JPS6361170A - Shape of magnetic core in current sensor - Google Patents
Shape of magnetic core in current sensorInfo
- Publication number
- JPS6361170A JPS6361170A JP61204973A JP20497386A JPS6361170A JP S6361170 A JPS6361170 A JP S6361170A JP 61204973 A JP61204973 A JP 61204973A JP 20497386 A JP20497386 A JP 20497386A JP S6361170 A JPS6361170 A JP S6361170A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- gap
- magnetic material
- magnetic 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.)
- Granted
Links
- 239000000696 magnetic material Substances 0.000 claims abstract description 35
- 239000004020 conductor Substances 0.000 claims abstract description 11
- 238000003780 insertion Methods 0.000 claims description 12
- 230000037431 insertion Effects 0.000 claims description 12
- 230000002093 peripheral effect Effects 0.000 claims description 3
- 230000004907 flux Effects 0.000 abstract description 12
- 238000001514 detection method Methods 0.000 abstract description 9
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 abstract description 4
- 229910052802 copper Inorganic materials 0.000 abstract description 4
- 239000010949 copper Substances 0.000 abstract description 4
- 230000000694 effects Effects 0.000 abstract description 4
- 238000010586 diagram Methods 0.000 description 3
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
Landscapes
- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
- Measurement Of Current Or Voltage (AREA)
Abstract
Description
【発明の詳細な説明】
発明の目的
(産業上の利用分野)
本発明はバッテリー駆動車両等に用いられる電流センサ
における磁気コアの形状に関するものである。DETAILED DESCRIPTION OF THE INVENTION Object of the Invention (Field of Industrial Application) The present invention relates to the shape of a magnetic core in a current sensor used in a battery-driven vehicle or the like.
(従来の技術)
従来、第4図、第5図に示すように左右対称に形成した
口字状のコア40.41を相対向配置し、周回状の磁路
の上下に二つのギャップ42.43を設けるようにした
磁気コア44がある。これは、磁路の各部の断面が一辺
の長さT1の正四角形となるようになっている。(Prior Art) Conventionally, as shown in FIGS. 4 and 5, symmetrically formed opening-shaped cores 40, 41 are arranged facing each other, and two gaps 42, 41 are formed above and below a circumferential magnetic path. There is a magnetic core 44 in which a magnetic core 43 is provided. The cross section of each part of the magnetic path is a regular square with a side length T1.
又、第6図に示すように前記一方のギャップ43をなく
し、周回状の磁路に対しギャップ42だけを設けた磁気
コア45、あるいは、第7図に示すように断面が直径T
1の円形状になる荒型の磁気コア46にギャップ42を
設けたものがある。Also, as shown in FIG. 6, a magnetic core 45 in which one gap 43 is eliminated and only a gap 42 is provided for the circular magnetic path, or a cross section with a diameter T as shown in FIG.
There is one in which a gap 42 is provided in a rough magnetic core 46 having a circular shape.
そして、それらを電流センサとして用いるときには、各
磁気コア44.45.46の中心部に形成される挿通部
47に対し電流が流される導体を配置する。そして、前
記導体から同導体に流れる電流に比例して発生し、各磁
気コア44.45゜46に集められる磁束を測定すべく
ギャップ42に対し例えばホール素子のような磁電変換
素子を配置している。When using them as a current sensor, a conductor through which a current flows is arranged in the insertion portion 47 formed at the center of each magnetic core 44, 45, 46. A magnetoelectric transducer, such as a Hall element, is arranged in the gap 42 in order to measure the magnetic flux generated in proportion to the current flowing from the conductor to the conductor and collected in each magnetic core 44.45° 46. There is.
(発明が解決しようとする問題点)
ところが、上記第4図に示す磁気コア44においては効
率がよいため小型化は可能であるが、その磁気回路上の
等価回路が第8図に示すように二つのギャップ42.4
3において磁気抵抗Rm1゜Rm2が形成される。従っ
て、磁気コア44の側面から同磁気コア44内に外部磁
気ノイズが入ると、その外部磁気ノイズが前記磁電変換
素子を配置したギャップ42とギャップ43の両方に流
れるため、前記磁電変換素子による測定結果が外部磁気
ノイズに影響されやすいといった問題がある。(Problems to be Solved by the Invention) However, although the magnetic core 44 shown in FIG. 4 has good efficiency and can be miniaturized, the equivalent circuit on the magnetic circuit is as shown in FIG. two gaps 42.4
3, magnetic resistances Rm1°Rm2 are formed. Therefore, when external magnetic noise enters into the magnetic core 44 from the side surface of the magnetic core 44, the external magnetic noise flows into both the gap 42 and the gap 43 where the magnetoelectric transducer is arranged, so that the magnetoelectric transducer can measure the noise. There is a problem that the results are easily influenced by external magnetic noise.
