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JPH0687067B2 - Magnetic detection device - Google Patents
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JPH0687067B2 - Magnetic detection device - Google Patents

Magnetic detection device

Info

Publication number
JPH0687067B2
JPH0687067B2 JP63210237A JP21023788A JPH0687067B2 JP H0687067 B2 JPH0687067 B2 JP H0687067B2 JP 63210237 A JP63210237 A JP 63210237A JP 21023788 A JP21023788 A JP 21023788A JP H0687067 B2 JPH0687067 B2 JP H0687067B2
Authority
JP
Japan
Prior art keywords
gap
sensor
magnetic field
core
center
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
JP63210237A
Other languages
Japanese (ja)
Other versions
JPH0259682A (en
Inventor
英伸 浜田
和郎 戸田
訓 石塚
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP63210237A priority Critical patent/JPH0687067B2/en
Publication of JPH0259682A publication Critical patent/JPH0259682A/en
Publication of JPH0687067B2 publication Critical patent/JPH0687067B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Measuring Magnetic Variables (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 この発明は、配電線電流モニタリングセンサーなどの磁
気検出装置に関し、円磁界の強度を感知するセンサー
を、磁界強度誤差が最小となる磁界強度分布が極小ある
いは極大となる点に精度よくかつ効率的に設置できる磁
気検出装置を提供するものである。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic detection device such as a distribution line current monitoring sensor, and a sensor for detecting the strength of a circular magnetic field has a minimum magnetic field strength distribution that minimizes a magnetic field strength error. Alternatively, the present invention provides a magnetic detection device that can be installed accurately and efficiently at the maximum point.

従来の技術 従来の磁気検出装置は、第3図に示すようにC型コア5
のギャップ50に磁気(図示せず)を設置しコア5内の磁
束すなわち磁界を検出するものである。センサーの設置
位置を位置決めする時は、わざわざ磁界強度分布を測定
して強度変化の最少となる点を観測してセンサーを設置
する方法がある。しかるに、この方法ではセンサーの設
置が極めてめんどうで実用的でない。l2はコアの中心
線、l3は端面の中心線である。そこでセンサーの設定位
置をコア5の動径方向において磁界強度分布が極大とな
らないギャップ50の中心40と決め、ここにセンサーを設
置するようにする方法がある。これはあらかじめセンサ
ーを取付けたセンサーケース2をギャップ50にあわせて
作成し、このケース2を、平面な端面20,21間のギャッ
プ50に設置する。後者の方法は、通常ギャップの中心40
が磁界強度分布の極大な点とならいないため、検出誤差
が生じる。前述した中心40が極大点と一致しないのはコ
アの端面20,21が平行であるためであると考えられる。
2. Description of the Related Art A conventional magnetic detection device has a C-shaped core 5 as shown in FIG.
A magnetic field (not shown) is installed in the gap 50 to detect the magnetic flux in the core 5, that is, the magnetic field. When locating the position of the sensor, there is a method of measuring the magnetic field intensity distribution and observing the point where the intensity change is the minimum, and then installing the sensor. However, this method is extremely cumbersome and impractical to install the sensor. l 2 is the center line of the core and l 3 is the center line of the end face. Therefore, there is a method in which the setting position of the sensor is set to the center 40 of the gap 50 where the magnetic field strength distribution does not maximize in the radial direction of the core 5, and the sensor is installed here. This is prepared by fitting the sensor case 2 with the sensor attached in advance to the gap 50, and installing the case 2 in the gap 50 between the flat end faces 20 and 21. The latter method is usually the center of the gap 40
Does not become the maximum point of the magnetic field strength distribution, resulting in a detection error. It is considered that the above-mentioned center 40 does not coincide with the maximum point because the end faces 20 and 21 of the core are parallel to each other.

