JPH0113373Y2 - - Google Patents

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Publication number
JPH0113373Y2
JPH0113373Y2 JP1982064695U JP6469582U JPH0113373Y2 JP H0113373 Y2 JPH0113373 Y2 JP H0113373Y2 JP 1982064695 U JP1982064695 U JP 1982064695U JP 6469582 U JP6469582 U JP 6469582U JP H0113373 Y2 JPH0113373 Y2 JP H0113373Y2
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JP
Japan
Prior art keywords
armature
permanent magnet
bypass member
yokes
yoke
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
Application number
JP1982064695U
Other languages
Japanese (ja)
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JPS58168105U (en
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Priority to JP6469582U priority Critical patent/JPS58168105U/en
Publication of JPS58168105U publication Critical patent/JPS58168105U/en
Application granted granted Critical
Publication of JPH0113373Y2 publication Critical patent/JPH0113373Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は、電磁石装置、詳しくは、平生は永久
磁石の磁力によりヨークの吸着面にアーマチユア
を吸着して保持し、励磁用コイルに通電すること
によつて吸着面におけるアーマチユアの吸着力が
打ち消されてアーマチユアが吸着面より離間動作
する、いわゆる釈放型の電磁石装置に関する。
[Detailed description of the invention] The present invention is an electromagnetic device, more specifically, an armature is attracted and held on the attraction surface of a yoke by the magnetic force of a permanent magnet, and the armature is held on the attraction surface by energizing an excitation coil. The present invention relates to a so-called release type electromagnetic device in which the armature's attraction force is canceled and the armature moves away from the attraction surface.

一般に、釈放型の電磁石装置は第1図に示すよ
うに構成されている。即ち、1対のヨーク1,2
間には、その後端近傍で永久磁石3が挟持されて
いると共にこのヨーク1,2の後端面および上記
永久磁石3に接して例えば鉄板等の強磁性体から
なるバイパス部材4が側磁路を形成するように設
けられており、また一方のヨーク1には通電時に
永久磁石3より発生した磁束を打ち消すように励
磁されるようにコイル5が嵌装されている。上記
1対のヨーク1,2の先端面1a,2aはアーマ
チユア6を吸着するための吸着面となつていて、
同吸着面1a,2aは高い吸着力を得るために高
い面精度で加工されている。
Generally, a release type electromagnet device is constructed as shown in FIG. That is, a pair of yokes 1 and 2
A permanent magnet 3 is sandwiched between the yokes 1 and 2 near their rear ends, and a bypass member 4 made of a ferromagnetic material such as an iron plate is in contact with the rear end surfaces of the yokes 1 and 2 and the permanent magnet 3. A coil 5 is fitted in one yoke 1 so as to be excited so as to cancel out the magnetic flux generated by the permanent magnet 3 when energized. The tip surfaces 1a and 2a of the pair of yokes 1 and 2 serve as suction surfaces for suctioning the armature 6,
The suction surfaces 1a and 2a are machined with high surface precision in order to obtain high suction force.

