JP2534824B2 - Proximity switch - Google Patents

Proximity switch

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Publication number
JP2534824B2
JP2534824B2 JP5269517A JP26951793A JP2534824B2 JP 2534824 B2 JP2534824 B2 JP 2534824B2 JP 5269517 A JP5269517 A JP 5269517A JP 26951793 A JP26951793 A JP 26951793A JP 2534824 B2 JP2534824 B2 JP 2534824B2
Authority
JP
Japan
Prior art keywords
detection coil
conductor layer
shield conductor
shield
loss
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
JP5269517A
Other languages
Japanese (ja)
Other versions
JPH07105808A (en
Inventor
純治 大野
正寿 河合
隆司 干場
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 Industrial Devices SUNX Co Ltd
Original Assignee
Sunx 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 Sunx Ltd filed Critical Sunx Ltd
Priority to JP5269517A priority Critical patent/JP2534824B2/en
Publication of JPH07105808A publication Critical patent/JPH07105808A/en
Application granted granted Critical
Publication of JP2534824B2 publication Critical patent/JP2534824B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Electronic Switches (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は検出コイルに高周波電流
を流して物体の接近を検出する近接スイッチに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a proximity switch for detecting the approach of an object by passing a high frequency current through a detection coil.

【0002】[0002]

【従来の技術】この種のスイッチは、検出回路を実装し
たプリント基板に、フェライトコアに巻装した検出コイ
ルを接着剤等によって張り付けて構成されており、検出
コイルに金属製の被検出物体が接近すると、コイル損失
が増大して発振振幅が低下することに基づいてスイッチ
ング動作が行われる。ところが、検出コイルは面積的に
大きな割合を占めるため、ここに誘導されるノイズ成分
も大きく、これが誤動作や検出精度の低下の原因となる
という問題があった。
2. Description of the Related Art This type of switch is constructed by attaching a detection coil wound around a ferrite core to a printed circuit board on which a detection circuit is mounted with an adhesive or the like. When approaching, the switching operation is performed based on the fact that the coil loss increases and the oscillation amplitude decreases. However, since the detection coil occupies a large area, a large noise component is induced in the detection coil, which causes a malfunction and a decrease in detection accuracy.

【0003】そこで、従来、例えば実開昭61−179
638号公報に示すように、プリント基板にシールド用
の導体パターンを設け、その上に検出コイルを張り付け
て検出コイルを電気的にシールドする構成が提供されて
いた。
Therefore, in the prior art, for example, the actual development Sho 61-179.
As disclosed in Japanese Patent No. 638, there has been provided a structure in which a printed circuit board is provided with a conductor pattern for shielding, and a detection coil is attached thereon to electrically shield the detection coil.

【0004】[0004]

【発明が解決しようとする課題】ところが、上述のよう
に検出コイルの裏面にシールドパターンを設けると、こ
こに渦電流損が発生することを避け得ない。磁束密度は
コイルからの距離に反比例するから、検出コイルのすぐ
近くにシールドパターンを設けると、検出コイルからの
漏れ磁束が少なくとも大きな損失が発生し、発振振幅が
大きく低下する傾向を呈する。
However, when the shield pattern is provided on the back surface of the detection coil as described above, eddy current loss is unavoidable. Since the magnetic flux density is inversely proportional to the distance from the coil, when a shield pattern is provided in the immediate vicinity of the detection coil, the leakage magnetic flux from the detection coil causes at least a large loss, and the oscillation amplitude tends to be greatly reduced.

