JPH083500B2 - Current detector - Google Patents

Current detector

Info

Publication number
JPH083500B2
JPH083500B2 JP62149404A JP14940487A JPH083500B2 JP H083500 B2 JPH083500 B2 JP H083500B2 JP 62149404 A JP62149404 A JP 62149404A JP 14940487 A JP14940487 A JP 14940487A JP H083500 B2 JPH083500 B2 JP H083500B2
Authority
JP
Japan
Prior art keywords
current detector
substrate
current
hole
conductor layer
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 - Lifetime
Application number
JP62149404A
Other languages
Japanese (ja)
Other versions
JPS63313072A (en
Inventor
みち子 遠藤
秀昭 依田
茂美 倉島
昇 若月
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP62149404A priority Critical patent/JPH083500B2/en
Priority to KR1019880003695A priority patent/KR910004261B1/en
Priority to EP88105535A priority patent/EP0286079B1/en
Priority to DE8888105535T priority patent/DE3878281T2/en
Priority to US07/180,120 priority patent/US5049809A/en
Publication of JPS63313072A publication Critical patent/JPS63313072A/en
Publication of JPH083500B2 publication Critical patent/JPH083500B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔概要〕 本発明は交流・直流の何れにも適用できる小型電流検
出器を得るため、磁電変換素子に近接した貫通孔の孔壁
に被着させた導体層に電流を流し、該磁電変換素子の出
力により簡易に電流値を検出する電流検出器である。
DETAILED DESCRIPTION OF THE INVENTION [Outline] In order to obtain a small-sized current detector applicable to both AC and DC, the present invention provides a current to a conductor layer adhered to a hole wall of a through hole close to a magnetoelectric conversion element. Is a current detector that simply detects the current value by the output of the magnetoelectric conversion element.

〔産業上の利用分野〕[Industrial applications]

本発明は、電流が流れたとき発生する磁界の強さの変
化により、電流値を検出する検出器を関する。
The present invention relates to a detector that detects a current value by changing the strength of a magnetic field generated when a current flows.

従来の電流検出器は、直流用・交流用とそれぞれ専用
のものを必要とすることが多く、比較的大型であり、特
に、直流用のものは絶縁型で小型の電流検出器を開発す
ることが要望された。
Conventional current detectors often require dedicated ones for direct current and alternating current, and are relatively large. Especially for direct current, it is necessary to develop a small insulated current detector. Was requested.

〔従来の技術〕[Conventional technology]

従来、交流電流測定用検出器には変成器を使用するも
のと、漏電センサを使用するものが一般的であり、直流
電流側定用検出器は抵抗素子を使用するものと、ホール
効果素子を使用するものが一般に使用されている。
Conventionally, a detector that uses a transformer and a detector that uses a leakage sensor are generally used as detectors for measuring AC current, and a detector that uses a resistance element and a Hall effect element for detectors that measure DC current. What you use is commonly used.

変成器を使用した交流電流検出器は、小型化が困難で
あり、変成器にはイングクタンス成分があるため、パル
ス電流等の高周波成分の多い電流では正確に測定が困難
である。他方、漏電センサを使用した交流電流検出器
は、使用電流とそれに適した大きさの環状コアが必要と
なり、適用範囲が広くできないという欠点がある。
An AC current detector using a transformer is difficult to miniaturize, and since the transformer has an inductance component, it is difficult to accurately measure a current having many high frequency components such as a pulse current. On the other hand, an AC current detector using a leak sensor has a drawback that it cannot be applied in a wide range because it requires a current core and an annular core having a size suitable for the current.

抵抗素子を使用した直流電流検出器は、抵抗素子にお
いて無駄な電力消費があり、電流値と抵抗素子の抵抗値
および、直流電位差計をその都度選定して使用する必要
があって、そのとき電流回路に不要信号が混入すると測
定に直接影響し、小型化できないという欠点がある。
A DC current detector using a resistance element consumes unnecessary power in the resistance element, and it is necessary to select and use the current value and the resistance value of the resistance element and the DC potentiometer each time. If an unnecessary signal is mixed in the circuit, it has a drawback that it directly affects the measurement and cannot be downsized.

