JPH0328043B2 - - Google Patents

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Publication number
JPH0328043B2
JPH0328043B2 JP60133211A JP13321185A JPH0328043B2 JP H0328043 B2 JPH0328043 B2 JP H0328043B2 JP 60133211 A JP60133211 A JP 60133211A JP 13321185 A JP13321185 A JP 13321185A JP H0328043 B2 JPH0328043 B2 JP H0328043B2
Authority
JP
Japan
Prior art keywords
fixed
electromagnetic coil
yoke
self
iron 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.)
Expired - Lifetime
Application number
JP60133211A
Other languages
Japanese (ja)
Other versions
JPS61290702A (en
Inventor
Shigeru Shirai
Yoshio Yamamoto
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 JP60133211A priority Critical patent/JPS61290702A/en
Publication of JPS61290702A publication Critical patent/JPS61290702A/en
Publication of JPH0328043B2 publication Critical patent/JPH0328043B2/ja
Granted 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、瞬時通電により作動する自己保持ソ
レノイドに関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a self-holding solenoid activated by instantaneous energization.

従来の技術 従来のこの種の自己保持ソレノイドは、第7図
に示すように、電磁コイル1の外側に固定継鉄2
を設け、前記電磁コイル1の内側に可動鉄心3を
摺動自在に設け、可動鉄心3が固定鉄心4に当接
した状態で吸着自己保持されるように永久磁石5
が固定継鉄2の内側の対称位置に対向固着させた
構成で、電磁コイル1に永久磁石5の磁束の向き
と逆方向の磁束が発生するように、瞬時電流を流
すと、永久磁石5が可動鉄心3を固定継鉄2に吸
着保持していた力が減少し、スプリング6の力で
可動鉄心3が固定鉄心2から離脱するようになつ
ていた。(例えば、実公昭59−23369号公報) 発明が解決しようとする問題点 しかしながら上記のような構成では、対向した
永久磁石5の磁束量が左右ほぼ同等なので、第7
図や第8図のように、可動鉄心3と固定鉄心4が
当接して吸着保持状態のとき、可動鉄心3が左右
の永久磁石5に引かれる力はほぼ同じとなり、可
動鉄心3が横方向へ傾斜する方向は一定しない。
したがつて可動鉄心3と固定鉄心4との当接箇所
も一定しない。可動鉄心3と固定鉄心4の当接箇
所つまり吸着面状態が一定しないことから、吸着
保持力が一定せず電磁コイル1に通電して可動鉄
心3が離脱作動する電流が都度変化しばらつくと
いう問題点を有していた。
BACKGROUND ART A conventional self-holding solenoid of this type has a fixed yoke 2 on the outside of an electromagnetic coil 1, as shown in FIG.
A movable core 3 is slidably provided inside the electromagnetic coil 1, and a permanent magnet 5 is installed so that the movable core 3 is self-adsorbed and held in a state in which it is in contact with the fixed core 4.
are fixed opposite to each other at symmetrical positions inside the fixed yoke 2, and when an instantaneous current is applied to the electromagnetic coil 1 so that a magnetic flux is generated in the opposite direction to the direction of the magnetic flux of the permanent magnet 5, the permanent magnet 5 The force holding the movable core 3 on the fixed yoke 2 decreased, and the force of the spring 6 caused the movable core 3 to separate from the fixed yoke 2. (For example, Japanese Utility Model Publication No. 59-23369) Problems to be Solved by the Invention However, in the above configuration, since the amount of magnetic flux of the opposing permanent magnets 5 is almost equal on the left and right sides, the seventh
As shown in the figure and FIG. 8, when the movable core 3 and the fixed core 4 are in contact with each other and are in an adsorbed and held state, the force with which the movable core 3 is attracted by the left and right permanent magnets 5 is almost the same, and the movable core 3 is pulled in the lateral direction. The direction of inclination is not constant.
Therefore, the contact points between the movable core 3 and the fixed core 4 are also not constant. The problem is that the contact point between the movable core 3 and the fixed core 4, that is, the state of the attraction surface, is not constant, so the attraction and holding force is not constant, and the current that flows through the electromagnetic coil 1 and causes the movable core 3 to separate varies each time. It had a point.