又、第6図に示す磁気コア45においてはそのその磁気
回路上の等価回路が第9図に示すようにギャップ42に
おいてのみ磁気抵抗Rm1が形成されるため、外部磁気
ノイズが磁気コア45内に入ってもその外部磁気ノイズ
は回路下側に設けた短絡部分を主に流れるため、ギャッ
プ42に配置した前記磁電変換素子による測定結果が外
部磁気ノイズに影響されにくいといった利点がある。し
かし、その半面、この磁気コア45は効率が前記第4図
に示す磁気コア44に比べよくないため、大型化すると
いった問題がある。Furthermore, in the magnetic core 45 shown in FIG. 6, the magnetic resistance Rm1 is formed only in the gap 42, as shown in FIG. Even if the external magnetic noise enters the circuit, the external magnetic noise mainly flows through the short-circuited portion provided at the bottom of the circuit, so there is an advantage that the measurement result by the magnetoelectric transducer arranged in the gap 42 is not easily influenced by the external magnetic noise. However, on the other hand, the efficiency of this magnetic core 45 is not as good as that of the magnetic core 44 shown in FIG. 4, so there is a problem that it becomes larger.
第7図に示す磁気コア46は前記磁気コア45と同じ利
点と問題点を持つばかりか、さらに、その形状から基板
に対する取付性がよくないといった問題がある。The magnetic core 46 shown in FIG. 7 not only has the same advantages and problems as the magnetic core 45, but also has the problem that it is not easy to attach to a substrate due to its shape.
なお、一般に第10図に示すように導体に流れる電流が
大きくなるとギャップ42における磁束密度が飽和点4
9において飽和し、電流の検出範囲上限付近における検
出精度が悪くなる。又、温度の変化によって磁束密度の
飽和点が飽和点50のように変動し、破線のように磁束
密度が低下することがある。そして、第11図に示すよ
うに電流の検出範囲上限付近においてもギャップ42に
おける磁束密度の直線性を確保するには、単純に磁気コ
アを大きくすればよいことが知られている。Generally, as shown in FIG. 10, when the current flowing through the conductor increases, the magnetic flux density in the gap 42 reaches the saturation point 4.
9, the detection accuracy deteriorates near the upper limit of the current detection range. Further, due to temperature changes, the saturation point of the magnetic flux density may vary as shown in the saturation point 50, and the magnetic flux density may decrease as shown by the broken line. As shown in FIG. 11, it is known that in order to ensure the linearity of the magnetic flux density in the gap 42 even near the upper limit of the current detection range, it is sufficient to simply increase the size of the magnetic core.
そこで、この発明の目的は所定の電流の検出範囲を確保
するとともに、小型でしかも外部磁気ノイズに対しても
影響の受けにくい磁気コアを提供することにある。SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a magnetic core that secures a predetermined current detection range, is small in size, and is less susceptible to external magnetic noise.
発明の構成
(問題点を解決するための手段)
そこで、本発明は前記問題点を解決するためになされた
ものであって、直方体状に形成した磁性材料の中心部に
対し、電流が流される導体を挿通ずる挿通部を設けると
ともに、その挿通部の四方の磁性材からなる周回状の磁
路を形成し、その−方の磁性材にはギャップを切欠形成
するとともに、その磁性材を他の磁性材より肉薄形成し
たものである。Structure of the Invention (Means for Solving the Problems) Therefore, the present invention has been made to solve the above problems, in which a current is passed through the center of a magnetic material formed in the shape of a rectangular parallelepiped. In addition to providing an insertion part through which the conductor is inserted, a circular magnetic path is formed by magnetic material on the four sides of the insertion part, and a gap is cut out in the magnetic material on that side, and the magnetic material is connected to the other magnetic material. It is made thinner than magnetic material.