さらに、ホール効果素子を使用した直流電流検出器
は、外部磁界および地磁気の影響を除く手段が必要とな
ることにより、装置が複雑かつ大型化するという欠点が
ある。
Further, the DC current detector using the Hall effect element has a drawback that the device becomes complicated and large in size because a means for removing the influence of the external magnetic field and the earth magnetism is required.

本願出願人が昭和62年4月9日付けで出願した特願昭
62−87749号は、前記欠点を除去した電流検出器であ
り、第8図は該電流検出器の原理構成図である。
Japanese Patent Application filed by the applicant of the present application on April 9, 1987
No. 62-87749 is a current detector from which the above-mentioned drawbacks are removed, and FIG. 8 is a principle configuration diagram of the current detector.

第8図において、一対の磁電変換素子1,2は同一特性
であり、導線3に電流4が流れたとき発生する磁気ルー
プ5に対し互いに同一で異なる方向の磁界を受ける。そ
のため、変換素子1,2から取り出した出力は逆位相であ
るから、合成部6において差動合成したとき、合成部6
の出力は素子単独出力のほぼ2倍となる。
In FIG. 8, the pair of magnetoelectric conversion elements 1 and 2 have the same characteristics and receive magnetic fields in the same but different directions with respect to the magnetic loop 5 generated when a current 4 flows through the conductor 3. Therefore, since the outputs extracted from the conversion elements 1 and 2 have opposite phases, when the synthesis section 6 performs differential synthesis, the synthesis section 6
Is almost twice as high as the output of the element alone.

一方、電流検出器8の全体に外部磁界7が影響してい
るとき、外部磁界7に対し磁電変換素子1,2の出力は同
相であるため、合成部6において差動合成した出力に
は、外部磁界7による出力信号が打消される。
On the other hand, when the external magnetic field 7 influences the whole of the current detector 8, the outputs of the magnetoelectric conversion elements 1 and 2 are in phase with the external magnetic field 7, and thus the output differentially combined in the combining unit 6 is: The output signal from the external magnetic field 7 is canceled.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

電流検出器8において、導線3は一対の磁電変換素子
1,2の対向中心に位置し、かつ、基板に対して垂直に電
流が流れるようにする必要がある。そこで、変換素子1,
2の形成または搭載する基板に明けた導線3の貫通孔
は、基板の表面に対し垂直かつ遊びのないことが必要で
ある。しかし、かかる貫通孔を設け、これに前記のよう
に導線を配置するのは極めて困難、かつ、電流検出器8
に高性能化を妨げるという問題点があり、その改善が強
く要望されるようになった。
In the current detector 8, the conducting wire 3 is a pair of magnetoelectric conversion elements.
It is necessary to locate the currents at the opposing centers of 1 and 2 and to make the current flow perpendicular to the substrate. Therefore, the conversion element 1,
It is necessary that the through hole of the conducting wire 3 formed on the substrate on which the substrate 2 is formed or mounted is perpendicular to the surface of the substrate and has no play. However, it is extremely difficult to provide such a through hole and dispose the conducting wire in the through hole, and the current detector 8
However, there is a problem that it hinders high performance, and there has been a strong demand for improvement.

〔問題点を解決するための手段〕[Means for solving problems]

第1図は本発明による電流検出器の原理構成図であ
る。
FIG. 1 is a block diagram showing the principle of a current detector according to the present invention.

第1図において、前記問題点の除去を目的とした電流
検出器11は、基板12の所定部に設けた貫通孔13の孔壁面
に被着し被測定電流18が流れる導体層14と、 導体層14に被測定電流18が流れた際に、導体層14の周
囲に発生する磁界19を、導体層14の周囲対向領域におい
て磁電変換する磁電変換素子15,16とを具え、構成して
なることを特徴とする。
In FIG. 1, a current detector 11 for the purpose of eliminating the above-mentioned problems comprises a conductor layer 14 which is attached to a hole wall surface of a through hole 13 provided in a predetermined portion of a substrate 12 and through which a current 18 to be measured flows. A magnetic field 19 generated around the conductor layer 14 when a current 18 to be measured flows in the layer 14 is provided with magnetoelectric conversion elements 15 and 16 for performing magnetoelectric conversion in a region facing the periphery of the conductor layer 14. It is characterized by

〔作用〕[Action]