【0005】ここで、シールドパターンにおける損失
が、いかなる状況でも同様に発生すれば単に平行的なレ
ベル変化となるから問題を生じないが、実際には、検出
コイルと被検出物体との間の距離が遠ければシールドパ
ターンにおける損失の割合が大きく、その距離が近くな
れば被検出物体における損失割合が増大してシールドパ
ターンにおける損失割合が減少することになる。具体的
には、被検出物体と検出コイルとの間の距離を横軸に採
り、発振振幅を縦軸に採ってシールドパターンが有ると
きと無いときとの発振振幅変化を描くと図6に示すよう
になり、シールドパターンがある場合には微小な距離変
化に対する発振振幅の変化が小さくなってしまう。この
ことは、より遠い距離において被検出物体の近接に伴う
スイッチング動作を行い得ないことを意味する。また、
シールドパターンが無い場合と同様な発振振幅を確保し
ようとすると、渦電流損による発振振幅の低下を補うた
めにコイル電流を増大させる必要があり、このために近
接スイッチの消費電流が増大するという問題を招く。
Here, if the loss in the shield pattern similarly occurs in any situation, it simply causes a level change in parallel, so that no problem occurs, but in reality, the distance between the detection coil and the object to be detected is small. Is larger, the loss ratio in the shield pattern is large, and as the distance is shorter, the loss ratio in the detected object increases and the loss ratio in the shield pattern decreases. Specifically, the distance between the object to be detected and the detection coil is plotted on the abscissa and the oscillation amplitude is plotted on the ordinate, and the change in the oscillation amplitude with and without the shield pattern is shown in FIG. When the shield pattern is provided, the change in the oscillation amplitude with respect to a minute change in distance becomes small. This means that the switching operation accompanying the proximity of the detected object cannot be performed at a farther distance. Also,
In order to secure the same oscillation amplitude as when there is no shield pattern, it is necessary to increase the coil current in order to compensate for the reduction in oscillation amplitude due to eddy current loss, which increases the current consumption of the proximity switch. Invite.

【0006】また、近年、この種の近接スイッチでは、
検出距離を長くすることが要望されており、このために
検出コイルのコアとして漏れ磁束が少ないE形コアに代
えて、開放度が高いいわゆるT形コアを使用することが
考えられている。しかし、このようにコアの開放度が高
くなればなるほど、漏れ磁束が増大するためにシールド
パターンにおける損失が増大し、上述の問題がより深刻
になるという傾向があった。
Recently, in this type of proximity switch,
It is desired to increase the detection distance, and for this reason, it is considered that a so-called T-shaped core having a high degree of openness is used as the core of the detection coil instead of the E-shaped core having a small leakage flux. However, the higher the degree of openness of the core, the more the leakage flux increases, so that the loss in the shield pattern increases, and the above-mentioned problem tends to become more serious.

【0007】本発明は上記事情に鑑みてなされたもので
あり、従って、検出コイルの電気的シールドを確実に図
りながら、シールド導体層に起因する電磁的損失を極力
小さく抑え、もって高い検出精度を得ると共に省電力化
を可能にできる近接スイッチを提供することを目的とす
る。
The present invention has been made in view of the above circumstances. Therefore, while ensuring the electric shield of the detection coil, the electromagnetic loss caused by the shield conductor layer is suppressed as small as possible, and the high detection accuracy is achieved. It is an object of the present invention to provide a proximity switch that can obtain the power and save power.

【0008】[0008]

【課題を解決するための手段】本発明に係る近接スイッ
チは、検出コイルを保持する基板に検出コイルを電気的
にシールドするシールド導体層を設けると共に、そのシ
ールド導体層にはこれを面方向に分断するスリットを形
成したところに特徴を有する。上記スリットは、シール
ド導体層のうち検出コイルの中心部に対応する位置から
放射方向に延びるように形成することがより好ましい。
In the proximity switch according to the present invention, a shield conductor layer for electrically shielding the detection coil is provided on a substrate holding the detection coil, and the shield conductor layer is provided with the shield conductor layer in a plane direction. The feature is that a slit for dividing is formed. More preferably, the slit is formed so as to extend in the radial direction from a position corresponding to the center of the detection coil in the shield conductor layer.

【0009】[0009]

【作用】検出コイルは基板上に位置するシールド導体層
によって電気的にシールドされ、耐ノイズ性が高まる。
そして、このシールド導体層にはこれを面方向に分断す
るようにしてスリットが形成されているから、シールド
導体層に検出コイルからの磁束が鎖交しても渦電流損は
小さくなり、検出コイルの損失が小さくなる。また、シ
ールド導体層のうち検出コイルの中心部に対応する位置
からスリットを放射方向に延びるように形成したもので
は、渦電流が検出コイルと同心状に発生するという事情
のもとで渦電流を効果的に減殺することができるように
なる。
The detection coil is electrically shielded by the shield conductor layer located on the substrate, and the noise resistance is enhanced.
Since a slit is formed in the shield conductor layer so as to divide the shield conductor layer in the surface direction, the eddy current loss is reduced even if the magnetic flux from the detection coil is linked to the shield conductor layer. Loss is reduced. Further, in the shield conductor layer in which the slit is formed so as to extend in the radial direction from the position corresponding to the central portion of the detection coil, the eddy current is generated in a situation where the eddy current is generated concentrically with the detection coil. You will be able to effectively kill.