本発明はかかる従来の問題を解消するもので、
自己保持ソレノイドの吸着保持力を安定化し、作
動特性のばらつきを小さくすることを目的とす
る。
The present invention solves such conventional problems,
The purpose is to stabilize the suction and holding force of the self-holding solenoid and reduce variations in operating characteristics.

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に本発明の自己保持
ソレノイドは、電磁コイルと、前記電磁コイルの
外側の略対称形の固定継鉄と、前記電磁コイルの
内側を摺動自在に設けられた可動鉄心と、前記固
定継鉄の内面と前記可動鉄心の間にあつて略対称
位置に対向固着した磁力の異なる永久磁石とから
構成したもの、または、電磁コイルと前記電磁コ
イルの外側の略対称形の固定継鉄と、前記電磁コ
イルの内側を摺動自在に設けられた可動鉄心と、
前記固定継鉄の内面と前記可動鉄心の間の片側に
永久磁石を固着したという構成を備えたものであ
る。
Means for Solving the Problems In order to solve the above problems, the self-holding solenoid of the present invention includes an electromagnetic coil, a substantially symmetrical fixed yoke on the outside of the electromagnetic coil, and a sliding yoke on the inside of the electromagnetic coil. A movable iron core that is freely movable, and permanent magnets with different magnetic forces that are fixed oppositely in substantially symmetrical positions between the inner surface of the fixed yoke and the movable iron core, or an electromagnetic coil and the electromagnetic core. a substantially symmetrical fixed yoke outside the coil; a movable iron core slidably provided inside the electromagnetic coil;
A permanent magnet is fixed to one side between the inner surface of the fixed yoke and the movable iron core.

作 用 本発明は上記した構成によつて、可動鉄心が永
久磁石に引かれて傾斜する方向が一定し、可動鉄
心が当接する吸着箇所も安定するので、永久磁石
による吸着保持力も安定するため、作動特性のば
らつきが小さくなるのである。
Effects According to the present invention, with the above-described configuration, the direction in which the movable core is attracted by the permanent magnet and tilts is constant, and the attraction location where the movable core comes into contact is also stabilized, so that the attraction and holding force by the permanent magnet is also stabilized. This reduces the variation in operating characteristics.

実施例 以下、本発明の実施例を添付図面にもとづいて
説明する。
Embodiments Hereinafter, embodiments of the present invention will be described based on the accompanying drawings.

第1図、第2図において、1は電磁コイルで、
この電磁コイル1の外側に略対称形の固定継鉄2
が装着されている。さらに電磁コイル1の内側に
は可動鉄心3が挿入され摺動自在で、その可動鉄
心3の端面が当接するように、電磁コイル1の内
側でかつ固定継鉄2の内側に固定鉄心4が固着さ
れている。さらにまた固定継鉄2の内面と可動鉄
心3の間の片側に永久磁石5を固着してある。本
実施例では永久磁石5のS極を固定継鉄2の内壁
面に接着固定した。またスプリング6は可動鉄心
3が電磁コイル1から抜ける方向にスプリング反
力が作用するようにセツトした構成である。7は
黄銅板で作つたカシメ板である。
In Figures 1 and 2, 1 is an electromagnetic coil,
A substantially symmetrical fixed yoke 2 is placed on the outside of this electromagnetic coil 1.
is installed. Furthermore, a movable core 3 is inserted and slidable inside the electromagnetic coil 1, and a fixed core 4 is fixed inside the electromagnetic coil 1 and inside the fixed yoke 2 so that the end face of the movable core 3 comes into contact with the movable core 3. has been done. Furthermore, a permanent magnet 5 is fixed to one side between the inner surface of the fixed yoke 2 and the movable iron core 3. In this embodiment, the S pole of the permanent magnet 5 was adhesively fixed to the inner wall surface of the fixed yoke 2. Further, the spring 6 is configured so that a spring reaction force acts in the direction in which the movable iron core 3 is removed from the electromagnetic coil 1. 7 is a caulking plate made of brass plate.