上記手段によれば、基板の貫通孔に被測定電流の流れ
る導体層を形成し、該導体層の周囲対向領域に少なくと
も一対の磁電変換素子を設けることにより、該導体層と
該磁電変換素子の相対的位置関係が高精度かつ固定され
る。そのため、被測定電流の測定値は高精度かつ安定化
し、高性能な電流検出器を実現した。
According to the above means, the conductor layer through which the current to be measured flows is formed in the through hole of the substrate, and at least a pair of magnetoelectric conversion elements are provided in the peripheral facing region of the conductor layer, whereby the conductor layer and the magnetoelectric conversion element are provided. The relative positional relationship is fixed with high accuracy. Therefore, the measured value of the measured current is highly accurate and stable, realizing a high-performance current detector.

〔実施例〕〔Example〕

本発明に使用する磁電変換素子として、ホール効果素
子あるいは磁気抵抗素子を使用できるが、特にバーバー
ポール型磁気抵抗素子を基板上に設けた検出器は、製造
および性能上有効である。
A Hall effect element or a magnetoresistive element can be used as the magnetoelectric conversion element used in the present invention. In particular, a detector provided with a barber pole type magnetoresistive element on a substrate is effective in manufacturing and performance.

以下に、図面を用いて本発明による電流検出器を説明
する。
Hereinafter, the current detector according to the present invention will be described with reference to the drawings.

第2図は本発明の一実施例による電流検出器の主要構
成を示す模式図、第3図は電流検出素子の全体を示す斜
視図、第4図はバーバーポール型磁気抵抗素子パターン
を示す平面図、第5図は基板の平面図(イ)と下面図
(ロ)および貫通孔の側断面図(ハ)である。
FIG. 2 is a schematic view showing the main configuration of a current detector according to an embodiment of the present invention, FIG. 3 is a perspective view showing the whole current detection element, and FIG. 4 is a plane showing a barber pole type magnetoresistive element pattern. 5 and 5 are a plan view (a), a bottom view (b), and a side sectional view (c) of the through hole.

第2図において、ガラスまたはシリコン等にてなる基
板12−1の表面に形成した磁気抵抗素子15−1,15−2と
16−1,16−2は、それぞれ対をなす磁気抵抗素子の例で
ある。磁気抵抗素子としてはバーバーポール型が好適で
あり、各抵抗素子15−1,15−2,16−1,16−2および、そ
れらの抵抗値調整用の抵抗素子15−3,16−3は、図示の
如くブリッジに接続される。
In FIG. 2, the magnetoresistive elements 15-1 and 15-2 formed on the surface of the substrate 12-1 made of glass or silicon are shown.
16-1 and 16-2 are examples of paired magnetoresistive elements. A barber pole type is suitable as the magnetic resistance element, and each resistance element 15-1, 15-2, 16-1, 16-2 and the resistance elements 15-3, 16-3 for adjusting their resistance values are , Connected to the bridge as shown.

基板12−1に穿設した断面円形の貫通孔13−1は、各
抵抗素子15−1,15−2,15−3,16−1,16−2,16−3の中心
部に位置し、第5図に示すように、孔壁に被測定電流の
流れる導体層14を被着し、基板12−1の表面には外部接
続端子を含むランド部14−1を導体層14と一体に形成す
ると共に、基板12−1の裏面全体には導体層14と一体に
形成し外部接続媒体となる導体層14−2を被着してな
る。なお、第5図(イ)において、一点鎖線で示す一対
の同心円に挟まれた領域は、抵抗素子15−1,15−2,16−
1,16−2の形成領域である。
The through hole 13-1 having a circular cross section formed on the substrate 12-1 is located at the center of each of the resistance elements 15-1, 15-2, 15-3, 16-1, 16-2, 16-3. As shown in FIG. 5, a conductor layer 14 through which a current to be measured flows is deposited on the hole wall, and a land portion 14-1 including external connection terminals is formed integrally with the conductor layer 14 on the surface of the substrate 12-1. Along with the formation, a conductor layer 14-2, which is formed integrally with the conductor layer 14 and serves as an external connection medium, is deposited on the entire back surface of the substrate 12-1. In FIG. 5 (a), the regions sandwiched by the pair of concentric circles indicated by the alternate long and short dash line are resistance elements 15-1, 15-2, 16-
It is a formation region of 1, 16-2.