【0010】[0010]

【発明の効果】このように本発明の近接スイッチによれ
ば、シールド導体層によって検出コイルの電気的シール
ドを確実に行い得る上に、そのシールド導体層に検出コ
イルからの磁束が鎖交して渦電流損が発生することを極
力抑えることができるから、検出精度を高くできると共
に省電力化が可能になるという優れた効果を奏する。
As described above, according to the proximity switch of the present invention, the shield conductor layer can surely electrically shield the detection coil, and the magnetic flux from the detection coil is linked to the shield conductor layer. Since it is possible to suppress the occurrence of eddy current loss as much as possible, it is possible to improve detection accuracy and save power.

【0011】[0011]

【実施例】以下本発明の第1実施例を図1ないし図3を
参照して説明する。本実施例の近接スイッチはプリント
回路基板11を樹脂12にてモールドして構成されてい
る。この回路基板11は、例えばセラミック製の両面基
板であり、一方の面に検出コイル13が装着され、他方
の面に検出回路の大部分を構成するIC等が実装されて
いる検出コイル13は例えばフェライト製のコア14に
マグネットワイヤを多数回巻回して構成され、そのコア
14は円形基板14aの中央に巻芯突部14bを突設し
て軸方向に沿った断面がT字形をなす、いわゆるT形コ
アで、漏れ磁束を比較的多くして被検出物体の長距離検
出が可能になるようにしている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A first embodiment of the present invention will be described below with reference to FIGS. The proximity switch of this embodiment is formed by molding the printed circuit board 11 with resin 12. The circuit board 11 is, for example, a ceramic double-sided board, and the detection coil 13 having one surface on which the detection coil 13 is mounted and the other surface on which an IC or the like forming a large part of the detection circuit is mounted are, for example, A magnet wire is wound around a ferrite core 14 a large number of times. The core 14 has a winding core projection 14b protruding from the center of a circular substrate 14a, and the section along the axial direction is T-shaped. The T-shaped core has a relatively large leakage flux to enable long-distance detection of an object to be detected.

【0012】さて、回路基板11のうち上記検出コイル
13の装着側の面には図3に拡大して示すような導体パ
ターンが例えば銀パラジウムペーストの印刷焼成によっ
て形成されており、これを詳述する。回路基板11の図
示上半部は検出コイル13の装着領域で、ここのほぼ全
域にシールド導体層15が形成されている。このシール
ド導体層15には検出コイル13の中心部に対応する位
置から放射方向に延びる多数のスリット16が形成さ
れ、シールド導体層15をその中心部を残して周方向に
間欠的に分断した形態となっている。また、このシール
ド導体層15からは、検出コイル13の装着領域の外側
に向けて連結部15aが延び出しており、その先端に接
地側ランド17が形成されている。更に、検出コイル1
3の装着領域の外側のうち上記接地側ランド17の隣に
は信号側ランド18が形成されており、またシールド導
体層15及び信号側ランド18は、スルーホール19,
20を介して裏面の検出回路と電気的に接続されてい
る。
Now, on the surface of the circuit board 11 on which the detection coil 13 is mounted, a conductor pattern as shown in an enlarged view in FIG. 3 is formed by printing firing of silver-palladium paste, for example. To do. The upper half of the circuit board 11 in the drawing is a mounting area of the detection coil 13, and the shield conductor layer 15 is formed almost all over this area. The shield conductor layer 15 is provided with a large number of slits 16 extending in a radial direction from a position corresponding to the center of the detection coil 13, and the shield conductor layer 15 is intermittently divided in the circumferential direction while leaving the center thereof. Has become. A connecting portion 15a extends from the shield conductor layer 15 toward the outside of the mounting area of the detection coil 13, and a ground side land 17 is formed at the tip thereof. Furthermore, the detection coil 1
A signal side land 18 is formed next to the ground side land 17 on the outside of the mounting region of No. 3, and the shield conductor layer 15 and the signal side land 18 are formed with through holes 19,
It is electrically connected to the detection circuit on the back surface via 20.

