JP2867276B2 - Current detector - Google Patents

Current detector

Info

Publication number
JP2867276B2
JP2867276B2 JP1309279A JP30927989A JP2867276B2 JP 2867276 B2 JP2867276 B2 JP 2867276B2 JP 1309279 A JP1309279 A JP 1309279A JP 30927989 A JP30927989 A JP 30927989A JP 2867276 B2 JP2867276 B2 JP 2867276B2
Authority
JP
Japan
Prior art keywords
current
current detector
magnetic
ferromagnetic
core
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
JP1309279A
Other languages
Japanese (ja)
Other versions
JPH03170873A (en
Inventor
洋 阿部
紀久夫 敦賀
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.)
TOOKIN KK
Original Assignee
TOOKIN 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 TOOKIN KK filed Critical TOOKIN KK
Priority to JP1309279A priority Critical patent/JP2867276B2/en
Publication of JPH03170873A publication Critical patent/JPH03170873A/en
Application granted granted Critical
Publication of JP2867276B2 publication Critical patent/JP2867276B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は,電子機器または電気機械等に使用される電
流検出器に関するもので,特にトロイダル状強磁性体コ
アの一部にギャップを設け該ギャップ内に感磁素子を構
成した方式の電流検出器の強磁性体コアの構成に関する
ものである。
Description: BACKGROUND OF THE INVENTION The present invention relates to a current detector used for an electronic device, an electric machine, or the like, and more particularly to a current detector provided with a gap in a part of a toroidal ferromagnetic core. The present invention relates to a configuration of a ferromagnetic core of a current detector in which a magnetic sensing element is formed in a gap.

[従来の技術] 従来,この種の電流検出器(第2図)に於いては,磁
気回路を形成する部分に使用されている強磁性体コア3
には,特に検出電流範囲を広げるために飽和磁束密度の
高い強磁性材料Aまたは検出誤差を小さくするために保
磁力の小さい強磁性材料Bが使用され,,ホール素子,ま
たは磁気抵抗効果素子のような感磁素子2を挿入する磁
気ギャップ1を形成し,その磁気ギャップ1に感磁素子
2を挿入して貫通電鍵5に流れる被測定電流に比例した
磁界が発生する磁気ギャップ1内に挿入した感磁素子2
により,電流の大きなに比例した出力電圧を得ている。
[Prior Art] Conventionally, in a current detector of this kind (FIG. 2), a ferromagnetic core 3 used in a portion forming a magnetic circuit is used.
In particular, a ferromagnetic material A having a high saturation magnetic flux density or a ferromagnetic material B having a small coercive force to reduce a detection error is used for expanding a detection current range. A magnetic gap 1 for inserting such a magnetic sensing element 2 is formed, and the magnetic sensing element 2 is inserted into the magnetic gap 1 and inserted into the magnetic gap 1 in which a magnetic field proportional to a measured current flowing through the through key 5 is generated. Magneto-sensitive element 2
As a result, an output voltage proportional to a large current is obtained.

感磁素子2で検出した貫通電線5の電流に比例した出
力電圧は,信号増幅回路によって増幅されて電流の大き
さに比例した出力電圧を得,貫通電流の大きさを検出し
ている。
The output voltage proportional to the current of the through wire 5 detected by the magnetic sensing element 2 is amplified by a signal amplifier circuit to obtain an output voltage proportional to the magnitude of the current, and the magnitude of the through current is detected.

[発明が解決しようとする課題] しかしながら,従来の電流検出器に於いて,磁気回路
を形成する部分に使用されている強磁性体コアの飽和磁
束密度は直接検出電流範囲に影響し,この強磁性体の飽
和磁束密度とコアの形状によって感度及び検出電流範囲
が一対象に限定設計されていた。そのために分解能が必
要な小電流範囲で高感度を得る為に磁気ギャップを小さ
くすると,強磁性体コアが飽和しやすくなり,十分な電
流検出範囲が得られなかった。又大電流範囲がリニヤリ
ティを上げるため磁気ギャップを大きくすると小電流範
囲の出力が小さいため,大電流検出と小電流検出は別々
の電流検出器が必要であった。
[Problems to be Solved by the Invention] However, in a conventional current detector, the saturation magnetic flux density of a ferromagnetic core used in a portion forming a magnetic circuit directly affects a detection current range. The sensitivity and the range of the detected current are designed to be limited to one target depending on the saturation magnetic flux density of the magnetic material and the shape of the core. Therefore, if the magnetic gap is reduced to obtain high sensitivity in a small current range where resolution is required, the ferromagnetic core is easily saturated, and a sufficient current detection range cannot be obtained. When the magnetic gap is increased to increase the linearity of the large current range, the output of the small current range is small when the magnetic gap is increased. Therefore, separate detection of the large current and the small current is required.