一方、このヨーク1,2の吸着面1a,2aと
対向する位置にはアーマチユア6が配設されてお
り、同アーマチユア6はアーマチユア支持レバー
7の一端部にカシメ付け等によつて固設されたア
ーマチユア支持軸8に同アーマチユア6の支持孔
6aを嵌入させることによつて同支持軸8に回転
自在に配設されている。アーマチユア支持軸8の
上部には周溝8aが形成されており、同周溝8a
にEリングを嵌合させることによつてアマチユア
6の抜け落ちが防止されている。また、アーマチ
ユア支持レバー7の上記支持軸8の近傍には、ア
ーマチユア6の回転位置を規制するためのストツ
パー部7a,7bが形成されている。アーマチユ
ア支持レバー7の回動中心となる位置にはあおり
ガタを防止するため同支持レバー7の面と垂直な
方向に比較的長く形成された円筒形状の軸受部1
0が固設されており同軸受部10に図示しない固
定軸が嵌合されることによりアーマチユア支持レ
バー7は同固定軸を中心に回動自在になつてい
る。さらに、このアーマチユア支持レバー7は不
動部材との間にばね11が張設されていて、同ば
ね11の付勢力により時計方向の回動習性を与え
られている。このように構成された電磁石装置に
おいてはアーマチユア支持レバー7が図示しない
リセツト部材によつて上記ばね11による回動習
性に抗して反時計方向に回動させられることによ
り、アーマチユア6がヨーク1,2の吸着面1
a,2aに当接すると、永久磁石3の磁力により
吸着面1a,2aにアーマチユア6が吸着され、
同吸着力は上記ばね11の付勢力よりも大きいの
で、平生は、同吸着状態が保持されることにな
る。そして、この吸着状態において、上記励磁用
コイル5に通電が行なわれると、同コイル5の通
電によつて発生する磁束により、アーマチユア6
を吸着するためのヨーク1,2中の磁束が減少
し、このため、上記ばね11の付勢力によつてア
ーマチユア支持レバー7が時計方向に回動してア
ーマチユア6がヨーク1,2の吸着面1a,2a
より離間する。
On the other hand, an armature 6 is disposed at a position facing the suction surfaces 1a and 2a of the yokes 1 and 2, and the armature 6 is fixed to one end of the armature support lever 7 by caulking or the like. It is rotatably disposed on the armature support shaft 8 by fitting the support hole 6a of the armature 6 into the armature support shaft 8. A circumferential groove 8a is formed in the upper part of the armature support shaft 8.
By fitting the E-ring into the armature 6, the armature 6 is prevented from falling off. Further, stopper portions 7a and 7b for regulating the rotational position of the armature 6 are formed near the support shaft 8 of the armature support lever 7. At the center of rotation of the armature support lever 7, a cylindrical bearing portion 1 is formed to be relatively long in a direction perpendicular to the surface of the armature support lever 7 in order to prevent tilting and backlash.
A fixed shaft (not shown) is fitted into the bearing portion 10, so that the armature support lever 7 is rotatable about the fixed shaft. Furthermore, a spring 11 is stretched between the armature support lever 7 and an immovable member, and the biasing force of the spring 11 gives it the ability to rotate clockwise. In the electromagnet device constructed in this way, the armature support lever 7 is rotated counterclockwise by a reset member (not shown) against the rotational behavior of the spring 11, so that the armature 6 is rotated so that the yoke 1, 2 suction surface 1
When it comes into contact with a, 2a, the armature 6 is attracted to the attraction surfaces 1a, 2a by the magnetic force of the permanent magnet 3,
Since the suction force is larger than the biasing force of the spring 11, the suction state will be maintained for a lifetime. In this attracted state, when the excitation coil 5 is energized, the armature 6 is caused by the magnetic flux generated by the energization of the coil 5.
The magnetic flux in the yokes 1 and 2 for attracting the yokes 1 and 2 decreases, and as a result, the armature support lever 7 rotates clockwise due to the biasing force of the spring 11, and the armature 6 moves onto the attracting surfaces of the yokes 1 and 2. 1a, 2a
be further apart.