(作用)
上記構成により、磁気コアはギャップが設けられた磁性
材が他の磁性材より肉薄形成されることにより小型化さ
れるとともに、挿通部に対し挿通された導体に流される
電流に比例して生じた磁束が四方の磁性材からなる周回
状の磁路に集められる。(Function) With the above configuration, the magnetic core is made smaller because the magnetic material provided with the gap is formed thinner than other magnetic materials, and the current flowing through the conductor inserted into the insertion portion is proportional to the current flowing through the conductor. The magnetic flux generated is collected in a circular magnetic path made of magnetic material on all sides.
(実施例)
以下、この発明を具体化した一実施例について第1図か
ら第3図に従って説明する。(Embodiment) An embodiment embodying the present invention will be described below with reference to FIGS. 1 to 3.
図面中、直方体状の磁性材料からなる磁気コア1の中央
部には、被検出電流が流される導体としての銅バー2が
挿通される挿通部3が形成されている。従って、前記磁
気コア1は四方の磁性材4゜5.6.7にて周回状の磁
路を形成するようになっており、その磁気コア1の上部
にあたる磁性材7の中央部にはギャップ8が切欠形成さ
れている。In the drawing, an insertion part 3 is formed in the center of a rectangular parallelepiped magnetic core 1 made of a magnetic material, into which a copper bar 2 serving as a conductor through which a current to be detected is passed is inserted. Therefore, the magnetic core 1 forms a circular magnetic path with four magnetic materials 4°, 5, 6, 7, and there is a gap in the center of the magnetic material 7 at the top of the magnetic core 1. 8 is notched.
前記ギャップ8に対応する磁性材7の一方の端面9には
磁電変換素子として用いられるホール素子10が配設さ
れている。前記磁性材7の上部を切欠いて形成した取付
段部11には回路基板12が取着され、同回路基板12
には前記ホール素子10からの信号に基づいて前記銅バ
ー2に流れる電流を演算する集積回路13等が設けられ
ている。A Hall element 10 used as a magnetoelectric conversion element is disposed on one end surface 9 of the magnetic material 7 corresponding to the gap 8. A circuit board 12 is attached to a mounting step 11 formed by cutting out the upper part of the magnetic material 7.
is provided with an integrated circuit 13 and the like that calculates the current flowing through the copper bar 2 based on the signal from the Hall element 10.
そして、前記磁気コア1.ホール素子10.回路基板1
2等から電流センサが構成される。The magnetic core 1. Hall element 10. circuit board 1
A current sensor is constructed from the second class.
又、磁気コア1の上部に取付段部11を切欠形成したこ
とにより、ギャップ8が設けられていない各磁性材4.
5.6の各断面寸法T2.T3゜T4は等しく、かつ、
ギャップ8が設けられた磁性材7の断面寸法T5より大
きくなっている。Moreover, by forming the mounting step portion 11 in the upper part of the magnetic core 1, each magnetic material 4. without the gap 8 is formed.
5.6 each cross-sectional dimension T2. T3°T4 are equal, and
It is larger than the cross-sectional dimension T5 of the magnetic material 7 in which the gap 8 is provided.
なお、前記磁性材4.5.6.7のギャップ8方向の幅
T6は前記断面寸法T2.T3.T4より大きくするこ
とにより飽和点が上昇するが、T6>2xT2 (T3
.T4)以後はその効果が小さくなるため、同幅T6は
本実施例では前記断面寸法T2.T3.T4のほぼ2倍
となるように設けられている。Note that the width T6 of the magnetic material 4.5.6.7 in the gap 8 direction is equal to the cross-sectional dimension T2. T3. The saturation point rises by making it larger than T4, but T6>2xT2 (T3
.. Since the effect becomes smaller after T4), the same width T6 is equal to the cross-sectional dimension T2.T4) in this embodiment. T3. It is provided so that it is approximately twice as large as T4.
又、前記挿通部3の内面コーナー部には磁気抵抗を小さ
くし、磁気コア1が小型化されるように周面R1,R2
,R3,R4が設けられている。Further, the inner corner portions of the insertion portion 3 are provided with circumferential surfaces R1 and R2 to reduce magnetic resistance and to downsize the magnetic core 1.
, R3, and R4 are provided.