抵抗素子15−1〜16−3を接続したブリッジの一方の
対角頂点は定電流源22に接続し、該ブリッジの他方の対
角頂点にはブリッジの出力を差動合成する演算増幅器
(合成部)23が接続される。
One diagonal apex of the bridge connecting the resistance elements 15-1 to 16-3 is connected to the constant current source 22, and the other diagonal apex of the bridge is an operational amplifier for differentially combining the outputs of the bridge. Part) 23 is connected.

このように構成した電流検出器21において、ランド部
14−1および導体層14−2にそれぞれ導線24,25を接続
し、導線24,25を介し導体層14に直流電流を流すと、導
体層14に発生した磁界は磁気抵抗素子15−1と15−2,16
−1と16−2に対しそれぞれ逆方向に影響し、それらの
抵抗値を変化させる。
In the current detector 21 configured as above, the land portion
When the conductors 24 and 25 are connected to the conductor layer 14-1 and the conductor layer 14-2, respectively, and a direct current is applied to the conductor layer 14 through the conductors 24 and 25, the magnetic field generated in the conductor layer 14 becomes the magnetoresistive element 15-1. 15-2,16
-1 and 16-2 are affected in the opposite directions to change their resistance values.

そのため、定電流源22から前記ブリッジの一方の対角
頂点間に印加した定電流が変化し、他方の対角頂点間か
ら取り出した出力は、演算増幅器23で差動増幅されるよ
うになり、導体層14に発生した磁界の強さの変化と演算
増幅器23の出力電圧について予め校正しておけば、演算
増幅器23の出力電圧から導体層14に流れる電流値を検知
できる。
Therefore, the constant current applied from the constant current source 22 to one of the diagonal vertices of the bridge is changed, the output taken from between the other diagonal vertices will be differentially amplified by the operational amplifier 23, If the change in the strength of the magnetic field generated in the conductor layer 14 and the output voltage of the operational amplifier 23 are calibrated in advance, the current value flowing in the conductor layer 14 can be detected from the output voltage of the operational amplifier 23.

導体層14に交流が流れるときは、交流ピーク値に対応
する磁界の強さ変化をブリッジの一方の対角頂点間から
取り出すことができる。
When an alternating current flows through the conductor layer 14, a change in the magnetic field strength corresponding to the alternating current peak value can be taken out from between one of the diagonal apexes of the bridge.

第3図は基板12−1をパッケージ27に収容した電流検
出素子26であり、貫通孔13−1,抵抗素子15−1,15−2,16
−1,16−2等を形成した基板12−1は、リード端子28−
1を一体に形成した金属板29に搭載し、ランド部14−1
とリード端子28−2,基板12−1に形成したパッド31−1
〜4と各パッド31−1〜4に対向するリード端子28−3
〜6とは、それぞれがボンディングワイヤ30により接続
される。
FIG. 3 shows a current detection element 26 in which the substrate 12-1 is housed in a package 27, which includes a through hole 13-1, resistance elements 15-1, 15-2, 16
-1, 16-2 and the like formed on the substrate 12-1 is a lead terminal 28-
1 is mounted on an integrally formed metal plate 29, and the land portion 14-1
And lead terminal 28-2, pad 31-1 formed on substrate 12-1
To 4 and lead terminals 28-3 facing the pads 31-1 to 31-4
6 to 6 are connected to each other by a bonding wire 30.

第4図において、公知技術によってつづら折り状に形
成したバーバーポール型磁気抵抗素子15−1,15−2,16−
1,16−2は、それらを環状に接続してなる。ただし、磁
気抵抗素子15−1の一端と磁気抵抗素子16−1の一端と
をボンディングパッド31−1に接続し、磁気抵抗素子15
−1の他端の磁気抵抗素子16−2の一端とをボンディン
グパッド31−4に接続し、磁気抵抗素子16−2の他端と
磁気抵抗素子15−2の一端とをボンディングパッド31−
3に接続し、磁気抵抗素子16−1の他端は抵抗値調整用
抵抗素子16−3を介してボンディングパッド31−2に接
続すると共に、磁気抵抗素子15−2の他端は抵抗値調整
用抵抗素子15−3を介してボンディングパッド31−2に
接続されてなる。
In FIG. 4, barber pole type magnetoresistive elements 15-1, 15-2, 16- formed in a zigzag shape by a known technique.
1, 16-2 are formed by connecting them in a ring shape. However, one end of the magnetoresistive element 15-1 and one end of the magnetoresistive element 16-1 are connected to the bonding pad 31-1 so that the magnetoresistive element 15-1
−1 of the other end of the magnetic resistance element 16-2 is connected to the bonding pad 31-4, and the other end of the magnetic resistance element 16-2 and one end of the magnetic resistance element 15-2 are connected to the bonding pad 31−.
3, the other end of the magnetic resistance element 16-1 is connected to the bonding pad 31-2 via the resistance value adjusting resistance element 16-3, and the other end of the magnetic resistance element 15-2 is adjusted in resistance value. It is connected to the bonding pad 31-2 through the resistance element 15-3 for use.