上記の釈放型電磁石装置において、上記コイル
5が通電されない状態のときと通電状態にあると
きとでのヨーク1,2を通過する磁束の変化につ
いて第2図A,Bによつて説明すると、永久磁石
3およびヨーク1,2を通過する磁束は2分され
ており、永久磁石3のN極>ヨーク1→アーマチ
ユア6→ヨーク2→永久磁石3のS極を通る磁束
により磁気回路12が形成され、永久磁石3のN
極→ヨーク1→バイパス部材4→ヨーク2→永久
磁石3のS極を通る磁束により磁気回路13が形
成されている。ヨーク1,2およびアーマチユア
6はパーマロイ等の高透磁率部材により形成さ
れ、バイパス部材4はヨーク1,2やアーマチユ
ア6の材料よりも磁気抵抗の高い、鉄板等の強磁
性体が形成されているので、コイル5に通電する
以前は、磁気回路12の方が磁気回路13よりも
磁気抵抗が低く、このため、永久磁石3より発し
た磁束は、第2図Aに実線と破線で示すように、
磁気回路12の方を磁気回路13よりも多く通
り、従つて、ヨーク1,2の吸着面1a,2aに
アーマチユア6が高い吸着力で吸着し保持され
る。コイル5が通電状態になると、コイル5には
永久磁石3が発生する磁束と逆向きの磁束が発生
するので、このとき上記磁気回路12の磁気抵抗
が磁気回路13の磁気抵抗よりも増大する。この
ため、第2図Bに示すように、アーマチユア6を
通る磁気回路12の磁束は減少し、バイパス部材
4を通る磁気回路13の磁束は増加するので、ヨ
ーク1,2の吸着面1a,2aにおけるアーマチ
ユア6の吸着力が減少し、アーマチユア6の吸着
状態が解除される。
In the release type electromagnet device described above, the change in the magnetic flux passing through the yokes 1 and 2 between when the coil 5 is not energized and when it is energized is explained using FIGS. 2A and B. The magnetic flux passing through the magnet 3 and yokes 1 and 2 is divided into two parts, and a magnetic circuit 12 is formed by the magnetic flux passing through the N pole of permanent magnet 3 > yoke 1 → armature 6 → yoke 2 → S pole of permanent magnet 3. , N of permanent magnet 3
A magnetic circuit 13 is formed by magnetic flux passing through the S pole of the pole → yoke 1 → bypass member 4 → yoke 2 → permanent magnet 3. The yokes 1 and 2 and the armature 6 are made of a high magnetic permeability material such as permalloy, and the bypass member 4 is made of a ferromagnetic material such as an iron plate that has higher magnetic resistance than the material of the yokes 1 and 2 and the armature 6. Therefore, before the coil 5 is energized, the magnetic resistance of the magnetic circuit 12 is lower than that of the magnetic circuit 13, and therefore, the magnetic flux emitted from the permanent magnet 3 is as shown by the solid line and broken line in FIG. 2A. ,
The magnetic circuit 12 passes through the magnetic circuit 13 more than the magnetic circuit 13, and therefore the armature 6 is attracted and held by the attraction surfaces 1a and 2a of the yokes 1 and 2 with a high attraction force. When the coil 5 is energized, a magnetic flux in the opposite direction to the magnetic flux generated by the permanent magnet 3 is generated in the coil 5, so that the magnetic resistance of the magnetic circuit 12 is greater than that of the magnetic circuit 13 at this time. Therefore, as shown in FIG. 2B, the magnetic flux of the magnetic circuit 12 passing through the armature 6 decreases, and the magnetic flux of the magnetic circuit 13 passing through the bypass member 4 increases. The adsorption force of the armature 6 decreases, and the adsorption state of the armature 6 is released.