上記構成において、可動鉄心3の端面が固定鉄
心4と当接した状態の場合、永久磁石5の磁束は
可動鉄心3から固定鉄心4を介し、さらに固定継
鉄2を通つて永久磁石4に入る。この時可動鉄心
3と電磁コイル1との間には、わずかではあるが
摺動するためのクリヤランスがあり、可動鉄心3
はそのクリヤランスの分だけガタついたり、傾斜
し得る訳であるが永久磁石5の方向に常に引つ張
られているため、固定鉄心4と当接する時の可動
鉄心3の吸着面当接位置は安定するように作用す
る。可動鉄心3が固定鉄心4に当接した状態で
は、前述した永久磁石5の磁束により、可動鉄心
3と固定鉄心4との間の磁気吸着力が、スプリン
グ6の反力よりも大きく、可動鉄心3は固定鉄心
4に吸着保持されている。そこで電磁コイル1に
永久磁石5の磁束と逆方向の磁束を生じる向きに
瞬時通電すると、可動鉄心3と固定鉄心4の吸着
面の永久磁石5による磁束を打ち消し減少させる
べく作用し、結果スプリング6の反力が吸着面磁
力に打ち勝つた時点で可動鉄心3は固定鉄心4か
ら離脱する。この可動鉄心3が離脱するコイル電
流(=離脱作動電流)は、自己保持ソレノイドを
機器に使用する場合、できるだけばらつかずに一
定していることが望ましい。ところが従来例のよ
うに可動鉄心3の吸着当接面が当接時一定せず不
安定だと、吸着面磁気空隙が吸着の繰返しによ
り、都度異なり吸引力は磁気空隙の二乗に逆比例
して変化し、結果、離脱電圧特性がばらついてし
まう。しかし本実施例のように永久磁石5が可動
鉄心3と固定継鉄2との内面片側だけに固着した
構成であると、前にも説明したように可動鉄心3
の吸着面磁気空隙が一定し、繰返し作動による離
脱電流特性のばらつきが小さく安定するという効
果がある。
In the above configuration, when the end face of the movable core 3 is in contact with the fixed core 4, the magnetic flux of the permanent magnet 5 passes from the movable core 3 through the fixed core 4, and further passes through the fixed yoke 2 to enter the permanent magnet 4. . At this time, there is a slight clearance between the movable core 3 and the electromagnetic coil 1 for sliding, and the movable core 3
Although it may wobble or tilt due to its clearance, it is always pulled in the direction of the permanent magnet 5, so when it comes into contact with the fixed core 4, the adsorption surface contact position of the movable core 3 is Acts to stabilize. When the movable core 3 is in contact with the fixed core 4, due to the magnetic flux of the permanent magnet 5 described above, the magnetic attraction force between the movable core 3 and the fixed core 4 is greater than the reaction force of the spring 6, and the movable core 3 is held by the fixed iron core 4 by suction. Therefore, when the electromagnetic coil 1 is momentarily energized in a direction that generates a magnetic flux in the opposite direction to the magnetic flux of the permanent magnet 5, it acts to cancel out and reduce the magnetic flux caused by the permanent magnet 5 on the attracting surfaces of the movable iron core 3 and the fixed iron core 4, and as a result, the spring 6 The movable core 3 separates from the fixed core 4 at the time when the reaction force overcomes the attraction surface magnetic force. When the self-holding solenoid is used in equipment, it is desirable that the coil current at which the movable core 3 is detached (=disengagement operating current) be constant with as little variation as possible. However, if the suction abutment surface of the movable iron core 3 is not constant and unstable during contact, as in the conventional example, the magnetic gap on the suction surface will vary each time due to repeated adsorption, and the attractive force will be inversely proportional to the square of the magnetic gap. As a result, the decoupling voltage characteristics vary. However, if the permanent magnet 5 is fixed to only one side of the inner surfaces of the movable core 3 and the fixed yoke 2 as in this embodiment, as described above, the movable core 5
This has the effect that the magnetic gap between the attracting surfaces is constant, and the dispersion of the detachment current characteristics due to repeated operation is small and stable.

