector. A gap 31 is provided in a part of the magnetic path of the magnetic core 11, and a Hall element 41 is provided in the gap 31.
Is provided, the output voltage of the Hall element 41 is amplified through a differential amplifier 44,
Is input to, by comparing the output voltage from the reference voltage 43 and the differential amplifier 44 to correspond to the detected current set in advance to detect a line current I 1. FIG. 5 shows the principle of the detection. In the hysteresis curve shown in FIG. 5, the magnetic core 11 is initialized to almost the origin of the BH hysteresis curve. When a detected direct current flows through the line, a magnetomotive force is generated in the magnetic core 11, and the applied magnetic field generates a magnetic field in the gap 31 of the magnetic core 11. The operating point of the magnetic core 11 moves on the BH hysteresis curve.
Reference voltage 43 of the comparator 42 the output voltage from the Hall element 31 by a magnetic field H 1 generated by 1 as a threshold
Is set, it is detected that the line current has reached the current value I 1 at the point A of the hysteresis curve in FIG. In general,
The line current flows up to about ± 100 mA at maximum, and within this range, the magnetization state of the ferromagnetic core, that is, the BH hysteresis curve characteristic is in a substantially linear range. If the line current is cut off after a large line current flows and the operating point reaches the saturation magnetization state, the operation point reaches the residual magnetization state along the hysteresis curve and is held. This state is clearly different from the earlier initial state. Therefore, when the line current flows in the same direction again, the operation starts in the residual magnetization state, and the magnetic flux B increases along the hysteresis curve. Thus, the output of the current detected by the set point B point of the comparator 42 is obtained, a line current value I 2 actual current values corresponding to the applied magnetic field H 2. Therefore, as shown in the figure, a current value ΔI corresponding to a difference between applied magnetic fields of ΔH = H 1 −H 2 is generated as an error. The present invention is to eliminate this error.

【0003】[0003]

【発明が解決しようとする課題】本発明が解決しようと
する課題は、電流検出器の主要構成部品である磁性体コ
アがもつB−Hヒステリシス曲線特性の残留磁化状態に
よって、該電流検出器の測定値に誤差が発生する。その
測定値の誤差を解消した電流検出器を供することにあ
る。
SUMMARY OF THE INVENTION The problem to be solved by the present invention is that the residual magnetization state of the BH hysteresis curve characteristic of the magnetic core, which is a main component of the current detector, causes the current detector to fail. An error occurs in the measured value. An object of the present invention is to provide a current detector in which an error in the measured value is eliminated.

【0004】[0004]