【0013】上述の導体パターンを備えた回路基板11
に対し、検出コイル13はそのコア14の円形基板14
aが例えば接着剤によってシールド導体層15の中央部
に固着され、その上で、検出コイル13の信号側リード
線13aが上記信号側ランド18に半田付けされ、接地
側リード線13bが接地側ランド17に半田付けされて
いる。なお、図1及び図2に示した符号21は、回路基
板11の所定の端子部に半田付けされたケーブルを示
す。
Circuit board 11 having the above-mentioned conductor pattern
On the other hand, the detection coil 13 has a circular substrate 14 of its core 14.
a is fixed to the central portion of the shield conductor layer 15 with an adhesive, for example, and the signal side lead wire 13a of the detection coil 13 is soldered to the signal side land 18, and the ground side lead wire 13b is grounded. Soldered to 17. Reference numeral 21 shown in FIGS. 1 and 2 denotes a cable soldered to a predetermined terminal portion of the circuit board 11.

【0014】上記構成の近接スイッチによれば、検出回
路に含まれる発振回路によって検出コイル13に高周波
電流が流され、検出コイル13を中心に高周波磁界が発
生する。この検出コイル13に金属製の被検出物体が接
近すると、ここに発生する渦電流損によって検出コイル
13における損失が増大するため、発振振幅が低下し、
これに基づき検出回路にてスイッチング動作が行われ
る。ここで、外部電界が検出コイル13に作用しても、
検出コイル13の裏面には接地側に接続されたシールド
導体層15が形成されているから、検出コイル13に誘
導されるノイズ成分は極めて小さくなり、電界ノイズに
起因する誤動作を防止できる。なお、シールド導体層1
5には多数のスリット16が形成されているが、その幅
は狭いからシールド効果にほとんど影響を与えず、優れ
た耐ノイズ性を発揮させることができる。
According to the proximity switch having the above structure, a high frequency current is caused to flow through the detection coil 13 by the oscillation circuit included in the detection circuit, and a high frequency magnetic field is generated around the detection coil 13. When an object to be detected made of metal approaches the detection coil 13, the loss in the detection coil 13 increases due to the eddy current loss generated there, and the oscillation amplitude decreases,
Based on this, the switching operation is performed in the detection circuit. Here, even if an external electric field acts on the detection coil 13,
Since the shield conductor layer 15 connected to the ground side is formed on the back surface of the detection coil 13, the noise component induced in the detection coil 13 becomes extremely small, and malfunction due to electric field noise can be prevented. The shield conductor layer 1
Although a large number of slits 16 are formed in 5, the width of the slits 16 is narrow, so that the shielding effect is hardly affected and excellent noise resistance can be exhibited.

【0015】一方、そのシールド導体層15には検出コ
イル13が作る高周波磁束が鎖交するため、シールド導
体層15に渦電流が発生する。しかし、このシールド導
体層15には多数のスリット16が形成されて電流経路
が分断されているから、渦電流が流れる経路は長くなっ
て電流値は低く抑えられる。しかも、この実施例では、
スリット16は検出コイル13の中心部に対応する位置
から放射状をなすように形成されているから、渦電流が
検出コイル13を中心にして同心状に流れようとすると
いう事情のもとで、その電流経路を効果的に分断するこ
とになり、渦電流を飛躍的に抑えることができることに
なる。この結果、検出コイル13における損失が低く抑
えられるから、被検出物体の接近を高精度で検出するこ
とができるようになり、また省電力化を図ることができ
る。
On the other hand, since the high frequency magnetic flux generated by the detection coil 13 is linked to the shield conductor layer 15, an eddy current is generated in the shield conductor layer 15. However, since a large number of slits 16 are formed in the shield conductor layer 15 to divide the current path, the path through which the eddy current flows becomes long and the current value can be kept low. Moreover, in this embodiment,
Since the slits 16 are formed to radiate from the position corresponding to the center of the detection coil 13, the eddy current tends to flow concentrically around the detection coil 13 under the circumstances. The current path is effectively divided, and the eddy current can be dramatically suppressed. As a result, the loss in the detection coil 13 is suppressed to a low level, so that the approach of the detected object can be detected with high accuracy, and power saving can be achieved.