ここで、特にカメラ用の釈放型電磁石装置にお
いては、アーマチユア6を高い吸着力で保持する
と共に、コイル5の通電時にはできるだけ少ない
消費電力で上記吸着力を大きく減少させるように
し、同時に、電磁石装置の全体を小型化すること
が高い信頼性を得るために重要である。コイル5
の通電時に上記吸着力を大きく減少させるものと
して、上記バイパス部材4の果す役割は大きく、
電磁気学における磁束の式、Φ=μo×μe×F×
A/(Φ;磁束、μe;比透磁率、μo;真空中
の透磁率、F;起磁力、A;断面積、;磁気回
路の長さ)からも、コイル5で発生する磁束は上
記バイパス部材4を含む磁気回路13の透磁率に
比例することが明らかである。即ち、上記コイル
5の通電時のヨークの吸着力を大きく減少させる
には磁気回路13(以下側磁路という)の磁気抵
抗を減少させればよいが、一方で高い吸着力を得
ようとすると、第2図Aに示したように、アーマ
チユア6を通る磁気回路12に十分な磁束を流す
必要があるので磁気抵抗を不用意に減少させるこ
とはできない。しかも、コイル5に通電したとき
には、上記のようにバイパス部材4を通過する磁
束が増加するので、この増加した磁束で側磁路は
磁気飽和しないだけの余裕が必要となる。
In particular, in a release-type electromagnet device for a camera, the armature 6 is held with a high attraction force, and when the coil 5 is energized, the above-mentioned attraction force is greatly reduced with as little power consumption as possible, and at the same time, the electromagnet device is Miniaturizing the entire device is important for achieving high reliability. coil 5
The bypass member 4 plays a large role in greatly reducing the adsorption force when energized.
Formula for magnetic flux in electromagnetism, Φ=μo×μe×F×
From A/(Φ: magnetic flux, μe: relative magnetic permeability, μo: magnetic permeability in vacuum, F: magnetomotive force, A: cross-sectional area, ; length of magnetic circuit), the magnetic flux generated in the coil 5 is bypassed. It is clear that it is proportional to the magnetic permeability of the magnetic circuit 13 containing the member 4. That is, in order to greatly reduce the attraction force of the yoke when the coil 5 is energized, it is sufficient to reduce the magnetic resistance of the magnetic circuit 13 (hereinafter referred to as the side magnetic path), but on the other hand, if you try to obtain a high attraction force, As shown in FIG. 2A, since sufficient magnetic flux must flow through the magnetic circuit 12 passing through the armature 6, the magnetic resistance cannot be reduced inadvertently. Moreover, when the coil 5 is energized, the magnetic flux passing through the bypass member 4 increases as described above, so that the side magnetic path must have enough margin to prevent magnetic saturation with this increased magnetic flux.

以上の理由から、高い吸着力を得ると共に、コ
イル5の通電時に吸着力を大きく減少させようと
すると、強い永久磁石を用いると共にバイパス部
材4を大きくしなければならないが、バイパス部
材4の占める体積はカメラ内部のスペース上無視
できないものであるので、この側磁路を形成する
ためのバイパス部材4はできる限り小さいことが
望ましい。そこで、従来は、第3,4図に示すよ
うに、プレス加工の容易な1mm〜0.4mm程度の厚
みを持つ鉄板等の強磁性体からなるバイパス部材
14a,14b,14cを磁気飽和しないだけの
断面積が得られるように必要とする枚数を重ね
て、永久磁石3および同磁石を挟んだヨーク1,
2の上側面或いは下側面に当接させた状態で側磁
路が形成されるように接着させていた。しかし、
このようにバイパス部材14a,14b,14c
を接着させるようにしたものにおいては、例えば
第5図に拡大して示すように、ヨーク1,2や永
久磁石3の寸法精度および接着等のずれによつて
エアギヤツプ15a,15bを生じてバイパス部
材14a,14bの密着が不完全になり、側磁路
としての磁気抵抗が極端に増大するだけでなく、
そのばらつきも大きくなるという欠点があつた。
また、バイパス部材14bの比透磁率はエアギヤ
ツプ15bによつてできる磁気抵抗によつて減少
し、バイパス部材14bと14cとの間にわずか
なエアギヤツプ15cが存在する場合には、さら
にバイパス部材14cの比透磁率を低下させてし
まう。このようにしてバイパス部材14cが、も
はや側磁路としての役割をほとんど果さないとい
う結果になつてしまつた場合はさらにバイパス部
材14dを設けても全く無意味になる。
For the above reasons, in order to obtain a high attraction force and to greatly reduce the attraction force when the coil 5 is energized, a strong permanent magnet must be used and the bypass member 4 must be made large, but the volume occupied by the bypass member 4 is Since this cannot be ignored due to the space inside the camera, it is desirable that the bypass member 4 for forming this side magnetic path is as small as possible. Therefore, conventionally, as shown in Figs. 3 and 4, bypass members 14a, 14b, 14c made of a ferromagnetic material such as an iron plate with a thickness of about 1 mm to 0.4 mm, which is easy to press, are made of a material that does not become magnetically saturated. A permanent magnet 3 and a yoke 1 sandwiching the magnet are stacked as many as necessary to obtain the cross-sectional area.
It was bonded so that a side magnetic path was formed when it was brought into contact with the upper or lower surface of 2. but,
In this way, the bypass members 14a, 14b, 14c
For example, as shown in an enlarged view in FIG. 5, air gaps 15a and 15b are formed due to deviations in the dimensional accuracy and adhesion of the yokes 1 and 2 and the permanent magnet 3, and the bypass member is The close contact between 14a and 14b becomes incomplete, and the magnetic resistance as a side magnetic path not only increases extremely, but also
The disadvantage is that the variation becomes large.
Further, the relative magnetic permeability of the bypass member 14b is reduced by the magnetic resistance created by the air gap 15b, and when a slight air gap 15c exists between the bypass members 14b and 14c, the relative magnetic permeability of the bypass member 14c is further reduced. This will reduce magnetic permeability. In this way, if the bypass member 14c no longer plays a role as a side magnetic path, it becomes completely meaningless to further provide the bypass member 14d.

