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JPH0668337B2 - Self-holding gas cutoff valve - Google Patents
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JPH0668337B2 - Self-holding gas cutoff valve - Google Patents

Self-holding gas cutoff valve

Info

Publication number
JPH0668337B2
JPH0668337B2 JP8878286A JP8878286A JPH0668337B2 JP H0668337 B2 JPH0668337 B2 JP H0668337B2 JP 8878286 A JP8878286 A JP 8878286A JP 8878286 A JP8878286 A JP 8878286A JP H0668337 B2 JPH0668337 B2 JP H0668337B2
Authority
JP
Japan
Prior art keywords
coil
temperature
flux density
yoke
magnetic flux
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
JP8878286A
Other languages
Japanese (ja)
Other versions
JPS62246670A (en
Inventor
昌彦 山本
正幸 岡本
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 JP8878286A priority Critical patent/JPH0668337B2/en
Publication of JPS62246670A publication Critical patent/JPS62246670A/en
Publication of JPH0668337B2 publication Critical patent/JPH0668337B2/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】 産業上の利用分野 本発明は、ガス機器やガス配管中に配置され、異常発生
時に外部信号などにより、ガス通路を遮断する自己保持
型ガス遮断弁に関するものである。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a self-holding type gas cutoff valve which is arranged in a gas device or gas pipe and shuts off a gas passage by an external signal or the like when an abnormality occurs.

従来の技術 従来の自己保持型ガス遮断弁は第1図に示すようなもの
であり、コイルユニット上部1にマグネット(永久磁
石)2a,2bを同極同士向い合せに装着し、の字型に曲
げたヨーク3にコイルユニット1をセットしている。ヨ
ーク3の底面には磁性体のピース4がかしめられてお
り、ピース4が嵌入可能な貫通孔5がコイルユニット1
に設けられている。コイルユニット下部の周部にコイル
6が巻かれており、その巻き線7の両端7a,7bが外部に
出ている。コイルユニット1はベースフランジ8により
固定され、ベースフランジ8はヨーク3にカシメられて
いる。プランジャ9の底端はピース4の上面とで吸着面
9aを形成しており、プランジャ9の頭端部には、ベンゴ
ムウケ10がカシメられており、ベンゴムウケ10の上部に
ベンゴム11が取り付けられている。ベンゴムウケ10とベ
ースフランジ8の間には、スプリング12が設けられてお
り、マグネット2a,2bの磁気回路13a,13bが形成されるこ
とにより、プランジャ9の吸着面9aがピース4に吸い付
くように吸着力(吸着力はマグネットの磁力が大きけれ
ば大きい程大となる。)が発生する。一方この吸着力を
打ち消す方向に逆磁界が発生するように巻線7に電圧
(パルス状の電圧で可)を加えれば、スプリング12の反
発力によりプランジャ9すなわちベンゴム11が飛び出し
て第2図に示すようになる。この吸着力を打ち消して、
プランジャ9が飛び出すときの印加電圧を作動電圧とい
う。この作動電圧は、バネの支発力が一定であるので、
吸着力を発生するマグネットの磁力と逆磁界を発生する
コイルに流れる電流を規定するコイル抵抗により決ま
る。またマグネットの磁力は、残留磁束密度が大きい程
強くなるが、この残留磁束密度は周囲温度の影響を受
け、またマグネットの種類によって、温度1℃当りの残
留磁束密度変化:ΔBr/Br/℃(温度係数)が異なって
くる。また、逆磁界の強さは、コイルに流れる電流が大
きい程強くなるが、コイル抵抗値も周囲温度に影響され
るので、印加電圧を一定とした場合逆磁界の磁束密度も
周囲の温度の影響を受ける。このように、作動電圧は、
マグネットの磁力(残留磁束密度の大きさによる)とコ
イルの抵抗値により決まりこれらは温度に関係してい
る。
2. Description of the Related Art A conventional self-holding type gas cutoff valve is as shown in FIG. 1, in which magnets (permanent magnets) 2a and 2b are attached to the upper part 1 of the coil unit so that the same poles face each other, and the shape becomes a square shape. The coil unit 1 is set on the bent yoke 3. A magnetic piece 4 is crimped on the bottom surface of the yoke 3, and a through hole 5 into which the piece 4 can be fitted has a through hole 5 formed therein.
It is provided in. The coil 6 is wound around the lower part of the coil unit, and both ends 7a and 7b of the winding wire 7 are exposed to the outside. The coil unit 1 is fixed by a base flange 8, and the base flange 8 is crimped to the yoke 3. The bottom end of the plunger 9 and the upper surface of the piece 4 are suction surfaces.
9a is formed, and a Ben rubber rake 10 is caulked at the head end of the plunger 9, and a Ben rubber 11 is attached to the upper part of the Ben rubber rake 10. A spring 12 is provided between the bevel rubber hook 10 and the base flange 8 to form the magnetic circuits 13a and 13b of the magnets 2a and 2b so that the attraction surface 9a of the plunger 9 may be attracted to the piece 4. Adsorption force (the larger the magnetic force of the magnet, the larger the adsorption force) is generated. On the other hand, if a voltage (a pulsed voltage is acceptable) is applied to the winding 7 so that a reverse magnetic field is generated in the direction of canceling out the attraction force, the repulsive force of the spring 12 causes the plunger 9, that is, the rubber bell 11 to pop out, and as shown in FIG. As shown. To cancel this attraction,
The applied voltage when the plunger 9 jumps out is called the operating voltage. Since this spring has a constant spring force,
It is determined by the magnetic force of the magnet that generates the attractive force and the coil resistance that defines the current that flows in the coil that generates the reverse magnetic field. Also, the magnetic force of the magnet becomes stronger as the residual magnetic flux density increases, but this residual magnetic flux density is affected by the ambient temperature, and depending on the type of magnet, the residual magnetic flux density change per 1 ° C temperature: ΔBr / Br / ° C ( The temperature coefficient) is different. Also, the strength of the reverse magnetic field increases as the current flowing through the coil increases, but the coil resistance value is also affected by the ambient temperature. Therefore, when the applied voltage is constant, the magnetic flux density of the reverse magnetic field also depends on the ambient temperature. Receive. Thus, the operating voltage is
It is determined by the magnetic force of the magnet (depending on the magnitude of the residual magnetic flux density) and the resistance value of the coil, and these are related to temperature.