【課題を解決するための手段】本発明は、上記問題点を
解決するために、磁性体コア内部の磁化状態を初期化す
るため、(1)ホール素子が磁性体コアに設けられた空
隙内に設置され、該磁性体コアに巻線されたコイル巻線
を流れる回線電流により、該磁性体コア内に発生する磁
束を該ホール素子にて検出し、その出力電圧を回路部に
て回線電流値として測定する電流検出器において、コイ
ル巻線の端子部にスイッチ回路を接続し、該スイッチ回
路によってコイル巻線を被測定回線、あるいは磁性体コ
アを初期化するための初期化用電流供給用の増幅器に切
り換え可能としたことを特徴とする回線電流検出用電流
検出器、及び(2)前記磁性体コアを初期化するために
流す電流は直流であって、前記磁性体コアを少なくとも
B−Hヒステリシス曲線の飽和磁化状態まで推移させる
のに必要な電流値を通電した後、該電流値を零として磁
性体コアの磁化状態を常に同一極性に残留磁化を持つよ
うに初期化することを特徴とする上記(1)の回線電流
検出用電流検出器、及び(3)ホール素子が磁性体コア
に設けられた空隙内に設置され、該磁性体コアに巻線さ
れたコイルを流れる回線電流により、該磁性体コア内に
発生する磁束を該ホール素子にて検出し、その出力電圧
を回路部にて回線電流値として測定する電流検出器にお
いて、該磁性体コアに巻線された第1のコイル部分は回
線電流検出用であって、被測定電流が流れる回線に接続
され、該磁性体コアに巻線された第2のコイル部分は該
磁性体コア内部の磁化状態を初期化させるための直流の
電流が通電可能であって、該磁性体コアを初期化するた
めに流す電流は直流であり、前記磁性体コアを少なくと
もB−Hヒステリシス曲線の飽和磁化状態まで推移させ
るのに必要な電流値を通電した後、該電流値を零として
磁性体コアの磁化状態を常に同一極性に残留磁化を持つ
ように初期化することを特徴とする回線電流検出用電流
検出器、及び(4)上記(1)の磁性体コアの磁化状態
を初期化する電流は交流であって、通電初期において、
その起磁力が、前記磁性体コアの磁化状態をB−Hヒス
テリシス曲線の飽和状態まで交流電流を加えた後、徐々
にその交流電流値を減少させていき、ほぼ零の交流電流
値まで減少させて、前記磁性体コアの磁化状態を残留磁
化が零に近いほぼ原点に初期化することを特徴とする回
線電流検出用電流検出器である。
According to the present invention, in order to solve the above-mentioned problems, in order to initialize a magnetization state inside a magnetic core, (1) a Hall element is provided in a gap provided in the magnetic core. The magnetic flux generated in the magnetic core is detected by the Hall element by the line current flowing through the coil winding wound on the magnetic core, and the output voltage is detected by the circuit unit in the circuit unit. In a current detector to be measured as a value, a switch circuit is connected to a terminal portion of a coil winding, and the switch circuit is used to supply a current for initialization for initializing a coil to be measured or a magnetic core to initialize the coil winding. And (2) a current flowing for initializing the magnetic core is DC, and the magnetic core is connected to at least B- H hysteresis After passing a current value necessary for transitioning to the saturation magnetization state of the curve, the current value is set to zero and the magnetization state of the magnetic core is initialized to always have the same magnetization and residual magnetization. The line current detection current detector of (1) and the Hall element (3) are installed in a gap provided in the magnetic core, and the line current flows through a coil wound around the magnetic core. A first coil portion wound around the magnetic core in a current detector for detecting a magnetic flux generated in the magnetic core by the Hall element and measuring an output voltage thereof as a line current value in a circuit portion; Is for line current detection, is connected to the line through which the current to be measured flows, and the second coil portion wound around the magnetic core is a DC coil for initializing the magnetization state inside the magnetic core. An electric current can be passed through the magnetic body The current flowing to initialize the magnetic core is a direct current, and a current value necessary for causing the magnetic material core to at least transition to the saturation magnetization state of the BH hysteresis curve is applied. A current detector for line current detection, wherein the magnetization state of the body core is always initialized to have the same polarity and residual magnetization, and (4) the magnetization state of the magnetic core described in (1) above is initialized. The current that flows is an alternating current,
After the magnetomotive force increases the magnetization state of the magnetic core to the saturation state of the BH hysteresis curve, the AC current value is gradually reduced, and then the AC current value is gradually reduced to almost zero. Wherein the magnetization state of the magnetic core is initialized to substantially the origin where the residual magnetization is close to zero.

【0005】[0005]

【作用】課題を解決するための第1の方法としては、強
磁性体コアに第1のコイル部分(被検出巻線)、及び第
2のコイル部分(磁性体コア初期化のたの電流通電用の
コイル)を巻線して、前記第2のコイルに直流、あるい
は交流を通電可能にしたので、磁性体コアを初期化する
ことが可能になった。あるいは、第2の方法としては、
第1のコイル部分にスイッチ回路を設け、被測定電流が
流れる該回線、あるいは初期化用電流を供給する回路の
出力端子に切り換えて、第1のコイル部分に磁性体コア
初期化用の特定の直流、あるいは交流電流を通電する方
法であり、磁性体コアに巻線されるコイル部分が一つだ
けで良く、小形化と廉価な電流検出器が提供できる。こ
のような方法によって、磁性体コア内の磁化状態を常に
初期化状態に保ち、被測定電流による磁性体コア内の磁
化状態はその初期化状態から常に起算するので、測定値
が常に安定しており、測定誤差を最小限にすることが可
能である。
As a first method for solving the problems, a first coil portion (detected winding) and a second coil portion (current supply for initializing the magnetic core) are applied to the ferromagnetic core. Coil, and direct current or alternating current can be applied to the second coil, so that the magnetic core can be initialized. Alternatively, as a second method,
A switch circuit is provided in the first coil portion, and the circuit is switched to an output terminal of the line through which the current to be measured flows or a circuit for supplying a current for initialization, and a specific coil for initializing the magnetic core is provided in the first coil portion. This is a method of applying a direct current or an alternating current, and only one coil portion needs to be wound around the magnetic core, so that a downsized and inexpensive current detector can be provided. By such a method, the magnetization state in the magnetic core is always kept in the initialized state, and the magnetization state in the magnetic core due to the measured current is always calculated from the initialized state, so that the measured value is always stable. And it is possible to minimize measurement errors.