発明が解決しようとする課題 従来の方法では、上記コアのギャップ中心線l1上の動径
方向における磁界強度分布の最大値が第4図に示すよう
にギャップ中心4にこないため、センサー設置前に磁界
強度の変化による誤差が最小となる位置を測定により知
る必要がある。また、その位置が知れたとしても、それ
は、ギャップ中心とは異なり中途半端な位置となり、セ
ンサー設置作業上非常に非効率である。
According to the conventional method, since the maximum value of the magnetic field strength distribution in the radial direction on the gap center line l 1 of the core does not come to the gap center 4 as shown in FIG. It is necessary to know the position where the error due to the change of the magnetic field strength is minimum. Also, even if the position is known, it is a halfway position unlike the center of the gap, which is very inefficient in the sensor installation work.

逆に、前述のごとくセンサー設置作業を効率的に進める
ために、センサー設置位置をギャップ中心と決めてケー
ス2を設置すると、ギャップ中心40は第4図に示すよう
に磁界強度変化が大きい所なので、センサー位置決め精
度を上げたとしても磁界強度変化による誤差は無視でき
ない。
On the contrary, in order to efficiently proceed the sensor installation work as described above, if the sensor installation position is set to the center of the gap and the case 2 is installed, the gap center 40 has a large magnetic field strength change as shown in FIG. Even if the sensor positioning accuracy is increased, the error due to the change in magnetic field strength cannot be ignored.

この発明は、従来のものがもつ上記のような課題を解決
させ、コアギャップ中心に最大磁界強度を与え、精度よ
くかつ効率的にセンサーをギャップ中心に設置できるよ
うにした磁気検出装置を提供することを目的とする。
The present invention solves the above-mentioned problems of the conventional one, and provides a maximum magnetic field strength at the center of the core gap to provide a magnetic detection device capable of accurately and efficiently installing the sensor at the center of the gap. The purpose is to

課題を解決するための手段 本発明は上記目的を達成するため、コアのギャップ中心
線上の動径方向において、最大磁界強度が、前記ギャッ
プの前記コアの外径と内径の中点に位置し、前記中点近
傍に磁気センサーを設置するもので、ギャップの形状に
一致したセンサーケースを使用することにより容易に装
置を形成することができる。
Means for Solving the Problems To achieve the above object, in the radial direction on the gap centerline of the core, the maximum magnetic field strength is located at the midpoint between the outer diameter and the inner diameter of the core of the gap, The magnetic sensor is installed in the vicinity of the midpoint, and the device can be easily formed by using a sensor case that matches the shape of the gap.

本発明の望ましい例は、C型コアは非平行な2つのギャ
ップ面からなっている。その2つのギャップ面は、ギャ
ップ中心線に対して対称である。また、ギャップ面のな
す角度については、ギャップ中心線上の動径方向におい
てギャップ中心に磁界強度最大の点がくるように、2つ
のギャップ面は少し広がり気味になっている。
In a preferred example of the present invention, the C-shaped core consists of two non-parallel gap faces. The two gap planes are symmetrical with respect to the gap centerline. Regarding the angle formed by the gap surfaces, the two gap surfaces are slightly widened so that the maximum magnetic field strength is located at the center of the gap in the radial direction on the gap center line.

一方、センサーケースは、コアギャップと同形状を有
し、ケースの先頭がコア内径上にくるようになってお
り、動径方向において固有位置を有する。センサーは、
センサーケース内において、その固有位置での位置がコ
アギャップ中心となる位置に固定されている。
On the other hand, the sensor case has the same shape as the core gap, the head of the case is located on the core inner diameter, and has a unique position in the radial direction. The sensor is
In the sensor case, the position at the specific position is fixed to the position that is the center of the core gap.

作用 上記の様なC型コアを使用すると、ギャップ中心線上の
動径方向においてギャップの中心に常に磁界強度最大の
点が存在するので、センサー設置前にギャップ中の磁界
強度分布を測定する必要がなくなる。また、常にギャッ
プの中心に磁界強度変化率が最小の点が存在するので、
センサーを位置決めの容易なギャップ中心にすることで
磁界強度の変化率による誤差を最小にすることができ
る。
Action When using the C-shaped core as described above, there is always a point of maximum magnetic field strength at the center of the gap in the radial direction on the gap centerline, so it is necessary to measure the magnetic field strength distribution in the gap before installing the sensor. Disappear. Also, since there is always a point with the smallest rate of change in magnetic field strength in the center of the gap,
The error due to the rate of change of the magnetic field strength can be minimized by placing the sensor at the center of the gap where positioning is easy.