【0016】ちなみに、本実施例構造の近接スイッチに
よる検出コイル13の損失を、シールド導体層を設けな
いものと、スリットの無いシールド導体層を設けたもの
とを比較して実測した結果を図5に示す。この測定例で
は、コア14はフェライト製で円形基板14aの直径が
11.3mm、高さが3.3mm、マグネットワイヤ径が
0.13mm、巻数55巻で、0.2Vrms 、300kH
zで高周波電流を流している。また、被検出物体は30
mm角、厚さ1mmの鉄板を使用し、被検出物体と検出コイ
ル13との間の距離に応じて検出コイル13の損失を測
定した。シールド導体層を設けないものは実線で示し、
スリットが無い(いわゆる「べた」の)シールド導体層
を設けたものは一点鎖線で示し、本実施例構造のシール
ド導体層15を設けたものは二点鎖線で示してある。こ
の実験からも明かなように、スリットが無いシールド導
体層を設けると大きな損失が生じるが、本実施例構造の
シールド導体層15を設けたものは、シールド導体層が
無いものと同程度の低損失となる。
By the way, the loss of the detection coil 13 due to the proximity switch of the present embodiment structure is actually measured by comparing the loss of the detection coil 13 with that without the shield conductor layer and that with the shield conductor layer without slits. Shown in. In this measurement example, the core 14 is made of ferrite, the circular substrate 14a has a diameter of 11.3 mm, a height of 3.3 mm, a magnet wire diameter of 0.13 mm, a number of turns of 55, 0.2 Vrms, 300 kHz.
A high-frequency current is flowing at z. The detected object is 30
The loss of the detection coil 13 was measured according to the distance between the object to be detected and the detection coil 13 using an iron plate having a square size of 1 mm and a thickness of 1 mm. Those without a shield conductor layer are shown by solid lines,
The one provided with a shield conductor layer having no slit (so-called "solid") is shown by a one-dot chain line, and the one provided with the shield conductor layer 15 of the structure of this embodiment is shown by a two-dot chain line. As is clear from this experiment, when a shield conductor layer having no slit is provided, a large loss occurs. However, the shield conductor layer 15 having the structure of the present embodiment has the same low loss as the shield conductor layer having no shield conductor layer. It will be a loss.

【0017】このように本実施例によれば、シールド導
体層15によって電界ノイズに対する優れた耐性を得な
がら、ここにスリット16を形成したから渦電流損を減
少させて検出コイル13における損失を大きく低減させ
ることができる。これにより、被検出物体の検出を高精
度で行うことができるようになり、また消費電力を減少
させることができる。
As described above, according to the present embodiment, while the shield conductor layer 15 provides excellent resistance to electric field noise, since the slit 16 is formed here, the eddy current loss is reduced and the loss in the detection coil 13 is increased. Can be reduced. This makes it possible to detect the detected object with high accuracy and reduce power consumption.

【0018】なお、本発明は上記実施例に限定されるも
のではなく、例えば次のように要旨を逸脱しない範囲で
種々変更して実施することができる。
The present invention is not limited to the above-mentioned embodiments, but can be implemented with various modifications within the scope not departing from the gist of the invention, for example.

【0019】(イ)シールド導体層には必ずしも放射状
のスリットを形成するに限らず、例えば図4に第2実施
例として示すように、検出コイルの配置領域に設けたシ
ールド導体層30に対してスリット31を蛇行状に形成
するようにしてもよく、この形態のスリット31も本願
の特許請求の範囲にいう「渦電流損を減少させるスリッ
ト」の概念に含まれる。
(B) The radial slits are not necessarily formed in the shield conductor layer, and for example, as shown in FIG. 4 as a second embodiment, the shield conductor layer 30 provided in the detection coil disposition region is not shown. The slit 31 may be formed in a meandering shape, and the slit 31 of this form is also included in the concept of “a slit for reducing eddy current loss” in the claims of the present application.

【0020】(ロ)上記実施例ではシールド導体層15
を導電性ペーストの印刷焼成によって形成したが、これ
に限られず、例えば金属メッキ、金属箔の回路基板への
接着、金属の蒸着或いは回路基板に予め設けた金属箔の
エッチング等によってシールド導体層を形成してもよ
く、これらを含めて他のいかなる形成方法によって形成
されたいかなる導体層でも「基板に検出コイルを電気的
にシールドするシールド導体層」として機能するもので
あれば、本願の特許請求の範囲に言う「シールド導体
層」の概念に含まれる。
(B) In the above embodiment, the shield conductor layer 15
Was formed by printing and firing a conductive paste, but the invention is not limited to this, and the shield conductor layer is formed by, for example, metal plating, adhesion of a metal foil to a circuit board, vapor deposition of metal, or etching of a metal foil previously provided on the circuit board. Any conductive layer that may be formed by any other forming method including these, as long as it functions as a “shield conductive layer that electrically shields the detection coil on the substrate”, It is included in the concept of "shield conductor layer" in the range of.