【0006】[0006]

【実施例】以下、本発明の実施例について図面を参照し
て説明する。図1(A)は、本発明の電流検出器の一実
施例を示す。磁性体コア1の磁路の一部に空隙3を設け
た磁性体コア1に第1のコイル部分(検出用コイル)2
1、初期化用の第2のコイル部分22が巻線されてい
る。空隙3内にはホール素子4が設置され、その出力電
圧は回路部5aの差動増幅器44により増幅され、コン
パーレータ42によって基準電圧43に対して出力電圧
との比較が行われる。前記検出用の第1のコイル部分2
1は被測定回線に接続される。一方、初期化用の第2の
コイル部分22は磁性体コア1の磁化状態を初期化する
ための電流通電用のコイルであり、回路部5a内の波形
発生器48、増幅器45の出力電流が初期化用の第2の
コイル部分22に通電される。初期化用の第2のコイル
部分22に通電される初期化電流としては、第1の例と
して、一方向の直流電流が1回のみ印加される直流電流
波形[図1(B)記載]、及び第2の例として、時間と
共に減少していく交流電流波形[図1(C)記載]があ
る。図2は、本発明による電流検出器の他の実施例であ
る。図2(A)において、磁性体コア1は前記実施例と
同じ構成であり、一部に空隙3が設けてある。空隙3に
はホール素子4が装着され、又磁性体コア1にコイル巻
線23が巻かれている。切り換えスイッチ6は、コイル
巻線23の端子211及び212を、被測定の回線側及
び初期化電流設定用回路の増幅器45の出力と切り換え
可能となっている。切り換えスイッチ6の切り替えは、
タイミング回路46からの信号によりスイッチ駆動回路
47にて駆動されている。初期化電流については前記第
1の実施例と同様の波形であり、図2(B)の直流によ
る初期化、あるいは図2(C)の交流による初期化の方
法を用いる。切り換えスイッチ6は、有接点方式のスイ
ッチあるいは電子的な切り換えスイッチの方式いずれで
もよい。本実施例によれば、1個のコイル巻線で磁性体
コア1の初期化と被測定電流検出の二つの働きを処理す
ることができ、センサ部分の巻線、及び端子形成工程を
第1実施例より短縮することができる。上記図1
(B)、図1(C)各々の初期化電流の場合の磁性体コ
ア1の磁気特性の状態を示すB−Hヒステリシス曲線を
図3(A)、及び図3(B)に示す。図3(A)には、
X軸に直流の初期化電流による起磁力を用いた場合を示
し、初期化電流印加後は、磁性体コア1の動作点はすべ
て点に残留磁場として保持される。以後、検出状態と
して被測定の回線電流が流れた場合は、図3(A)のB
−Hヒステリシス曲線上の点→の曲線ライン上を移
動し、例えば磁束密度B1に対応する磁場H1が高精度に
検出可能となり、これに対応した回線電流I1が安定に
検出できる。又、図3(B)は交流の初期化電流通電の
場合を示す。特定の初期化電流通電後は、動作点はB−
Hヒステリシス曲線の座標の原点[図3(B)の点]
に落ち着く。それ以後検出状態として、被測定のための
回線電流が流れた場合、磁性体コア1の動作ラインはB
−Hヒステリシス曲線の点→の曲線ライン上を移動
し、磁束密度B2に対応する磁場H2が安定に高精度に検
出される。従来の方法では初期動作点(起算点)がばら
ついているので、回線電流が流れた場合のB−Hヒステ
リシス曲線の動作ループがばらつき、従って後段のコン
パレータ42を通った後の検出電流値がばらつき誤差が
生じるという問題点があった。本発明ではこの点を解決
している。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1A shows an embodiment of the current detector of the present invention. A first coil portion (detection coil) 2 is provided on a magnetic core 1 in which a gap 3 is provided in a part of a magnetic path of the magnetic core 1.
1. A second coil portion 22 for initialization is wound. A Hall element 4 is provided in the air gap 3, and its output voltage is amplified by the differential amplifier 44 of the circuit section 5 a, and the comparator 42 compares the reference voltage 43 with the output voltage. First coil part 2 for detection
1 is connected to the line to be measured. On the other hand, the second coil portion 22 for initialization is a current-carrying coil for initializing the magnetization state of the magnetic core 1, and the output current of the waveform generator 48 and the amplifier 45 in the circuit portion 5a is reduced. Power is supplied to the second coil portion 22 for initialization. Examples of the initializing current supplied to the second coil portion 22 for initialization include, as a first example, a DC current waveform in which a unidirectional DC current is applied only once (described in FIG. 1B), As a second example, there is an alternating current waveform that decreases with time [described in FIG. 1C]. FIG. 2 shows another embodiment of the current detector according to the present invention. In FIG. 2A, a magnetic core 1 has the same configuration as that of the above-described embodiment, and a gap 3 is provided in a part. A hole element 3 is mounted in the gap 3, and a coil winding 23 is wound around the magnetic core 1. The changeover switch 6 is capable of switching the terminals 211 and 212 of the coil winding 23 with the line side to be measured and the output of the amplifier 45 of the initialization current setting circuit. Switching of the changeover switch 6
It is driven by a switch drive circuit 47 by a signal from the timing circuit 46. The initialization current has the same waveform as that of the first embodiment, and the DC initialization method shown in FIG. 2B or the AC initialization method shown in FIG. 2C is used. The changeover switch 6 may be either a contact switch or an electronic changeover switch. According to the present embodiment, the two functions of the initialization of the magnetic core 1 and the detection of the current to be measured can be processed by one coil winding, and the winding of the sensor portion and the terminal formation step are performed in the first step. It can be shorter than the embodiment. Figure 1 above
FIGS. 3A and 3B show BH hysteresis curves showing the state of the magnetic characteristics of the magnetic core 1 at the initialization currents shown in FIGS. 3B and 1C, respectively. In FIG. 3A,
A case where a magnetomotive force generated by a DC initialization current is used on the X axis is shown. After the application of the initialization current, all operating points of the magnetic core 1 are held as residual magnetic fields at all points. Thereafter, when the line current to be measured flows as the detection state, B in FIG.
Moving on the curve line from the point to the −H hysteresis curve →, for example, the magnetic field H 1 corresponding to the magnetic flux density B 1 can be detected with high accuracy, and the line current I 1 corresponding to this can be stably detected. FIG. 3B shows a case in which an AC initialization current is supplied. After the specific initialization current is supplied, the operating point becomes B-
Origin of the coordinates of the H hysteresis curve [point in FIG. 3 (B)]
Calm down. After that, when a line current for measurement flows as a detection state, the operation line of the magnetic core 1 becomes B
Move point → curve line above the -H hysteresis curve, magnetic field H 2 corresponding to the magnetic flux density B 2 is detected stably with high precision. In the conventional method, since the initial operating point (starting point) varies, the operation loop of the BH hysteresis curve when the line current flows varies, and therefore, the detected current value after passing through the comparator 42 at the subsequent stage varies. There is a problem that an error occurs. The present invention solves this point.