このように、この磁気コア1においては磁路に対し1つ
のギャップ8だけを設けているため、ホール素子10に
よる電流検出に外部磁気ノイズの影響が生じにくく、正
確な電流検出が行える。又、磁性材7の断面寸法T5は
他の磁性材4,5.6の断面寸法T2.T3.T4より
小さくしたため、この磁気コア1は小型でありながらギ
ャップ8における磁束密度の飽和点を高くできる。さら
に、挿通部3の内面コーナー部に設けた周面R1,R2
、R3,R4によって前記磁束密度の飽和点を高くでき
、又、磁性材4,5.6.7のギャップ8方向の幅T6
は前記断面寸法T2.T3.T4のほぼ2倍となるよう
に設けたため、磁気コア1を大型化することなくさらに
前記磁束密度の飽和点を高くできる。In this way, in this magnetic core 1, only one gap 8 is provided with respect to the magnetic path, so that the current detection by the Hall element 10 is hardly affected by external magnetic noise, and accurate current detection can be performed. Also, the cross-sectional dimension T5 of the magnetic material 7 is the cross-sectional dimension T2 of the other magnetic materials 4, 5.6. T3. Since the magnetic core 1 is made smaller than T4, the saturation point of the magnetic flux density in the gap 8 can be made high even though the magnetic core 1 is small. Further, peripheral surfaces R1 and R2 provided at the inner corner portions of the insertion portion 3
, R3, R4 can increase the saturation point of the magnetic flux density, and also increase the width T6 of the magnetic material 4, 5.6.7 in the gap 8 direction.
is the cross-sectional dimension T2. T3. Since it is provided so as to be approximately twice T4, the saturation point of the magnetic flux density can be further increased without increasing the size of the magnetic core 1.
従って、この磁気コア1においては所定の正確な電流検
出範囲を確保しつつ小型でしかも外部磁気ノイズに対し
ても影響を受けにくい。Therefore, this magnetic core 1 is small while ensuring a predetermined accurate current detection range, and is less susceptible to external magnetic noise.
なお、この発明は前記実施例に限定されるものではなく
、挿通部3の内面コーナー部に周面R1゜R2,R3,
R4を設けないで実施したり、磁性材4,5,6.7の
ギャップ8方向の幅T6を変更して実施したりする等こ
の発明の趣旨から逸脱しない範囲で任意に変更してもよ
い。Note that the present invention is not limited to the above-mentioned embodiments, and the inner corner portion of the insertion portion 3 has peripheral surfaces R1°R2, R3,
Any changes may be made without departing from the spirit of the invention, such as without providing R4 or by changing the width T6 of the magnetic members 4, 5, 6.7 in the gap 8 direction. .
発明の効果
以上詳述したように、本発明においては所定の正確な電
流検出範囲を確保するとともに、小型でしかも外部磁気
ノイズに対しても影響の受けにくい磁気コアを提供する
ことができるという産i利゛用上優れた効果を秦する。Effects of the Invention As detailed above, the present invention has the advantage of ensuring a predetermined accurate current detection range and providing a magnetic core that is small and less susceptible to external magnetic noise. It has excellent effects when used.
第1図から第3図は本発明を具体化した一実施例を示し
、第1図は電流センサの要部を示す図、第2図は磁気コ
アの正面図、第3図は磁気コアの側面図、第4図から第
7図は従来の磁気コアを示し、第4図は磁気コアの正面
図、第5図は磁気コアの側面図、第6図は磁気コアの正
面図、第7因は荒型の磁気コアの正面図、第8図は磁気
コアの等価回路を示す図、第9図は同じく磁気コアの等
価回路を示す図、第10図は被検出電流とギャップにお
ける磁束密度を示す図、第11図は同じく被検出電流と
ギャップにおける磁束密度を示す図である。
1は磁気コア、2は導体としての銅バー、3は挿通部、
4.5,6.7は磁性材、8はギャップである。1 to 3 show an embodiment embodying the present invention, FIG. 1 is a diagram showing the main parts of the current sensor, FIG. 2 is a front view of the magnetic core, and FIG. 3 is a diagram of the magnetic core. 4 to 7 show conventional magnetic cores, FIG. 4 is a front view of the magnetic core, FIG. 5 is a side view of the magnetic core, and FIG. 6 is a front view of the magnetic core. The reason is the front view of the rough magnetic core, Figure 8 shows the equivalent circuit of the magnetic core, Figure 9 shows the equivalent circuit of the magnetic core, and Figure 10 shows the detected current and magnetic flux density in the gap. FIG. 11 is a diagram similarly showing the detected current and the magnetic flux density in the gap. 1 is a magnetic core, 2 is a copper bar as a conductor, 3 is an insertion part,
4.5 and 6.7 are magnetic materials, and 8 is a gap.