更に、センサーケースがコアギャップと同形状を有し、
ギャップ中において固有位置をもつため、高精度,高再
現性を保ちつつ容易かつ効率的にセンサーの設置作業を
行うことができる。
Furthermore, the sensor case has the same shape as the core gap,
Since it has a unique position in the gap, it is possible to easily and efficiently install the sensor while maintaining high accuracy and high reproducibility.

実施例 この発明の実施例を第1図,第2図,第3図を参照しな
がら説明する。本実施例は、第1図に示すように、コア
1の端面10,20は、ギャップ中心線l1に対して対称で非
平行でやや外側に広がり気味になっており、この端面1
0,20間でギャップ15が形成されている。ギャップ15の面
10,20のなす角度については、ギャップ15の巾に依存
し、計算あるいは簡単な実験により決定することができ
る。すなわち、面10,20の角度を適当に選択することに
より、ギャップの中心と磁界強度変化率の最小の点を一
致させることができる。第2図は、第1図に示すコアの
ギャップ中心線l1上の動径方向における磁界強度分布を
示す。第2図では、ギャップ中心4において、磁界強度
は最大で、磁界強度変化率は最小となることを示してい
る。これは前述のごとく端面10,20を適当な角度で非平
行とすることにより実現できる。したがって、ギャップ
15に合わせて、センサーケース2を作成し、上述の中心
4又はその近傍にくるようにセンサー3をケース2に設
置しておけばよい。たとえばセンサーケース2は、コア
ギャップ15と同形状の台形で、その中心側は内径に一致
させておけばよく、磁気センサー3はギャップ15中にお
いて固有位置(中心4)を占める。前述のごとくセンサ
ー3は、センサーケース2内において、その固有位置で
の位置がコアギャップ中心4となる位置にあらかじめ固
定されている。ケース2の辺21,22を端面10,20に合致さ
せ、辺23をコア1の内径と一致させるようにしておけ
ば、組み立ても容易である。
Embodiment An embodiment of the present invention will be described with reference to FIG. 1, FIG. 2, and FIG. In the present embodiment, as shown in FIG. 1, the end faces 10 and 20 of the core 1 are symmetrical with respect to the gap center line l 1 and non-parallel to each other, and are slightly spread outward.
A gap 15 is formed between 0 and 20. Face of gap 15
The angle formed by 10, 20 depends on the width of the gap 15, and can be determined by calculation or simple experiment. That is, by appropriately selecting the angles of the surfaces 10 and 20, the center of the gap and the point of the minimum magnetic field strength change rate can be matched. FIG. 2 shows the magnetic field strength distribution in the radial direction on the gap center line l 1 of the core shown in FIG. FIG. 2 shows that the magnetic field strength is maximum and the magnetic field strength change rate is minimum at the gap center 4. This can be realized by making the end faces 10 and 20 non-parallel at an appropriate angle as described above. Therefore, the gap
The sensor case 2 may be prepared in accordance with 15, and the sensor 3 may be installed in the case 2 so as to come to the center 4 or the vicinity thereof. For example, the sensor case 2 has a trapezoidal shape having the same shape as the core gap 15, and the center side thereof may be matched with the inner diameter, and the magnetic sensor 3 occupies a proper position (center 4) in the gap 15. As described above, the sensor 3 is fixed in advance within the sensor case 2 at a position where its unique position is the core gap center 4. If the sides 21 and 22 of the case 2 are aligned with the end faces 10 and 20 and the side 23 is aligned with the inner diameter of the core 1, the assembly is easy.