発明が解決しようとする問題点 従来では一般に永久磁石は、同一のものどうし(たとえ
ばフェライト磁石同士あるいは希士類磁石同士)を使用
しており、温度係数がたとえば−0.18%/℃近辺のマグ
ネットのみを用いた遮断弁においては、導体線の抵抗値
の温度係数が+0.4%/℃であればコイル抵抗値の温度
変化による作動電圧への影響よりマグネットの温度係数
が−0.18%/℃近辺であるので、マグネットの残留磁束
密度の温度変化による作動電圧への影響の方が大となる
ため、第4図に示すような特性となる。第4図におい
て、実線は常温において作動電圧規格値Vで作動する
遮断弁作動電圧温度特性で点線は個々のバラツキを考慮
した作動電圧温度特性である。この温度、駆動電源がV
であるため、個々のバラツキを考慮すると作動下限温
度T以上の温度でしか使用できないことになる。
Problems to be Solved by the Invention Conventionally, generally, the same permanent magnets are used (for example, ferrite magnets or rare magnets), and only a magnet having a temperature coefficient of around −0.18% / ° C. is used. If the temperature coefficient of resistance value of the conductor wire is + 0.4% / ℃, the temperature coefficient of magnet is around −0.18% / ℃ due to the influence of coil temperature change on operating voltage. Therefore, the influence of the temperature change of the residual magnetic flux density of the magnet on the operating voltage is larger, and the characteristics are as shown in FIG. In FIG. 4, the solid line shows the operating voltage temperature characteristic of the shut-off valve which operates at the operating voltage standard value VA at room temperature, and the dotted line shows the operating voltage temperature characteristic in consideration of individual variations. At this temperature, the drive power supply is V
Since it is D , it can be used only at a temperature equal to or higher than the operation lower limit temperature T L in consideration of individual variations.