次に本発明の他の実施例を第3図を用いて説明
する。第3図において前記実施例と相違する点は
固定継鉄2の内面と可動鉄心3の間の片側に固着
した永久磁石5と略対称位置に補助継鉄8を設け
てなる構成としたことにあり、この構成によれば
第1図、第2図の実施例と同じ理由により作動電
流特性のばらつきが小さいという効果に加えて、
電磁コイル1に通電して発生する磁束の磁路の磁
気抵抗が小さくなり、低電力で作動可能にならし
める効果がある。つまり永久磁石5の磁束と逆方
向の磁束を電磁コイル1に通電して発生すると、
その磁束は固定鉄心4から可動鉄心を通り、さら
に補助継鉄8を介して固定継鉄2から固定鉄心4
へと磁路が形成されており、永久磁石5よりも補
助継鉄8の方が、はるかに透磁率が高く、磁路の
磁気抵抗が減少し、小さいコイル電流で永久磁石
5の磁束を所定量打ち消すだけの電磁コイル1の
磁束が可動鉄心3と固定鉄心4との吸着面に生じ
るためである。
Next, another embodiment of the present invention will be described with reference to FIG. The difference in FIG. 3 from the previous embodiment is that an auxiliary yoke 8 is provided at a position approximately symmetrical to the permanent magnet 5 fixed to one side between the inner surface of the fixed yoke 2 and the movable iron core 3. According to this configuration, in addition to the effect that the variation in operating current characteristics is small for the same reason as the embodiments shown in FIGS. 1 and 2,
The magnetic resistance of the magnetic path of the magnetic flux generated by energizing the electromagnetic coil 1 is reduced, which has the effect of enabling operation with low power. In other words, when a magnetic flux in the opposite direction to the magnetic flux of the permanent magnet 5 is generated by energizing the electromagnetic coil 1,
The magnetic flux passes from the fixed iron core 4 to the movable iron core, and then from the fixed yoke 2 to the fixed iron core 4 via the auxiliary yoke 8.
The auxiliary yoke 8 has a much higher magnetic permeability than the permanent magnet 5, and the magnetic resistance of the magnetic path is reduced, making it possible to control the magnetic flux of the permanent magnet 5 with a small coil current. This is because the magnetic flux of the electromagnetic coil 1 which can be canceled out by a certain amount is generated on the attraction surface between the movable iron core 3 and the fixed iron core 4.

次に本発明のさらに他の実施例を第4図を用い
て説明する。第4図において前記実施例と相違す
る点は、永久磁石5と略対称位置に寸法のやや小
さい永久磁石5′を対向固着してなる構成とした
ことにあり、この構成によれば永久磁石5だけよ
りも永久磁石5′の分だけ余分に永久磁石の磁束
が増加し、より強力な吸着保持力が得られるとい
う効果がある。永久磁石5と永久磁石5′の寸法
が異なる分だけ可動鉄心3を横方向へ引きつける
磁力は左右異なつて作用し、前々記実施例と同様
に作動電流特性のばらつきは小さく安定する効果
があることは、もちろんである。この実施例で永
久磁石5と5′の寸法は同寸法として、永久磁石
特性の違う材質の磁石にした場合でも同様の効果
を得ることができる。
Next, still another embodiment of the present invention will be described using FIG. 4. The difference in FIG. 4 from the previous embodiment is that a permanent magnet 5', which is slightly smaller in size, is fixed opposite to the permanent magnet 5 at a position substantially symmetrical to the permanent magnet 5. The magnetic flux of the permanent magnet increases by an amount corresponding to the permanent magnet 5', and a stronger attraction and holding force can be obtained. To the extent that the dimensions of the permanent magnets 5 and 5' are different, the magnetic force that attracts the movable iron core 3 in the lateral direction acts differently on the left and right sides, and as in the previous embodiments, the variation in the operating current characteristics is small and stable. Of course. In this embodiment, even if the dimensions of the permanent magnets 5 and 5' are the same and the magnets are made of materials with different permanent magnet characteristics, the same effect can be obtained.