発明の効果 以上の説明から明らかなように、本発明は、コアのギャ
ップ中心線上の動径方向において最大磁界強度がギャッ
プ中心にくるようにギャップ面を設けることが可能とな
り、センサーを内部に固定したセンサーケースにギャッ
プ中で固有位置を与えることにより、磁界強度変化率に
よる誤差が最小となる位置に、高精度・高再現性を保ち
つつ容易かつ効率的にセンサー設置作業を行うことがで
きる。
EFFECTS OF THE INVENTION As is apparent from the above description, according to the present invention, it is possible to provide the gap surface so that the maximum magnetic field strength is located at the center of the gap in the radial direction on the gap centerline of the core, and the sensor is fixed inside. By giving a unique position to the sensor case in the gap, it is possible to easily and efficiently install the sensor at a position where the error due to the magnetic field strength change rate is minimized while maintaining high accuracy and high reproducibility.

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

第1図(a),(b)は本発明の実施例におけるC型コ
ア部の側面図,正面図,第2図は同実施例におけるギャ
ップ中心線上の動径方向の磁界強度分布図、第3図
(a),(b)は従来のギャップ面平行C型コアの側面
図,正面図、第4図は従来のC型コアのギャップ中心線
上の動径方向の磁界強度分布図である。 1……C型コア、2……センサーケース、3……センサ
ー、4……ギャップ中心、10,11……端面。
1 (a) and 1 (b) are a side view and a front view of a C-shaped core portion in an embodiment of the present invention, and FIG. 2 is a radial magnetic field strength distribution diagram on a gap center line in the embodiment, 3 (a) and 3 (b) are a side view and a front view of a conventional gap surface parallel C-shaped core, and FIG. 4 is a radial magnetic field strength distribution diagram on the gap center line of the conventional C-shaped core. 1 ... C-shaped core, 2 ... sensor case, 3 ... sensor, 4 ... gap center, 10, 11 ... end face.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】コアのギャップ中心線上の動径方向におい
て、最大磁界強度が前記ギャップの前記コアの外径と内
径の中点に位置し、前記中点近傍に磁気センサーを設置
してなることを特徴とする磁気検出装置。
1. A maximum magnetic field strength is located at a midpoint between the outer diameter and the inner diameter of the core in the radial direction on the center line of the gap of the core, and a magnetic sensor is installed in the vicinity of the midpoint. Magnetic detection device characterized by.
【請求項2】ギャップの形状に一致したセンサーケース
を使用することを特徴とした特許請求の範囲第1項に記
載の磁気検出装置。
2. The magnetic detection device according to claim 1, wherein a sensor case having a shape of a gap is used.
JP63210237A 1988-08-24 1988-08-24 Magnetic detection device Expired - Fee Related JPH0687067B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63210237A JPH0687067B2 (en) 1988-08-24 1988-08-24 Magnetic detection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63210237A JPH0687067B2 (en) 1988-08-24 1988-08-24 Magnetic detection device

Publications (2)

Publication Number Publication Date
JPH0259682A JPH0259682A (en) 1990-02-28
JPH0687067B2 true JPH0687067B2 (en) 1994-11-02

Family

ID=16586054

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63210237A Expired - Fee Related JPH0687067B2 (en) 1988-08-24 1988-08-24 Magnetic detection device

Country Status (1)

Country Link
JP (1) JPH0687067B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0740780A (en) * 1993-07-30 1995-02-10 Natl House Ind Co Ltd Load carrying platform installation structure for parallel body

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6175229B1 (en) * 1999-03-09 2001-01-16 Eaton Corporation Electrical current sensing apparatus
JP2008039517A (en) * 2006-08-03 2008-02-21 Denso Corp Current sensor
JP5107779B2 (en) * 2008-04-21 2012-12-26 矢崎総業株式会社 Current sensor
JP2011064648A (en) * 2009-09-18 2011-03-31 Tokai Rika Co Ltd Current sensor
JP2014106101A (en) * 2012-11-27 2014-06-09 Toyota Industries Corp Current sensor
JP2014106100A (en) * 2012-11-27 2014-06-09 Toyota Industries Corp Current sensor
JP6732563B2 (en) * 2016-06-28 2020-07-29 日置電機株式会社 Sensors and current measuring devices

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6319272U (en) * 1986-07-21 1988-02-08

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0740780A (en) * 1993-07-30 1995-02-10 Natl House Ind Co Ltd Load carrying platform installation structure for parallel body

Also Published As

Publication number Publication date
JPH0259682A (en) 1990-02-28

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