また、温度係数がたとえば−0.04%/℃近辺のマグネッ
トのみを用いた遮断弁においては、コイル抵抗値の温度
変化による作動電圧への影響の方が、マグネットの温度
係数が−0.04%/℃近辺であるのでマグネットの残留磁
束密度の温度変化よる作動電圧への影響より大きくな
り、第5図に示すような特性となる。この場合、温度係
数が−0.18%/℃近辺のマグネットのみを使用したもの
とは逆に、高温で問題となり、作動上限温度T以下の
温度でしか使用できないことになる。Tより高い温度
あるいはTより低い温度においても使用可能にするに
は、バラツキ巾を従来以上に小さくするよう性能を出す
か、バラツキ巾を小さくするように、選別工程において
検査合格巾を小さくして、選別しなければならないとい
う問題があった。
Also, in a shut-off valve that uses only a magnet with a temperature coefficient of around -0.04% / ° C, the effect of the change in coil resistance on the operating voltage is that the temperature coefficient of the magnet has a temperature coefficient of around -0.04% / ° C. Therefore, the effect on the operating voltage due to the temperature change of the residual magnetic flux density of the magnet is larger, and the characteristics shown in FIG. 5 are obtained. In this case, contrary to what temperature coefficient using only magnet near -0.18% / ° C., high temperature becomes a problem, it will not be used only in operating upper limit temperature T H or lower. To also enable the T H higher temperature or T L lower temperatures, or issues of performance to reduce the variation width than before, so as to reduce the variation width, reduce the inspection pass width in a selection process Then, there was a problem that it had to be selected.

本発明は、上記問題点を解消するものであり、従来のよ
うに環境温度に影響されず、あらゆる温度範囲にて安定
した性能を有する遮断弁を提供するものである。
The present invention solves the above-mentioned problems, and provides a shutoff valve which is not affected by the ambient temperature and has stable performance in all temperature ranges as in the prior art.

問題点を解決するための手段 上記問題点を解決するため、本発明は、貫通孔を有する
ボビン周部に導体線を回巻して形成されたコイルを、
字形状の磁性体からなるヨークの字内側底部に配置
し、前記貫通孔に、磁性体からなり、頭端部に弁体を有
し、底端部が前記ヨークに当接可能なプランジャを出退
自在に設け、前記ヨークを固定するベースフランジと前
記弁体間に、弾性体を設け、前記ヨークの字両側部
に、前記弾性体の付勢力に抗して前記プランジャの底端
部を前記ヨークを介して吸着可能な一対の永久磁石を、
同極を対向させて設け、前記一対の永久磁石のそれぞれ
の磁石を、前記コイルの発生磁束密度の温度変位に較べ
て残留磁束密度の温度変位が大なるものと小なるものと
で構成し、前記一対の永久磁石の残留磁束密度の温度変
位が前記コイルの発生磁束密度の温度変位に対応するよ
うに構成したものである。
Means for Solving the Problems In order to solve the above problems, the present invention provides a coil formed by winding a conductor wire around a bobbin having a through hole.
It is placed in the bottom of the inside of the Y-shaped yoke made of magnetic material, and has a valve body at the head end that is made of a magnetic material in the through hole. An elastic body is provided between the valve body and a base flange that fixes the yoke, and the bottom end portion of the plunger is provided on both side portions of the yoke against the biasing force of the elastic body. A pair of permanent magnets that can be attracted via the yoke,
The same poles are provided to face each other, and each magnet of the pair of permanent magnets is configured such that the temperature variation of the residual magnetic flux density is large and the temperature variation of the residual magnetic flux density is small compared to the temperature displacement of the magnetic flux density generated by the coil. The temperature variation of the residual magnetic flux density of the pair of permanent magnets corresponds to the temperature variation of the generated magnetic flux density of the coil.