【0021】(ハ)上記実施例では、被検出物体の検出
可能距離を長くするために漏れ磁束が多いT形コアを使
用したが、これに限らず、コイルの外周側にも環状に磁
性材が存在するいわゆるE形コアを使用したり、或い
は、無芯の検出コイルであってもよく、これらも全て本
願の特許請求の範囲に言う「検出コイル」の概念に含ま
れる。
(C) In the above embodiment, the T-shaped core having a large leakage flux is used in order to increase the detectable distance of the object to be detected, but the present invention is not limited to this, and the magnetic material is annularly formed on the outer peripheral side of the coil. May be used, or a coreless detection coil may be used, and these are all included in the concept of "detection coil" referred to in the claims of the present application.

【0022】その他、本発明は上記しかつ図面に限定さ
れるものではなく、要旨を逸脱しない範囲内で種々変更
して実施することができるものである。
Besides, the present invention is not limited to the above description and is not limited to the drawings, and various modifications can be made without departing from the scope of the invention.

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

【図1】本発明の第1実施例に係る近接スイッチの横断
面図
FIG. 1 is a cross-sectional view of a proximity switch according to a first embodiment of the present invention.

【図2】同じく縦断面図[Fig. 2] Similarly, a vertical sectional view

【図3】同じく回路基板の平面図FIG. 3 is a plan view of the same circuit board.

【図4】本発明の第2実施例に係る回路基板の平面図FIG. 4 is a plan view of a circuit board according to a second embodiment of the present invention.

【図5】第1実施例の構造における検出コイルの損失を
測定したグラフ
FIG. 5 is a graph in which the loss of the detection coil in the structure of the first embodiment is measured.

【図6】シールドが無いものと従来のシールドパターン
を設けた近接スイッチとを比較するための発振振幅を示
すグラフ
FIG. 6 is a graph showing an oscillation amplitude for comparison between a switch without a shield and a proximity switch provided with a conventional shield pattern.

【符号の説明】[Explanation of symbols]

11…プリント回路基板(基板) 13…検出コイル 14…コア 15…シールド導体層 16…スリット 30…シールド導体層 31…スリット 11 ... Printed circuit board (board) 13 ... Detection coil 14 ... Core 15 ... Shield conductor layer 16 ... Slit 30 ... Shield conductor layer 31 ... Slit

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 基板に設けた検出コイルに高周波電流を
流してその検出コイルへの物体の接近を検出してスイッ
チング動作を行うものにおいて、 前記基板に前記検出コイルを電気的にシールドするシー
ルド導体層を設けると共に、そのシールド導体層にはそ
の渦電流損を減少させるスリットを形成したことを特徴
とする近接スイッチ。
1. A shield conductor for electrically shielding the detection coil on the substrate, wherein a high frequency current is passed through the detection coil provided on the substrate to detect an approach of an object to the detection coil to perform a switching operation. A proximity switch characterized in that a slit for reducing the eddy current loss is formed in the shield conductor layer while the layer is provided.
【請求項2】 スリットは、シールド導体層のうち検出
コイルの中心部に対応する位置から放射方向に延びるよ
うに形成されていることを特徴とする近接スイッチ。
2. The proximity switch, wherein the slit is formed so as to extend in a radial direction from a position corresponding to the center of the detection coil in the shield conductor layer.
JP5269517A 1993-09-30 1993-09-30 Proximity switch Expired - Fee Related JP2534824B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5269517A JP2534824B2 (en) 1993-09-30 1993-09-30 Proximity switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5269517A JP2534824B2 (en) 1993-09-30 1993-09-30 Proximity switch

Publications (2)

Publication Number Publication Date
JPH07105808A JPH07105808A (en) 1995-04-21
JP2534824B2 true JP2534824B2 (en) 1996-09-18

Family

ID=17473507

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5269517A Expired - Fee Related JP2534824B2 (en) 1993-09-30 1993-09-30 Proximity switch

Country Status (1)

Country Link
JP (1) JP2534824B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ATE427585T1 (en) * 2005-07-01 2009-04-15 Senstronic S A INDUCTIVE PRESENCE, PROXIMITY OR POSITION SENSOR
WO2010087317A1 (en) 2009-01-30 2010-08-05 株式会社村田製作所 Contactless power receiving device

Also Published As

Publication number Publication date
JPH07105808A (en) 1995-04-21

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