本考案の目的は、上記事情に鑑み、上記ヨーク
の永久磁石を保持した部分に、枠体形状のバイパ
ス部材を嵌装させることにより、低電力で駆動で
き、小型で大きな吸着力を得ることができると共
に、生産性を高くし、低コスト化を計ることがで
きる電磁石装置を提供することにある。
In view of the above circumstances, the purpose of the present invention is to fit a frame-shaped bypass member into the part of the yoke that holds the permanent magnet, so that it can be driven with low power and can obtain a large attraction force with a small size. It is an object of the present invention to provide an electromagnet device that can increase productivity and reduce costs.

以下、本考案を図示の実施例によつて説明す
る。
Hereinafter, the present invention will be explained with reference to illustrated embodiments.

第6図は、本考案の一実施例を示す電磁石装置
の組立斜視図である。この電磁石装置は永久磁石
3を挟持したヨーク1,2の後端部20に、前記
従来のバイパス部材4の代りに、強磁性体によつ
て一体に形成されてなる箱型枠体のバイパス部材
21が装着されるようにしたものである。その他
の、アーマチユア6を回動自在に支持してなるア
ーマチユア支持レバー等の構成は第1図に示すも
のと同様であるので図示を省略する。即ち、直方
体形状に形成された箱型枠体のバイパス部材21
は内部に直方体形状の空間部22を有しており、
その前面の開口部22aは、上記ヨーク1,2の
後端部20が上記空間部22に比較的容易に嵌挿
されるように上記永久磁石3を挟持したヨーク
1,2の後端面20aよりも僅かに広く形成され
ている。
FIG. 6 is an assembled perspective view of an electromagnet device showing an embodiment of the present invention. This electromagnet device has a box-shaped frame body bypass member integrally formed with a ferromagnetic material in place of the conventional bypass member 4 at the rear end portion 20 of the yokes 1 and 2 that sandwich the permanent magnet 3. 21 is attached. The other structures, such as the armature support lever that rotatably supports the armature 6, are the same as those shown in FIG. 1, and are therefore not shown. That is, the bypass member 21 is a box-shaped frame body formed in the shape of a rectangular parallelepiped.
has a rectangular parallelepiped-shaped space 22 inside,
The front opening 22a is larger than the rear end surface 20a of the yokes 1, 2 that sandwich the permanent magnet 3 so that the rear end 20 of the yokes 1, 2 can be inserted into the space 22 relatively easily. It is slightly wider.