Claims (1)
が流される導体を挿通する挿通部を設けるとともに、そ
の挿通部の四方の磁性材からなる周回状の磁路を形成し
、その一方の磁性材にはギャップを切欠形成するととも
に、その磁性材を他の磁性材より肉薄形成した電流セン
サにおける磁気コアの形状。 2、挿通部の内面コーナー部には周面が設けられたもの
である特許請求の範囲第1項記載の電流センサにおける
磁気コアの形状。 3、磁性材のギャップ方向の幅は磁性材の肉厚より大き
くしたものである特許請求の範囲第1項又は第2項のう
ちいずれか一項記載の電流センサにおける磁気コアの形
状。[Scope of Claims] 1. An insertion part through which a conductor through which current is passed is provided in the center of the magnetic material formed in the shape of a rectangular parallelepiped, and a circular magnetic path made of the magnetic material on the four sides of the insertion part. A magnetic core shape in a current sensor in which one of the magnetic materials is formed with a gap cut out, and the magnetic material is thinner than the other magnetic material. 2. The shape of the magnetic core in the current sensor according to claim 1, wherein the inner corner of the insertion portion is provided with a peripheral surface. 3. The shape of the magnetic core in the current sensor according to claim 1 or 2, wherein the width of the magnetic material in the gap direction is larger than the thickness of the magnetic material.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61204973A JPH0690226B2 (en) | 1986-08-30 | 1986-08-30 | Shape of magnetic core in current sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61204973A JPH0690226B2 (en) | 1986-08-30 | 1986-08-30 | Shape of magnetic core in current sensor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6361170A true JPS6361170A (en) | 1988-03-17 |
JPH0690226B2 JPH0690226B2 (en) | 1994-11-14 |
Family
ID=16499360
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61204973A Expired - Lifetime JPH0690226B2 (en) | 1986-08-30 | 1986-08-30 | Shape of magnetic core in current sensor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0690226B2 (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0599953A (en) * | 1991-10-04 | 1993-04-23 | Mitsubishi Electric Corp | Electric current detector |
JP2008145352A (en) * | 2006-12-12 | 2008-06-26 | Jeco Co Ltd | Current sensor and current detecting method |
JP2012163401A (en) * | 2011-02-04 | 2012-08-30 | Aisan Ind Co Ltd | Current sensor |
JP2014219221A (en) * | 2013-05-01 | 2014-11-20 | 富士通コンポーネント株式会社 | Current sensor |
JP2015210272A (en) * | 2014-04-28 | 2015-11-24 | タイコ エレクトロニクス アンプ コリア カンパニーTyco Electronics AMP Korea Co.,Ltd | Hybrid current sensor assembly |
US11204373B2 (en) | 2019-02-27 | 2021-12-21 | Mitsubishi Electric Corporation | Electric power converting apparatus |
-
1986
- 1986-08-30 JP JP61204973A patent/JPH0690226B2/en not_active Expired - Lifetime
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0599953A (en) * | 1991-10-04 | 1993-04-23 | Mitsubishi Electric Corp | Electric current detector |
JP2008145352A (en) * | 2006-12-12 | 2008-06-26 | Jeco Co Ltd | Current sensor and current detecting method |
JP2012163401A (en) * | 2011-02-04 | 2012-08-30 | Aisan Ind Co Ltd | Current sensor |
JP2014219221A (en) * | 2013-05-01 | 2014-11-20 | 富士通コンポーネント株式会社 | Current sensor |
JP2015210272A (en) * | 2014-04-28 | 2015-11-24 | タイコ エレクトロニクス アンプ コリア カンパニーTyco Electronics AMP Korea Co.,Ltd | Hybrid current sensor assembly |
US11204373B2 (en) | 2019-02-27 | 2021-12-21 | Mitsubishi Electric Corporation | Electric power converting apparatus |
Also Published As
Publication number | Publication date |
---|---|
JPH0690226B2 (en) | 1994-11-14 |
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