【0007】[0007]

【発明の効果】以上、本発明によれば、従来は磁性体コ
ア内の磁化状態は初期時点ではランダムな状態にあり、
回線電流検出値に大きな誤差を生じていた。本発明によ
れば、磁性体コアに特定の初期化電流を通電することに
より、磁性体コア内磁化状態を常に一定の値に設定する
ことができ、従って回線電流検出時の磁性体コアの磁化
動作点の移動が一定の値を経由して行われ、回線電流検
出値の精度が従来に比べ格段に改善される。
As described above, according to the present invention, conventionally, the magnetization state in the magnetic core is initially in a random state,
A large error occurred in the line current detection value. According to the present invention, by supplying a specific initialization current to the magnetic core, the magnetization state in the magnetic core can always be set to a constant value. The movement of the operating point is performed via a certain value, and the accuracy of the line current detection value is remarkably improved as compared with the related art.

【図面の簡単な説明】[Brief description of the drawings]

【図1】図1(A)は本発明による回線電流検出用電流
検出器の第1の実施例を示す回路ブロック図であり、図
1(B)と図1(C)は実施例における磁性体コア1を
初期化するための電流波形。
FIG. 1A is a circuit block diagram showing a first embodiment of a current detector for detecting a line current according to the present invention, and FIGS. 1B and 1C are magnetic circuits in the embodiment. A current waveform for initializing the body core 1.