作用 上記構成により、永久磁石の残留磁束密度の温度変位は
各々の永久磁石によって異なるが、両永久磁石の磁力が
あわさるヨークのプランジャ当接部における残留磁束密
度の温度変位は、前記2者の中間的なものとなり、コイ
ルの発生磁束密度の温度変位に対応することができるの
で、プランジャとヨークを離間させるに必要な逆磁界を
コイルに生じせしめる作動電圧は、周囲の温度変化の影
響を受けず一定のものとなり、広い温度範囲にわたって
作用させることが出来る。
Action With the above configuration, the temperature variation of the residual magnetic flux density of the permanent magnet differs depending on each permanent magnet, but the temperature variation of the residual magnetic flux density at the plunger abutting portion of the yoke where the magnetic forces of both permanent magnets meet is the same as that of the above two. Since it is an intermediate value and can cope with the temperature variation of the magnetic flux density generated by the coil, the operating voltage that causes the reverse magnetic field required for separating the plunger and the yoke from occurring in the coil is not affected by ambient temperature changes. Instead, it becomes constant and can act over a wide temperature range.

実施例 以下、本発明の一実施例を説明する。本実施例は、第1
図のマグネット2aあるいは2bに温度係数が−0.18%/℃
近辺のマグネット(例えば、フェライト磁石)を用い、
対向する側のマグネット2bあるいは2aに温度係数が−0.
04%/℃近辺のマグネット(例えば、希土類磁石)を用
いる以外は、従来の遮断弁と機械的構成は変わらないの
で説明を省略する。しかしながら、温度係数が−0.18%
/℃近辺のマグネットと−0.04%/℃近辺のマグネット
を組み合せてこれら2種類のマグネットを同時に用いる
ことにより、コイル抵抗の温度変化による作動電圧への
影響とマグネットの温度係数による作動電圧の影響の均
衡がとれ、第3図に示すように、あらゆる温度範囲に
て、ほぼ一定の電圧で作動することとなる。
Example One example of the present invention will be described below. This embodiment is the first
The temperature coefficient of the magnet 2a or 2b in the figure is -0.18% / ℃
Use a nearby magnet (for example, a ferrite magnet),
The temperature coefficient of the opposite magnet 2b or 2a is −0.
Except for using a magnet near 04% / ° C (for example, a rare earth magnet), the mechanical structure is the same as that of the conventional shutoff valve, and therefore the description is omitted. However, the temperature coefficient is -0.18%
By combining these two types of magnets by combining a magnet near / ° C and a magnet near -0.04% / ° C, it is possible to reduce the influence of the coil resistance on the operating voltage and the effect of the magnet temperature coefficient on the operating voltage. It is balanced and, as shown in FIG. 3, operates at a substantially constant voltage in all temperature ranges.

発明の効果 以上述べたごとく本発明によれば、遮断弁に用いる永久
磁石として、コイルの発生磁束密度の温度変位に較べ残
留磁束密度の温度変位が大なるものと、小なるものの2
種類の永久磁石を組み合せて用いることにより、常温計
において、作動電圧が駆動電源電圧以下であれば、あら
ゆる環境温度で使用することが出来る。
EFFECTS OF THE INVENTION As described above, according to the present invention, as the permanent magnets used in the shutoff valve, there are two types of permanent magnets, one having a large temperature displacement of the residual magnetic flux density as compared with the temperature displacement of the magnetic flux density generated by the coil and the other having a small temperature displacement.
By using various types of permanent magnets in combination, the ambient temperature meter can be used at any ambient temperature as long as the operating voltage is equal to or lower than the driving power supply voltage.