[課題を解決するための手段] 本発明によれば,従来のかかる欠点を除くため,トロ
イダル状強磁性体コアの磁路の一部にギャップを設け,
該ギャップ内に感磁素子を挿入構成した電流検出器の強
磁性体コアにおいて,該強磁性体コアの中央部分に飽和
磁束密度の異なる他の強磁性材料を直列に挿入すること
によって二種類以上の強磁性材料の直列接続でコアを構
成し,二段階以上の感度を持つことを特徴とする電流検
出器が得られる。
[Means for Solving the Problems] According to the present invention, a gap is provided in a part of the magnetic path of the toroidal ferromagnetic core to eliminate the conventional disadvantage.
In a ferromagnetic core of a current detector having a magneto-sensitive element inserted in the gap, two or more types of ferromagnetic materials having different saturation magnetic flux densities are inserted in series at the center of the ferromagnetic core. A current detector characterized in that the core is constituted by a series connection of the above ferromagnetic materials and has a sensitivity of two or more stages.

[発明の構成] トロイダル状の強磁性体コアの磁路の一部にギャップ
を設け該ギャップ内に感磁素子を挿入構成した電流検出
器の強磁性体コアに於いて,第1図に示すように飽和磁
束密度の高い強磁性材料Aで形成するトロイダル状の強
磁性体コア3のコア中央部に飽和磁束密度の低い磁性材
料Bの薄板を挿入し,二種類あるいは低い磁性材料Bの
薄板挿入し,二種類あるいはそれ以上の磁性材料の直列
接続でコアを構成する。
[Constitution of the Invention] FIG. 1 shows a ferromagnetic core of a current detector in which a gap is provided in a part of a magnetic path of a toroidal ferromagnetic core and a magneto-sensitive element is inserted into the gap. As described above, a thin plate of a magnetic material B having a low saturation magnetic flux density is inserted into the center of the core of a toroidal ferromagnetic core 3 formed of a ferromagnetic material A having a high saturation magnetic flux density. The core is inserted and two or more magnetic materials are connected in series.

[作用] 第1図のように構成したコアを用いた電流検出器は強
磁性材料Bが磁気飽和点に至るまでの感度は,磁気ギャ
ップ長さLg貫通電線巻数N,検出電流Iによって(NI/
Lg)に比例する。磁性材料Bが飽和した後,磁性材料B
部分には,それ以上の磁束は通らず,等価的に磁気ギャ
ップと見なすことができ,強磁性体コアは第1図(b)
と同等な動作をする。よって強磁性材料Bが飽和した後
の感度は,(NI/Lg+L2)に比例する。以後の強磁性材
料Aが飽和に至るまでリニアな出力を得ることができ
る。また,磁性材料Aの飽和点は磁気ギャップが等価的
に拡大したことにより伸び,検出電流検出器範囲は広く
なる。
[Operation] current detector using a configuration cores as in the first figure the sensitivity to ferromagnetic material B reaches the magnetic saturation point, the magnetic gap length L g through wire turns N, the detected current I ( NI /
L g ). After the magnetic material B is saturated, the magnetic material B
No magnetic flux passes through the portion, and it can be regarded as equivalent to a magnetic gap.
Works the same as. Therefore sensitivity after ferromagnetic material B is saturated it is proportional to (NI / L g + L 2 ). A linear output can be obtained until the subsequent ferromagnetic material A reaches saturation. Further, the saturation point of the magnetic material A is extended due to the magnetic gap being enlarged equivalently, and the range of the detection current detector is widened.