一方、このバイパス部材21が装着される上記
ヨーク1,2の後端部20においては、ヨーク
1,2と永久磁石3とは接着剤により固着されて
いるものであるが、この固着に際してヨーク1,
2および永久磁石3の下面20bを面精度の高い
基準面に当て付けながら固着するか、或いは、固
着後に上記下面20bを研摩するなどして、ヨー
ク1,2と永久磁石3の固着後における下面20
bを、高精度に平担な面に仕上げている。
On the other hand, in the rear end portions 20 of the yokes 1 and 2 to which the bypass member 21 is attached, the yokes 1 and 2 and the permanent magnet 3 are fixed with an adhesive. ,
The lower surfaces 20b of the yokes 1, 2 and the permanent magnets 3 are fixed by pressing them against a reference surface with high surface accuracy, or by polishing the lower surfaces 20b after the fixing. 20
b is finished to a flat surface with high precision.

このあと、上記ヨーク1,2の後端部20は、
第7図に示すように、上記バイパス部材21の開
口部22aより空間部に、上記後端面20aがバ
イパス部材21の内部後端面21aに衝合する位
置まで嵌合挿入され、同状態で上記後端部20と
バイパス部材21とが接着剤等により固着され
る。従つて、ヨーク1,2および永久磁石3は少
なくともその下面において平面性が高いため、極
めて僅かのエアギヤツプ或いは接着剤層を介して
バイパス部材21の内部下面21bに密着するこ
とになる。また、上記ヨーク1,2の後端面20
aをも高精度に研摩加工しておけば、この後端面
20aでもバイパス部材21の内部後端面21a
に密着されるものとなる。こうして、上記ヨーク
1,2の後端部20がバイパス部材21に密着し
て一体化されると、これによつて、バイパス部材
21の上記後端部20に密着した部分は全て側磁
路としての役割を果たすことになる。従つて、こ
の箱型枠体のバイパス部材21は永久磁石3およ
びヨーク1,2の後端部20を囲繞した状態で装
着されることにより、従来の板状のバイパス部材
に較べて密着性が高くかつ均一であり、部品精度
等のばらつきの影響を受けにくいものとなつてお
り、小型で効率よく側磁路が形成されることにな
る。
After this, the rear end portions 20 of the yokes 1 and 2 are
As shown in FIG. 7, the bypass member 21 is fitted and inserted into the space through the opening 22a until the rear end surface 20a abuts the inner rear end surface 21a of the bypass member 21, and in the same state, the rear end surface 20a abuts the inner rear end surface 21a of the bypass member 21. The end portion 20 and the bypass member 21 are fixed with adhesive or the like. Therefore, since the yokes 1, 2 and the permanent magnet 3 have high flatness at least on their lower surfaces, they come into close contact with the inner lower surface 21b of the bypass member 21 with an extremely small air gap or adhesive layer interposed therebetween. Further, the rear end surface 20 of the yokes 1 and 2
If a is also polished with high precision, this rear end surface 20a will also have the internal rear end surface 21a of the bypass member 21.
It will be closely followed. In this way, when the rear end portions 20 of the yokes 1 and 2 are closely integrated with the bypass member 21, the entire portion of the bypass member 21 that is in close contact with the rear end portion 20 serves as a side magnetic path. will play the role of Therefore, this box-shaped frame bypass member 21 is attached to surround the permanent magnet 3 and the rear end portions 20 of the yokes 1 and 2, so that it has better adhesion than a conventional plate-shaped bypass member. It is high and uniform, and is not easily affected by variations in component accuracy, etc., and the side magnetic path can be formed efficiently in a small size.