次にまたさらに本発明の他の実施例を第5図を
用いて説明する。第5図において前記実施例と相
違する点は、略対称位置に対向固着した一方の永
久磁石5′は、隣接した補助継鉄8′とからなる構
成としたことにあり、前記実施例同様に永久磁石
5,5′により、可動鉄心3と固定鉄心4の吸着
面に多くの永久磁石磁束が作用するため、強力な
吸着自己保持力が得られる効果が一つと、二つ目
に補助継鉄8′が電磁コイル1の磁束の通る磁路
の磁気空隙を小さくするように作用し、磁気抵抗
が小さくなり、低電力で可動鉄心3を離脱作動で
きる効果がある。さらに三つ目に左右の永久磁石
5,5′の磁力の差により、可動鉄心3を横方向
へ引つ張る磁力が片寄るため、可動鉄心3と固定
鉄心4の吸着面当接位置が安定し、作動電流特性
のばらつきが小さいという効果がある。
Next, another embodiment of the present invention will be described with reference to FIG. The difference in FIG. 5 from the previous embodiment is that one of the permanent magnets 5' which are opposed and fixed in substantially symmetrical positions is constituted by an adjacent auxiliary yoke 8', which is similar to the previous embodiment. Due to the permanent magnets 5 and 5', a large amount of permanent magnet magnetic flux acts on the adhesion surfaces of the movable iron core 3 and fixed iron core 4, so one effect is that a strong adsorption self-holding force can be obtained, and the second effect is that the auxiliary yoke 8' acts to reduce the magnetic gap in the magnetic path through which the magnetic flux of the electromagnetic coil 1 passes, reducing magnetic resistance and allowing the movable core 3 to be detached with low power. Third, due to the difference in magnetic force between the left and right permanent magnets 5 and 5', the magnetic force that pulls the movable core 3 in the lateral direction is biased, so the position where the movable core 3 and the fixed core 4 come into contact with the attraction surfaces becomes stable. , the effect is that the variation in operating current characteristics is small.

次にまたまたさらに本発明の他の実施例を第6
図を用いて説明する。第6図において前記実施例
と相違する点は、電磁コイル1の外側の略対称形
の固定継鉄2′は、略対称位置に対向固着した互
いに厚みの異なる永久磁石5,5′と密着してな
る構成としたことにあり、この構成によれば、前
記第5図実施例と同様に永久磁石5,5′により
可動鉄心3と固定鉄心4の吸着面に多くの永久磁
石磁束が作用するため、強力な吸着自己保持力が
得られる効果と、電磁コイル1の磁束が固定鉄心
4→可動鉄心3→永久磁石5′→固定継鉄2′→固
定鉄心4といつた磁路を通り、このうち透磁率の
低い永久磁石5′は厚みが薄いためこの部分の磁
気空隙が比較的小さく磁気抵抗が小さい分だけ電
磁コイル1に加える電力は小さい電力で、可動鉄
心は離脱できるという特有の効果がある。もちろ
ん本来の目的である作動電流特性のばらつきを小
さくする効果についても、左右の永久磁石5,
5′の磁力の差があるため、可動鉄心3を横方向
へ引張る磁力が片寄り、可動鉄心3と固定鉄心4
の吸着面当接位置が安定することにより達成でき
る。
Next, a sixth embodiment of the present invention will be described.
This will be explained using figures. The difference in FIG. 6 from the previous embodiment is that the substantially symmetrical fixed yoke 2' on the outside of the electromagnetic coil 1 is in close contact with permanent magnets 5, 5' of mutually different thickness, which are fixed oppositely in substantially symmetrical positions. According to this structure, a large amount of permanent magnet magnetic flux acts on the attracting surfaces of the movable iron core 3 and the fixed iron core 4 by the permanent magnets 5 and 5', similar to the embodiment shown in FIG. Therefore, a strong adsorption self-holding force is obtained, and the magnetic flux of the electromagnetic coil 1 passes through the magnetic path from fixed iron core 4 → movable iron core 3 → permanent magnet 5' → fixed yoke 2' → fixed iron core 4, Among these, the permanent magnet 5' with low magnetic permeability is thin, so the magnetic gap in this part is relatively small and the magnetic resistance is small, so the electric power applied to the electromagnetic coil 1 is small and the movable iron core can be detached. There is. Of course, regarding the original purpose of reducing variations in operating current characteristics, the left and right permanent magnets 5,
Because of the difference in magnetic force of
This can be achieved by stabilizing the contact position of the suction surface.