【図面の簡単な説明】 第1図は本発明の実施例における遮断弁の構成図兼従来
例の構成図および開状態図、第2図は第1図の遮断弁の
閉状態図、第3図は本発明の実施例の作動電圧温度特性
図、第4図・第5図は従来の作動電圧温度特性図であ
る。 1……コイルユニット、2a,2b……マグネット、3……
ヨーク、4……ピース、5……貫通孔、6……コイル、
8……ベースフランジ、9……ブランジャ、10……ベン
ゴムウケ、11……ベンゴム、12……スプリング、13a,13
b……磁気回路
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram of a shutoff valve according to an embodiment of the present invention and a block diagram of a conventional example and an open state diagram. FIG. 2 is a closed state diagram of the shutoff valve of FIG. FIG. 4 is a diagram showing the operating voltage temperature characteristic of the embodiment of the present invention, and FIGS. 4 and 5 are conventional operating voltage temperature characteristic diagrams. 1 ... Coil unit, 2a, 2b ... Magnet, 3 ...
Yoke, 4 ... piece, 5 ... through hole, 6 ... coil,
8 ... Base flange, 9 ... Blancer, 10 ... Ben rubber bracket, 11 ... Ben rubber, 12 ... Spring, 13a, 13
b ... magnetic circuit

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】貫通孔を有するボビン周部に導体線を回巻
して形成されたコイルを、字形状の磁性体からなるヨ
ークの字内側底部に配置し、前記貫通孔に、磁性体か
らなり、頭端部に弁体を有し、底端部が前記ヨークに当
接可能なプランジャを出退自在に設け、前記ヨークを固
定支持するべースフランジと前記弁体間に、弾性体を設
け、前記ヨークの字両側部に、前記弾性体の付勢力に
抗して前記プランジャの底端部を前記ヨークを介して吸
着可能な一対の永久磁石を、同極を対向させて設け、前
記一対の永久磁石のそれぞれの磁石を、前記コイルの発
生極束密度の温度変位に較べて残留磁束密度の温度変位
が大なるものと小なるものとで構成し、前記一対の永久
磁石の残留磁束密度の温度変位が前記コイルの発生磁束
密度の温度変位に対応するように構成した自己保持型ガ
ス遮断弁。
1. A coil, which is formed by winding a conductor wire around a bobbin having a through hole, is arranged at the bottom of the inside of a yoke made of a letter-shaped magnetic material, and the through hole is made of a magnetic material. And has a valve body at the head end and a bottom end which is provided with a plunger capable of coming into contact with the yoke in a retractable manner, and an elastic body is provided between the base flange for fixedly supporting the yoke and the valve body. , A pair of permanent magnets that can attract the bottom end of the plunger through the yoke against the biasing force of the elastic body are provided on both sides of the yoke with the same poles facing each other. Of the permanent magnets of the pair of permanent magnets, the residual magnetic flux density of which is large and the residual magnetic flux density of which is small as compared with the temperature displacement of the generated pole flux density of the coil. The temperature displacement of the coil corresponds to the temperature displacement of the magnetic flux density generated by the coil. Self-hold gas shutoff valve configured as.
JP8878286A 1986-04-17 1986-04-17 Self-holding gas cutoff valve Expired - Lifetime JPH0668337B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8878286A JPH0668337B2 (en) 1986-04-17 1986-04-17 Self-holding gas cutoff valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8878286A JPH0668337B2 (en) 1986-04-17 1986-04-17 Self-holding gas cutoff valve

Publications (2)

Publication Number Publication Date
JPS62246670A JPS62246670A (en) 1987-10-27
JPH0668337B2 true JPH0668337B2 (en) 1994-08-31

Family

ID=13952416

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8878286A Expired - Lifetime JPH0668337B2 (en) 1986-04-17 1986-04-17 Self-holding gas cutoff valve

Country Status (1)

Country Link
JP (1) JPH0668337B2 (en)

Also Published As

Publication number Publication date
JPS62246670A (en) 1987-10-27

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