第8図はこの考案の他の実施例を示す組立斜視
図である。すなわち、絞り加工等によつて箱型に
成形された強磁性体からなるバイパス部材23
は、内部に直方体形状の空間部24を有してお
り、前面に開口部24aが形成されている。そし
て、この開口部24aから空間部24にヨーク2
5,26および永久磁石27が、それぞれ単体
で、永久磁石27がヨーク25,26で挟まれた
形で嵌入される。その後、第9図AおよびBの組
立後の斜視図および断面図に矢印で示すように、
箱型のバイパス部材23に対して、開口部24a
を有する面以外の他の5つの面の方向から機械的
に高い圧縮力を加えることにより、箱形バイパス
部材23は、ヨーク25,26および永久磁石2
7の表面形状にならつて、カシメ固定される。
FIG. 8 is an assembled perspective view showing another embodiment of this invention. In other words, the bypass member 23 is made of a ferromagnetic material formed into a box shape by drawing or the like.
has a rectangular parallelepiped-shaped space 24 inside, and an opening 24a formed in the front surface. Then, the yoke 2 is inserted into the space 24 from this opening 24a.
5 and 26 and the permanent magnet 27 are each inserted individually, with the permanent magnet 27 sandwiched between the yokes 25 and 26. Thereafter, as shown by arrows in the assembled perspective view and cross-sectional view of FIGS. 9A and 9B,
Opening 24a for box-shaped bypass member 23
By mechanically applying a high compressive force from the direction of the other five surfaces other than the surface having , the box-shaped bypass member 23 is
It is caulked and fixed according to the surface shape of 7.

このようにして固着されたヨーク25,26お
よび永久磁石27は、バイパス部材23との各圧
縮面において略完全に密着した状態が得られる。
したがつて、従来の板状のバイパス部材に較べて
密着性が高く均一であり、小型で効率よい側磁路
が形成されることになる。さらに、この実施例の
場合、前記実施例で必要とされたヨーク、永久磁
石およびバイパス部材の接着や溶接等を省略する
ことができると共に、ヨーク、永久磁石、および
バイパス部材のそれ程高い部品精度を必要とする
ことがない。また、従来人手にたよつていた作業
を機械的に自動組立することも可能であり、装置
のバラツキを少なくすることができ、低コスト化
を計ることができる。
The yokes 25, 26 and the permanent magnet 27 fixed in this manner are in substantially complete contact with the bypass member 23 on each compression surface.
Therefore, compared to the conventional plate-shaped bypass member, the adhesion is higher and more uniform, and a smaller and more efficient side magnetic path is formed. Furthermore, in the case of this embodiment, the gluing, welding, etc. of the yoke, permanent magnet, and bypass member, which were required in the previous embodiment, can be omitted, and the precision of the parts of the yoke, permanent magnet, and bypass member can be increased accordingly. never need it. Further, it is also possible to automatically assemble the device mechanically, which previously required manual assembly, and it is possible to reduce variations in the device and reduce costs.

なお、上記2つの実施例の場合、第10図Aに
示すように枠体形状のバイパス部材として、一面
に開口部28aを有し、他面に後端面28bを有
した箱型形状のものを示してきたが、第10図B
に示すように、両端が開口した直方体形状の貫通
孔29を有する筒型形状のものにしてもよいこと
はもちろんである。
In the case of the above two embodiments, as shown in FIG. 10A, a box-shaped bypass member having an opening 28a on one side and a rear end surface 28b on the other side is used as the frame-shaped bypass member. As shown in Figure 10B
As shown in FIG. 2, it is of course possible to use a cylindrical shape having a rectangular parallelepiped-shaped through hole 29 with both ends open.

以上述べたように、本考案によれば、ヨークの
永久磁石を保持した部分に、枠体形状のバイパス
部材を嵌装させることにより、バイパス部材と、
ヨークおよび永久磁石との密着性が高められ、バ
イパス効率が良好となり小型で大きな吸着力が得
られると共に、生産性を高め、低コスト化を計る
ことができる電磁石装置を提供することができ
る。
As described above, according to the present invention, by fitting the frame-shaped bypass member into the part of the yoke that holds the permanent magnet, the bypass member and
It is possible to provide an electromagnet device in which the adhesion between the yoke and the permanent magnet is improved, the bypass efficiency is improved, and a large attraction force is obtained with a small size, and productivity can be increased and costs can be reduced.