なお、抵抗素子15−1,15−2,16−1,16−2のつづら折
り状パターンは、リソグラフィ技術によってつづら折り
状の磁性薄膜に縞状の導電帯を積層してなる。
The zigzag pattern of the resistance elements 15-1, 15-2, 16-1, 16-2 is formed by laminating striped conductive bands on the zigzag magnetic thin film by a lithography technique.

第6図は他の実施例による電流検出器の基板を示す平
面図(イ)とその下面図(ロ)とその下面図(ロ)およ
び貫通孔の側断面図(ハ)、第7図はさらに他の実施例
による電流検出器の基板を示す平面図(イ)とその下面
図(ロ)およびA−A断面図(ハ),B−B断面図(ニ)
である。
FIG. 6 is a plan view (a) showing a substrate of a current detector according to another embodiment, a bottom view thereof (b), a bottom view thereof (b), a side sectional view of a through hole (c), and FIG. A plan view (a) showing a substrate of a current detector according to still another embodiment, its bottom view (b), AA sectional view (c), and BB sectional view (d).
Is.

公知のようにシリコン単結晶は、加熱アルカリ性のエ
ッチング液を用いてエッチングすると、その結晶方位に
よってエッチング速度が異なる異方性エッチングとな
る。即ち、両方位が(100),(110)方向はエッチング
速度が速い反面、(111)面はエッチング速度が極めて
遅い。そのため、異方性エッチング液でエッチングする
と、(111)面が残るようになる。
As is well known, when a silicon single crystal is etched using a heated alkaline etching solution, it becomes anisotropic etching in which the etching rate varies depending on the crystal orientation. That is, while the etching rate is fast in the (100) and (110) directions on both sides, the etching rate is extremely slow in the (111) plane. Therefore, the (111) plane will remain when etching with an anisotropic etching solution.

従って、適当な面方位を持つシリコンウエーハを用
い、酸化膜のマスクパターンの透孔を適当な結晶軸方向
に揃え、異方性エッチングすることにより、シリコン基
板には中心に対し正確な点対称断面の貫通孔が形成され
るようになる。
Therefore, by using a silicon wafer with an appropriate plane orientation, aligning the through holes of the mask pattern of the oxide film with the appropriate crystal axis direction, and performing anisotropic etching, the silicon substrate has an accurate point symmetric cross section with respect to the center. Through holes are formed.

第6図において、前述の基板12−1に相当する基板12
−2は面方位が(100)のシリコン単結晶板であり、角
錐台形の貫通孔13−2は、シリコン基板12−2の表面<
110>方向にマスクの角度透孔辺を合わせ、異方性エッ
チングにより形成したものであり、貫通孔13−2の孔壁
には被測定電流の流れる導体層32を被着し、基板12−2
の上面には外部接続端子を含むランド部32−1を導体層
32と一体に形成すると共に、基板12−2の下面全体には
導体層32と一体に形成し外部接続媒体となる導体層32−
2を被着してなる。
In FIG. 6, a substrate 12 corresponding to the above-mentioned substrate 12-1.
-2 is a silicon single crystal plate having a plane orientation of (100), and the truncated pyramid-shaped through hole 13-2 is a surface of the silicon substrate 12-2 <
The mask is formed by anisotropic etching with the angle side of the mask aligned with the 110> direction, and the conductor layer 32 through which the current to be measured flows is attached to the hole wall of the through hole 13-2. Two
A land portion 32-1 including external connection terminals is provided on the upper surface of the conductor layer.
32 is formed integrally with the conductor layer 32 and is formed integrally with the conductor layer 32 on the entire lower surface of the substrate 12-2 to serve as an external connection medium.
2 is attached.