発明の効果 以上のように本発明の自己保持ソレノイドによ
れば、次の効果が得られる。
Effects of the Invention As described above, the self-holding solenoid of the present invention provides the following effects.

(1) 電磁コイルと、前記電磁コイルの外側の略対
称形の固定継鉄と、前記電磁コイルの内側を摺
動自在に設けられた可動鉄心と、前記固定継鉄
の内面と前記可動鉄心の間にあつて略対称位置
に対向固着した磁力の異なる永久磁石とから構
成したもの、または電磁コイルと前記電磁コイ
ルの外側の略対称形の固定継鉄と、前記電磁コ
イルの内側を摺動自在に設けられた可動鉄心
と、前記固定継鉄の内面と前記可動鉄心の間の
片側に永久磁石を固着したという構成としてい
るので、自己保持ソレノイドの作動特性のばら
つきが小さいという効果がある。
(1) An electromagnetic coil, a substantially symmetrical fixed yoke on the outside of the electromagnetic coil, a movable core that is slidably provided inside the electromagnetic coil, an inner surface of the fixed yoke, and the movable core. An electromagnetic coil, a substantially symmetrical fixed yoke on the outside of the electromagnetic coil, and a fixed yoke that can freely slide on the inside of the electromagnetic coil. Since the structure includes a movable iron core provided in the fixed yoke and a permanent magnet fixed to one side between the inner surface of the fixed yoke and the movable iron core, there is an effect that variations in the operating characteristics of the self-holding solenoid are small.

(2) 略対称形の固定継鉄の内側の片側のみまたは
略対称位置に厚みの異なる永久磁石を固着した
構成であるから、電磁コイルの磁路の磁気抵抗
が小さくできるため、低電力で作動ができると
いう特有の効果がある。
(2) Since it has a structure in which permanent magnets of different thicknesses are fixed to only one side of the substantially symmetrical fixed yoke or in substantially symmetrical positions, the magnetic resistance of the magnetic path of the electromagnetic coil can be reduced, so it can operate with low power. It has the unique effect of being able to

(3) 上記の効果により、電池駆動など電力の限ら
れた電源で長期間安定して使用できる効果があ
る。
(3) Due to the above effects, it is possible to use the device stably for a long period of time using a power source with limited power such as battery drive.

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

第1図は本発明の第1の実施例における自己保
持ソレノイドの斜視図、第2図は自己保持ソレノ
イドの正面断面図、第3図、第4図、第5図、第
6図は本発明の第2の実施例における自己保持ソ
レノイドの正面断面図、第7図、第8図は従来の
自己保持ソレノイドの正面断面図である。 1……電磁コイル、2,2′……固定継鉄、3
……可動鉄心、5,5′……永久磁石、8,8′…
…補助継鉄。
FIG. 1 is a perspective view of a self-holding solenoid according to a first embodiment of the present invention, FIG. 2 is a front sectional view of the self-holding solenoid, and FIGS. 3, 4, 5, and 6 are according to the present invention. 7 and 8 are front sectional views of a conventional self-holding solenoid in the second embodiment. 1... Electromagnetic coil, 2, 2'... Fixed yoke, 3
...Movable iron core, 5,5'...Permanent magnet, 8,8'...
...Auxiliary yoke.