[実施例] 実施例について図面を参照して説明すると,第2図は
従来の電流検出器の構成正面図である。トロイダル状の
強磁性体コア23に被測定電流を流す貫通電線5を貫通さ
せ,該貫通電線5の電流によって生じる磁束を強磁性体
コア3が集束し,該強磁性体コア3の磁気ギャップ1の
空間に磁束を生じさせ,磁気ギャップ1の磁束を感磁素
子を2にて磁束の強さを測定するものである。この第2
図の電流検出器の感度は,(NI/Lg)に比例する。第2
図の強磁性体コアに方向性硅素鋼を用いたときの入出力
特性を第3図破線で示す。
[Embodiment] An embodiment will be described with reference to the drawings. FIG. 2 is a configuration front view of a conventional current detector. A through wire 5 for passing a current to be measured is passed through the toroidal ferromagnetic core 23, and a magnetic flux generated by the current of the through wire 5 is focused by the ferromagnetic core 3, and a magnetic gap 1 of the ferromagnetic core 3 is formed. A magnetic flux is generated in the space, and the magnetic flux of the magnetic gap 1 is measured by the magneto-sensitive element 2 to measure the intensity of the magnetic flux. This second
The sensitivity of the current detector in the figure is proportional to (NI / L g ). Second
The input / output characteristics when a directional silicon steel is used for the ferromagnetic core in the figure are shown by broken lines in FIG.

第1図に本発明電流検出器の強磁性体コア構成一実施
例を示す。強磁性体Aに飽和磁束密度が高い強磁性材料
である方向性硅素鋼,強磁性体Bに飽和磁束密度が低い
強磁性材料であるパーマロイを用いえ図1の様な強磁性
体コアを構成している。第3図において,実線で本実施
例のコアを用いた電流検出器の入出力特性が示されてい
る。第3図において,点Pまで,パーマロイ部はコアの
一部として動作し,その感度は(NI/Lg)に比例する。
第3図点P〜Lではパーマロイ部は飽和して磁気ギャッ
プと等価になり,電流検出器の感度は(NI/Lg+L2)に
比例し,この区間の出力もリニアである。感度は磁気ギ
ャップが増えた分低下したことにより,硅素鋼のみで構
成した電流検出器の検出電流範囲が第3図A1であったも
のが,実施例の電流検出器では第3図A2まで検出電流範
囲が広くなっている。
FIG. 1 shows an embodiment of a ferromagnetic core configuration of the current detector according to the present invention. A ferromagnetic core as shown in FIG. 1 is formed by using directional silicon steel, which is a ferromagnetic material having a high saturation magnetic flux density, as the ferromagnetic material A, and permalloy, which is a ferromagnetic material having a low saturation magnetic flux density, as the ferromagnetic material B. doing. In FIG. 3, the solid line shows the input / output characteristics of the current detector using the core of this embodiment. In FIG. 3, up to point P, the permalloy operates as part of the core, and its sensitivity is proportional to (NI / L g ).
Permalloy portion in FIG. 3 point P~L becomes magnetic gap equivalent saturated, the sensitivity of the current detector is proportional to (NI / L g + L 2 ), the output of this leg is also linear. The sensitivity was reduced by the increase of the magnetic gap, and the current detection range of the current detector composed of only silicon steel was A1 in Fig. 3, but the current detector of the embodiment detected up to A2 in Fig. 3. The current range is wide.

図1のように構成したコアを用いた電流検出器はパー
マロイ部分が飽和する点(変極点)を境に二段階の感度
を持ち,これにより分解能の必要な小電流範囲での高感
度特性と大電流範囲用の広い電流検出範囲を合わせ持つ
電流検出器の提供が可能となった。
The current detector using the core configured as shown in Fig. 1 has two stages of sensitivity at the point where the permalloy portion saturates (inflection point), thereby achieving high sensitivity characteristics in a small current range where resolution is required. It has become possible to provide a current detector having a wide current detection range for a large current range.

[発明の効果] 以上のように,分解能が必要な小電流範囲では従来の
感度を保ち,大電流範囲で感度を落とすことで検出電流
範囲をリニアに拡大することができる。又この電流検出
器の感度の変極点及び変極点以後の傾きは,挿入する強
磁性体Bの種類及び厚さ(L2)を選択することにより任
意に設定することができる。この二段階の感度を持つ電
流検出器は分解能が必要な小電流電流検出器と,大電流
までリニアな出力が必要な大電流検出器の特徴を合わせ
持つため,一つの電流検出器の外に大電流検出用貫通電
線及び小電流検出用貫通電線を巻くことにより一つの電
流検出器で大電流検出と小電流検出をかねることがで
き,産業上有益な発明である。
[Effects of the Invention] As described above, the conventional sensitivity is maintained in the small current range where resolution is required, and the detection current range can be linearly expanded by lowering the sensitivity in the large current range. The inflection point and the inclination after the inflection point of the sensitivity of the current detector can be arbitrarily set by selecting the type and thickness (L 2 ) of the ferromagnetic substance B to be inserted. This two-stage sensitivity current detector combines the characteristics of a small current detector that requires resolution and a large current detector that requires a linear output up to a large current. By winding a through-wire for detecting a large current and a through-wire for detecting a small current, it is possible to detect both a large current and a small current with a single current detector, which is an industrially useful invention.