かかる基板12−2の主要製造工程例を工程順に記載す
ると下記のとおりである。
An example of the main manufacturing process of the substrate 12-2 will be described below in order of process.

シリコン基板12−2の表面に熱酸化による酸化膜を
厚さ0.5〜1.0μmに形成する。
An oxide film by thermal oxidation is formed on the surface of the silicon substrate 12-2 to a thickness of 0.5 to 1.0 μm.

ホトリソグラフィ技術により酸化膜の所要部に正方
形の透孔を明け、レジストマスクパターンが完成する。
ただし、該透孔の一辺はシリコン基板12−2の表面<11
0>方向となるようにする。
A square through hole is formed in a required portion of the oxide film by photolithography, and a resist mask pattern is completed.
However, one side of the through hole is the surface of the silicon substrate 12-2 <11.
0> direction.

異方性エッチングにより貫通孔13−2を明けると、
貫通孔13−2は孔壁の傾斜角度や約55度の角錐台形にな
る。ただし、エッチング液としてエチレンジアミン255c
c,H2O120cc,カテコール45gの混合液を100〜110℃で使用
したとき、エッチング深さは60〜80μm/時間であり、シ
リコン基板12−2の厚さを280μmとしたとき、貫通孔1
3−2の形成に4時間程度を要する。
When the through hole 13-2 is opened by anisotropic etching,
The through hole 13-2 has a truncated pyramid shape with an inclination angle of the hole wall and about 55 degrees. However, as an etchant, ethylenediamine 255c
When a mixed solution of 120 g of c, H 2 O and 45 g of catechol is used at 100 to 110 ° C., the etching depth is 60 to 80 μm / hour, and when the thickness of the silicon substrate 12-2 is 280 μm, the through hole 1
It takes about 4 hours to form 3-2.

熱酸化によりシリコン基板12−2の全表面に酸化膜
を形成させる。
An oxide film is formed on the entire surface of the silicon substrate 12-2 by thermal oxidation.

シリコン基板12−2の表面に磁気抵抗素子を形成さ
せる。
A magnetoresistive element is formed on the surface of the silicon substrate 12-2.

該磁気抵抗素子の保護膜を形成させる。 A protective film for the magnetoresistive element is formed.

導体層32,32−1,32−2を被着させる。 The conductor layers 32, 32-1, 32-2 are deposited.

第7図において、前述の基板12−1に相当する基板12
−3は両方位が(110)のシリコン単結晶板であり、上
面で菱形となり下面で六角形である貫通孔13−3は、シ
リコン基板12−3の表面<111>方向に、鋭角が70.5度
に形成したマスクの菱形透孔の一辺を合わせ、異方性エ
ッチングにより形成したものであり、該菱形の鈍角部分
で表面に対し垂直にエッチングされる反面、該菱形の鋭
角コーナからは斜面にエッチングされる。貫通孔13−3
の孔壁には被測定電流の流れる導体層33を被着し、基板
12−3の上面には外部接続端子を含むランド部33−1を
導体層33と一体に形成すると共に、基板12−3の下面全
体には導体層33と一体に形成し外部接続媒体となる導体
層33−2を被着してなる。
In FIG. 7, a substrate 12 corresponding to the above-mentioned substrate 12-1.
-3 is a silicon single crystal plate of which both positions are (110), and the upper surface is rhomboid and the lower surface is hexagonal. Through-hole 13-3 has a sharp angle of 70.5 in the surface <111> direction of silicon substrate 12-3. One side of the rhombic through hole of the mask is formed by anisotropic etching, and the obtuse angle portion of the rhombus is etched perpendicularly to the surface, but from the sharp corner of the rhombus to the slope. Is etched. Through hole 13-3
A conductor layer 33 through which a measured current flows is deposited on the hole wall of the
A land portion 33-1 including external connection terminals is formed integrally with the conductor layer 33 on the upper surface of 12-3, and is formed integrally with the conductor layer 33 on the entire lower surface of the substrate 12-3 to serve as an external connection medium. The conductor layer 33-2 is deposited.

かかる基板12−3は、基板12−2と同様の工程により
製造される。
The substrate 12-3 is manufactured by the same process as the substrate 12-2.