【図2】図2(A)は本発明による回線電流検出用電流
検出器の第2の実施例を示す回路ブロック図であり、図
2(B)と図2(C)は実施例における磁性体コア1を
初期化するための電流波形。
FIG. 2A is a circuit block diagram showing a second embodiment of a line current detection current detector according to the present invention, and FIGS. 2B and 2C are magnetic circuit diagrams of the embodiment. A current waveform for initializing the body core 1.

【図3】図1又は図2の実施例における磁性体コアの動
作点の初期化を示すB−Hヒステリシス曲線の図で、図
3(A)は直流で初期化するB−Hヒステリシス曲線の
図であり、図3(B)は交流で初期化するB−Hヒステ
リシス曲線の図。
FIG. 3 is a diagram of a BH hysteresis curve showing the initialization of the operating point of the magnetic core in the embodiment of FIG. 1 or FIG. 2, and FIG. 3 (A) is a diagram of the BH hysteresis curve initialized by DC. FIG. 3B is a diagram of a BH hysteresis curve initialized by alternating current.

【図4】従来の回線電流検出用電流検出器の例を示す回
路ブロック図。
FIG. 4 is a circuit block diagram showing an example of a conventional line current detection current detector.

【図5】従来の回線電流検出用電流検出器での磁性体コ
ア内の磁化状態を示すB−Hヒステリシス曲線の図。
FIG. 5 is a BH hysteresis curve showing a magnetization state in a magnetic core in a conventional line current detection current detector.

【符号の説明】[Explanation of symbols]

1,11 磁性体コア 2,21 (検出用の)第1のコイル部分 3,31 空隙 4,41 ホール素子 5a,5b,51 回路部 6 切り換えスイッチ 22 (初期化用の)第2のコイル部分 23 コイル巻線 42 コンパレータ 43 基準電圧 44 差動増幅器 45 増幅器 46 タイミング回路 47 スイッチ駆動回路 48 波形発生器 211,212 コイル巻線23の端子 1,11 Magnetic core 2,21 First coil part (for detection) 3,31 Air gap 4,41 Hall element 5a, 5b, 51 Circuit part 6 Changeover switch 22 Second coil part (for initialization) Reference Signs List 23 Coil winding 42 Comparator 43 Reference voltage 44 Differential amplifier 45 Amplifier 46 Timing circuit 47 Switch driving circuit 48 Waveform generator 211, 212 Terminal of coil winding 23