Claims (1)

【特許請求の範囲】 1 電磁コイルと、前記電磁コイルの外側の略対
称形の固定継鉄と、前記電磁コイルの内側を摺動
自在に設けられた可動鉄心と、前記固定継鉄の内
面と可動鉄心の間にあつて略対称位置に対向固着
した磁力の異なる永久磁石とからなる自己保持型
ソレノイド。 2 略対称位置に対向固着した永久磁石は、互い
に寸法の異なる永久磁石で構成された特許請求の
範囲第1項記載の自己保持型ソレノイド。 3 略対称位置に対向固着した永久磁石は、互い
に材質の異なる永久磁石で構成された特請求の範
囲第1項記載の自己保持型ソレノイド。 4 略対称位置に対向固着した一方の永久磁石
は、隣接した補助継鉄とから構成された特許請求
の範囲第1項記載の自己保持型ソレノイド。 5 電磁コイルの外側の略対称形の固定継鉄は、
略対称位置に対向固着した互いに厚みの異なる永
久磁石と密着して構成された特許請求の範囲第1
項記載の自己保持型ソレノイド。 6 電磁コイルと、前記電磁コイルの外側の略対
称形の固定継鉄と、前記電磁コイルの内側を摺動
自在に設けられた可動鉄心と、前記固定継鉄の内
面と前記可動鉄心の間の片側に固着した永久磁石
とからなる自己保持型ソレノイド。 7 固定継鉄の内面と可動鉄心の間の片側に固着
した永久磁石と略対称位置に補助継鉄を設けてな
る特許請求の範囲第6項記載の自己保持型ソレノ
イド。
[Scope of Claims] 1. An electromagnetic coil, a substantially symmetrical fixed yoke outside the electromagnetic coil, a movable iron core slidably provided inside the electromagnetic coil, and an inner surface of the fixed yoke. A self-holding solenoid consisting of permanent magnets with different magnetic forces that are fixed in opposing positions in substantially symmetrical positions between a movable iron core. 2. The self-holding solenoid according to claim 1, wherein the permanent magnets fixed opposite each other in substantially symmetrical positions are composed of permanent magnets having different dimensions. 3. The self-holding solenoid according to claim 1, wherein the permanent magnets fixed oppositely in substantially symmetrical positions are made of permanent magnets of different materials. 4. The self-holding solenoid according to claim 1, wherein one of the permanent magnets that are opposed and fixed in substantially symmetrical positions is constituted by an adjacent auxiliary yoke. 5 The approximately symmetrical fixed yoke outside the electromagnetic coil is
Claim 1, which is configured in close contact with permanent magnets having mutually different thicknesses and fixed oppositely in substantially symmetrical positions.
Self-retaining solenoid as described in section. 6. An electromagnetic coil, a substantially symmetrical fixed yoke on the outside of the electromagnetic coil, a movable iron core that is slidably provided inside the electromagnetic coil, and a space between the inner surface of the fixed yoke and the movable iron core. A self-holding solenoid consisting of a permanent magnet fixed to one side. 7. A self-holding solenoid according to claim 6, wherein an auxiliary yoke is provided at a position substantially symmetrical to a permanent magnet fixed to one side between the inner surface of the fixed yoke and the movable iron core.
JP60133211A 1985-06-19 1985-06-19 self-holding solenoid Granted JPS61290702A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60133211A JPS61290702A (en) 1985-06-19 1985-06-19 self-holding solenoid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60133211A JPS61290702A (en) 1985-06-19 1985-06-19 self-holding solenoid

Publications (2)

Publication Number Publication Date
JPS61290702A JPS61290702A (en) 1986-12-20
JPH0328043B2 true JPH0328043B2 (en) 1991-04-17

Family

ID=15099323

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60133211A Granted JPS61290702A (en) 1985-06-19 1985-06-19 self-holding solenoid

Country Status (1)

Country Link
JP (1) JPS61290702A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106158233B (en) * 2016-08-31 2018-02-27 昆山国力源通新能源科技有限公司 Magnetic keeps magnetic structure

Also Published As

Publication number Publication date
JPS61290702A (en) 1986-12-20

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