〔発明の効果〕〔The invention's effect〕

以上説明した本発明によれば、少なくとも一対の磁電
変換素子の対向中心に貫通孔を設け、該貫通孔の孔壁に
被測定電流の流れる導体層を形成し、磁電変換素子と導
体層との位置関係が正確かつ固定されることにより、磁
電変換素子の出力変化を取り出して該導体層に流れる測
定電流値の検出が、高精度かつ安定化した効果が顕著で
ある。
According to the present invention described above, at least a pair of magnetoelectric conversion elements is provided with a through hole at the facing center, and a conductor layer through which a current to be measured flows is formed on the hole wall of the through hole, and the magnetoelectric conversion element and the conductor layer are connected. Since the positional relationship is accurate and fixed, the output change of the magnetoelectric conversion element can be taken out and the measurement current value flowing through the conductor layer can be detected with high accuracy and stability.

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

第1図は本発明の電流検出器の原理構成図、 第2図は本発明の一実施例の電流検出器の主要構成を示
す模式図、 第3図は電流検出素子の全体を示す斜視図、 第4図はバーバーポール型磁気抵抗素子パターンを示す
平面図、 第5図は第2図に示す基板の構成図、 第6図は他の実施例による電流検出器の基板の構成図、 第7図はさらに他の実施例により電流検出器の基板の構
成図、 第8図は従来の電流検出器の原理構成図、 である。 図中において、 11,21は電流検出器、12,12−1,12−2,12−3は基板、1
3,13−1,13−2,13−3は貫通孔、14,32,33は導体層、1
5,16は磁電変換素子、15−1,15−2,16−1,16−2はバー
バーポール磁気抵抗素子、17は合成部、18は被測定電
流、19は磁気ループ、 を示す。
FIG. 1 is a principle configuration diagram of a current detector of the present invention, FIG. 2 is a schematic diagram showing a main configuration of a current detector of one embodiment of the present invention, and FIG. 3 is a perspective view showing an entire current detection element. 4, FIG. 4 is a plan view showing a barber pole type magnetoresistive element pattern, FIG. 5 is a block diagram of a substrate shown in FIG. 2, FIG. 6 is a block diagram of a substrate of a current detector according to another embodiment, 7 is a block diagram of a substrate of a current detector according to still another embodiment, and FIG. 8 is a principle block diagram of a conventional current detector. In the figure, 11,21 are current detectors, 12,12-1,12-2,12-3 are substrates, 1
3,13-1,13-2,13-3 are through holes, 14,32,33 are conductor layers, 1
5, 16 are magnetoelectric conversion elements, 15-1, 15-2, 16-1, 16-2 are barber pole magnetoresistive elements, 17 is a combining part, 18 is a measured current, and 19 is a magnetic loop.

フロントページの続き (72)発明者 若月 昇 神奈川県川崎市中原区上小田中1015番地 富士通株式会社内 (56)参考文献 特開 昭63−253264(JP,A) 特開 昭57−128854(JP,A)Front page continuation (72) Inventor Noboru Wakatsuki 1015 Kamiodanaka, Nakahara-ku, Kawasaki City, Kanagawa Prefecture, Fujitsu Limited (56) References JP-A-63-253264 (JP, A) JP-A-57-128854 (JP) , A)