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

第1図(a)は本発明の電流検出器の強磁性体コア部
分,第1図(b)は第1図(a)の強磁性体Bを除いた
状態を示す図,第2図は一般に用いられている電流検出
器の構成を示す構成正面図,第3図は電流検出器の入出
力特性を示す図である。なお,実線は本発明の一実施例
の強磁性体コアを用いた電流検出器を示す。 1……磁気ギャップ,2……感磁素子,3……強磁性材料A
(方向性硅素鋼),4……強磁性材料B(パーマロイ),5
……貫通電線,……回路部品,7……回路実装基板,8……
外部端子。
FIG. 1 (a) shows a ferromagnetic core portion of the current detector of the present invention, FIG. 1 (b) shows a state in which the ferromagnetic material B of FIG. 1 (a) is removed, and FIG. FIG. 3 is a front view showing the configuration of a generally used current detector, and FIG. 3 is a diagram showing input / output characteristics of the current detector. The solid line indicates a current detector using a ferromagnetic core according to one embodiment of the present invention. 1 ... magnetic gap, 2 ... magnetic sensing element, 3 ... ferromagnetic material A
(Oriented silicon steel), 4 ... ferromagnetic material B (permalloy), 5
…… through wire, …… circuit parts, 7 …… circuit board, 8 ……
External terminal.

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.6,DB名) G01R 15/20 G01R 33/06 - 33/09──────────────────────────────────────────────────続 き Continued on front page (58) Field surveyed (Int.Cl. 6 , DB name) G01R 15/20 G01R 33/06-33/09

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】トロイダル状強磁性体コアの磁路の一部に
ギャップを設け,該ギャップ内に感磁素子を挿入構成し
た電流検出器の強磁性体コアにおいて,該強磁性体コア
の中央部分に飽和磁束密度の異なる他の強磁性材料を直
列に挿入することによって二種類以上の強磁性材料の直
列接続でコアを構成し,二段階以上の感度を持つことを
特徴とする電流検出器。
1. A ferromagnetic core of a current detector in which a gap is provided in a part of a magnetic path of a toroidal ferromagnetic core, and a magneto-sensitive element is inserted into the gap. A current detector characterized by having two or more types of ferromagnetic material connected in series by inserting another ferromagnetic material having a different saturation magnetic flux density in series into the core and having two or more levels of sensitivity .
JP1309279A 1989-11-30 1989-11-30 Current detector Expired - Fee Related JP2867276B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1309279A JP2867276B2 (en) 1989-11-30 1989-11-30 Current detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1309279A JP2867276B2 (en) 1989-11-30 1989-11-30 Current detector

Publications (2)

Publication Number Publication Date
JPH03170873A JPH03170873A (en) 1991-07-24
JP2867276B2 true JP2867276B2 (en) 1999-03-08

Family

ID=17991088

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1309279A Expired - Fee Related JP2867276B2 (en) 1989-11-30 1989-11-30 Current detector

Country Status (1)

Country Link
JP (1) JP2867276B2 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102005024075B4 (en) 2005-05-25 2007-04-12 Lisa Dräxlmaier GmbH Method and device for measuring a current flowing in an electrical conductor
DE102005040316B4 (en) 2005-08-25 2007-09-27 Lisa Dräxlmaier GmbH Apparatus and method for measuring a current flowing in an electrical conductor
DE102006032763B4 (en) 2006-07-14 2009-05-07 Lisa Dräxlmaier GmbH Apparatus and method for measuring a current flowing in an electrical conductor
JP2009058451A (en) * 2007-09-03 2009-03-19 Osaki Electric Co Ltd Current sensor-use magnetic core and current sensor employing the same
GB202008170D0 (en) * 2020-06-01 2020-07-15 Secr Defence Injury protection device

Also Published As

Publication number Publication date
JPH03170873A (en) 1991-07-24

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