Claims (4)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 ホール素子が磁性体コアに設けられた空
隙内に設置され、該磁性体コアに巻線されたコイル巻線
を流れる回線電流により、該磁性体コア内に発生する磁
束を該ホール素子にて検出し、その出力電圧を回路部に
て回線電流値として測定する電流検出器において、コイ
ル巻線の端子部にスイッチ回路を接続し、該スイッチ回
路によってコイル巻線を被測定回線、あるいは磁性体コ
アを初期化するための初期化用電流供給用の増幅器に切
り換え可能としたことを特徴とする回線電流検出用電流
検出器。
1. A magnetic sensor according to claim 1, wherein a Hall element is provided in a gap provided in the magnetic core, and a magnetic flux generated in the magnetic core is generated by a line current flowing through a coil winding wound on the magnetic core. In a current detector which detects the output voltage with a Hall element and measures the output voltage as a line current value in a circuit section, a switch circuit is connected to a terminal portion of the coil winding, and the coil winding is connected to the circuit to be measured by the switch circuit. Or a line current detecting current detector capable of switching to an amplifier for supplying an initializing current for initializing a magnetic core.
【請求項2】 前記磁性体コアを初期化するために流す
電流は直流であって、前記磁性体コアを少なくともB−
Hヒステリシス曲線の飽和磁化状態まで推移させるのに
必要な電流値を通電した後、該電流値を零として磁性体
コアの磁化状態を常に同一極性に残留磁化を持つように
初期化することを特徴とする請求項1記載の回線電流検
出用電流検出器。
2. A current flowing to initialize the magnetic core is a direct current, and the magnetic core is supplied with at least B-
After passing a current value necessary for shifting to the saturation magnetization state of the H hysteresis curve, the current value is set to zero and the magnetization state of the magnetic core is initialized to always have the same magnetization and residual magnetization. 2. The current detector for detecting line current according to claim 1, wherein
【請求項3】 ホール素子が磁性体コアに設けられた空
隙内に設置され、該磁性体コアに巻線されたコイルを流
れる回線電流により、該磁性体コア内に発生する磁束を
該ホール素子にて検出し、その出力電圧を回路部にて回
線電流値として測定する電流検出器において、該磁性体
コアに巻線された第1のコイル部分は回線電流検出用で
あって、被測定電流が流れる回線に接続され、該磁性体
コアに巻線された第2のコイル部分は該磁性体コア内部
の磁化状態を初期化させるための直流の電流が通電可能
であって、該磁性体コアを初期化するために流す電流は
直流であり、前記磁性体コアを少なくともB−Hヒステ
リシス曲線の飽和磁化状態まで推移させるのに必要な電
流値を通電した後、該電流値を零として磁性体コアの磁
化状態を常に同一極性に残留磁化を持つように初期化す
ることを特徴とする回線電流検出用電流検出器。
3. A Hall element is provided in a gap provided in a magnetic core, and a magnetic flux generated in the magnetic core by a line current flowing through a coil wound on the magnetic core. In a current detector for detecting the output voltage as a line current value in a circuit section, a first coil portion wound around the magnetic core is used for detecting a line current, and And a second coil portion wound around the magnetic core is capable of passing a DC current for initializing a magnetization state inside the magnetic core. The current flowing to initialize the magnetic core is a direct current, and after passing a current value necessary to cause the magnetic core to at least transition to the saturation magnetization state of the BH hysteresis curve, the current value is set to zero, and The magnetization state of the core is always the same pole A current detector for detecting a line current, wherein the current detector is initialized so as to have residual magnetization.
【請求項4】 前記磁性体コアの磁化状態を初期化する
電流は交流であって、通電初期において、その起磁力
が、前記磁性体コアの磁化状態をB−Hヒステリシス曲
線の飽和状態まで交流電流を加えた後、徐々にその交流
電流値を減少させていき、ほぼ零の交流電流値まで減少
させて、前記磁性体コアの磁化状態を残留磁化が零に近
いほぼ原点に初期化することを特徴とする請求項1に記
載の回線電流検出用電流検出器。
4. A current for initializing the magnetization state of the magnetic core is an alternating current. In the initial stage of energization, the magnetomotive force changes the magnetization state of the magnetic core to a saturation state of a BH hysteresis curve. After applying the current, the AC current value is gradually reduced, and the AC current value is reduced to almost zero, thereby initializing the magnetization state of the magnetic core to the origin where the residual magnetization is close to zero. 2. The current detector for detecting line current according to claim 1, wherein:
JP20874493A 1993-07-30 1993-07-30 Current detector for line current detection Expired - Fee Related JP3305445B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20874493A JP3305445B2 (en) 1993-07-30 1993-07-30 Current detector for line current detection

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20874493A JP3305445B2 (en) 1993-07-30 1993-07-30 Current detector for line current detection

Publications (2)

Publication Number Publication Date
JPH0743389A JPH0743389A (en) 1995-02-14
JP3305445B2 true JP3305445B2 (en) 2002-07-22

Family

ID=16561368

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20874493A Expired - Fee Related JP3305445B2 (en) 1993-07-30 1993-07-30 Current detector for line current detection

Country Status (1)

Country Link
JP (1) JP3305445B2 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1329735B1 (en) 2000-10-26 2009-06-17 The Foundation: The Research Institute of Electric and Magnetic Materials Thin-film magnetic field sensor
JP4204775B2 (en) * 2001-10-12 2009-01-07 財団法人電気磁気材料研究所 Thin film magnetic field sensor
JP5531216B2 (en) * 2010-10-07 2014-06-25 アルプス・グリーンデバイス株式会社 Current sensor
US9704637B2 (en) * 2013-07-15 2017-07-11 Texas Instruments Incorporated Method and apparatus for demagnetizing transformer cores in closed loop magnetic current sensors
CN112881939B (en) * 2021-03-29 2023-06-27 赣南师范大学 Computer circuit detects winding displacement ware

Also Published As

Publication number Publication date
JPH0743389A (en) 1995-02-14

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