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】基板(12)の所定部に設けた貫通孔(13)
の孔壁面に被着し被測定電流(18)が流れる導体層(1
4)と、 該導体層(14)に該被測定電流(18)が流れた際に、該
導体層(14)の周囲に発生する磁界(19)を、該導体層
(14)の周囲対向領域において磁電変換する磁電変換素
子(15,16)とを具え、構成してなることを特徴とする
電流検出器。
1. A through hole (13) provided in a predetermined portion of a substrate (12).
Of the conductor layer (1
4) and a magnetic field (19) generated around the conductor layer (14) when the current to be measured (18) flows through the conductor layer (14) faces the periphery of the conductor layer (14). A current detector comprising a magnetoelectric conversion element (15, 16) for performing a magnetoelectric conversion in a region.
【請求項2】前記磁電変換素子として磁気抵抗素子を使
用してなることを特徴とする前記特許請求の範囲第1項
記載の電流検出器。
2. The current detector according to claim 1, wherein a magnetoresistive element is used as the magnetoelectric conversion element.
【請求項3】前記磁電変換素子(15,16)が前記基板(1
2)に形成してなることを特徴とする前記特許請求の範
囲第1項記載の電流検出器。
3. The magnetoelectric conversion element (15, 16) is provided on the substrate (1).
The current detector according to claim 1, wherein the current detector is formed in 2).
【請求項4】前記磁気抵抗素子(15,16)がバーバーポ
ール型磁気抵抗素子であることを特徴とする前記特許請
求の範囲第2項および第4項記載の電流検出器。
4. The current detector according to claim 2, wherein the magnetoresistive elements (15, 16) are barber pole type magnetoresistive elements.
【請求項5】前記貫通孔(13)がエッチングにより前記
基板(12)に穿設してなることを特徴とする前記特許請
求の範囲第1項記載の電流検出器。
5. The current detector according to claim 1, wherein the through hole (13) is formed in the substrate (12) by etching.
【請求項6】前記基板(12)がシリコン基板であり、前
記貫通孔(13)がシリコンの異方性エッチングを利用し
穿設してなることを特徴とする前記特許請求の範囲第5
項記載の電流検出器。
6. The method according to claim 5, wherein the substrate (12) is a silicon substrate, and the through hole (13) is formed by utilizing anisotropic etching of silicon.
The current detector according to the item.
【請求項7】前記シリコン基板の面方位が(110)であ
り、前記貫通孔(13)が一方の開口を菱形,他方の開口
を六角形とし孔壁の一部が該シリコン基板の表面に対し
垂直に形成してなることを特徴とする前記特許請求の範
囲第6項記載の電流検出器。
7. The surface orientation of the silicon substrate is (110), and the through hole (13) has one opening of a rhombic shape and the other opening of a hexagonal shape, and part of the hole wall is on the surface of the silicon substrate. The current detector according to claim 6, wherein the current detector is formed vertically.
【請求項8】前記シリコン基板の面方位が(100)であ
り、前記貫通孔(13)が断面正方形に形成してなること
を特徴とする前記特許請求の範囲第6項記載の電流検出
器。
8. The current detector according to claim 6, wherein the silicon substrate has a plane orientation of (100) and the through hole (13) is formed in a square cross section. .
JP62149404A 1987-04-09 1987-06-16 Current detector Expired - Lifetime JPH083500B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP62149404A JPH083500B2 (en) 1987-06-16 1987-06-16 Current detector
KR1019880003695A KR910004261B1 (en) 1987-04-09 1988-04-01 Detector using rotating conversion element
EP88105535A EP0286079B1 (en) 1987-04-09 1988-04-07 Sensing devices utilizing magneto electric transducers
DE8888105535T DE3878281T2 (en) 1987-04-09 1988-04-07 SENSOR WITH A MAGNETO-ELECTRICAL TRANSDUCER.
US07/180,120 US5049809A (en) 1987-04-09 1988-04-11 Sensing device utilizing magneto electric transducers

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62149404A JPH083500B2 (en) 1987-06-16 1987-06-16 Current detector

Publications (2)

Publication Number Publication Date
JPS63313072A JPS63313072A (en) 1988-12-21
JPH083500B2 true JPH083500B2 (en) 1996-01-17

Family

ID=15474390

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62149404A Expired - Lifetime JPH083500B2 (en) 1987-04-09 1987-06-16 Current detector

Country Status (1)

Country Link
JP (1) JPH083500B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2013051567A1 (en) * 2011-10-03 2015-03-30 アルプス・グリーンデバイス株式会社 Current sensor
JPWO2013051566A1 (en) * 2011-10-03 2015-03-30 アルプス・グリーンデバイス株式会社 Current sensor

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2712206B2 (en) * 1987-11-30 1998-02-10 株式会社デンソー Current detector
JP5793681B2 (en) * 2011-01-21 2015-10-14 パナソニックIpマネジメント株式会社 Power measuring device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2013051567A1 (en) * 2011-10-03 2015-03-30 アルプス・グリーンデバイス株式会社 Current sensor
JPWO2013051566A1 (en) * 2011-10-03 2015-03-30 アルプス・グリーンデバイス株式会社 Current sensor

Also Published As

Publication number Publication date
JPS63313072A (en) 1988-12-21

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