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

第1図は、従来の電磁石装置の一例を示す組立
斜視図、第2図A,Bは、上記第1図に示す電磁
石装置の励磁用コイルの非通電状態と通電状態と
をそれぞれ説明する平面図、第3図は、上記第1
図に示す電磁石装置に補助バイパス部材を設けた
電磁石装置の側面図、第4図は、上記第3図に示
す電磁石装置の−線に沿う背面図、第5図
は、上記第4図を拡大した、従来の電磁石装置の
不具合を説明する背面図、第6図は、本考案の一
実施例を示す電磁石装置の組立斜視図、第7図は
上記第6図に示す電磁石装置の要部断面図、第8
図は本考案の他の実施例を示す組立斜視図、第9
図Aは第8図の実施例の組立例の組立後の斜視
図、第9図Bは第9図Aにおけるバイパス部材で
囲繞された部分の断面図、第10図A,Bは本考
案のバイパス部材の形状を説明するための断面図
である。 1,2,25,26……ヨーク、3,27……
永久磁石、4,21,23……バイパス部材、5
……励磁用コイル、6……アーマチユア。
FIG. 1 is an assembled perspective view showing an example of a conventional electromagnet device, and FIGS. 2A and 2B are plan views respectively illustrating the non-energized state and the energized state of the excitation coil of the electromagnet device shown in FIG. 1. Figure 3 is the above-mentioned figure 1.
4 is a rear view of the electromagnet device shown in FIG. 3 taken along the - line, and FIG. 5 is an enlarged view of FIG. 4 above. 6 is an assembled perspective view of an electromagnet device showing an embodiment of the present invention, and FIG. 7 is a cross-sectional view of the main part of the electromagnet device shown in FIG. 6 above. Figure, 8th
Figure 9 is an assembled perspective view showing another embodiment of the present invention.
Figure A is a perspective view of the assembly example of the embodiment shown in Figure 8 after assembly, Figure 9B is a sectional view of the portion surrounded by the bypass member in Figure 9A, and Figures 10A and B are views of the present invention. FIG. 3 is a cross-sectional view for explaining the shape of a bypass member. 1, 2, 25, 26... York, 3, 27...
Permanent magnet, 4, 21, 23... Bypass member, 5
... Excitation coil, 6... Armature.

Claims (1)

【実用新案登録請求の範囲】 永久磁石と、 この永久磁石の一方の極に後端部を連結された
第1のヨークと、 上記永久磁石の他方の極に後端部を連結された
第2のヨークと、 上記第1、第2のヨークの先端面に、上記永久
磁石の磁力によつて吸着されるアーマチユアと、 上記第1、第2のヨークの内少なくとも一方に
巻装され、通電されることにより上記永久磁石の
磁力による吸着力を減少させて、上記第1、第2
のヨークの先端面より上記アーマチユアを離間さ
せる励磁用コイルとを具備する電磁石装置におい
て、 上記第1、第2のヨークの後端部及び上記永久
磁石の、少なくとも側面及び上下面を覆うよう
に、枠体形状に成型された強磁性体からなるバイ
パス部材をカシメにより外嵌させたことを特徴と
する電磁石装置。
[Claims for Utility Model Registration] A permanent magnet, a first yoke whose rear end is connected to one pole of the permanent magnet, and a second yoke whose rear end is connected to the other pole of the permanent magnet. an armature that is attracted to the front end surfaces of the first and second yokes by the magnetic force of the permanent magnet; and an armature that is wound around at least one of the first and second yokes and is energized. By reducing the attraction force due to the magnetic force of the permanent magnet, the first and second
and an excitation coil that separates the armature from the distal end surface of the yoke, the electromagnetic device comprising: an excitation coil that separates the armature from the distal end surface of the yoke; An electromagnet device characterized in that a bypass member made of a ferromagnetic material molded into a frame shape is fitted onto the outside by caulking.
JP6469582U 1982-04-30 1982-04-30 electromagnet device Granted JPS58168105U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6469582U JPS58168105U (en) 1982-04-30 1982-04-30 electromagnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6469582U JPS58168105U (en) 1982-04-30 1982-04-30 electromagnet device

Publications (2)

Publication Number Publication Date
JPS58168105U JPS58168105U (en) 1983-11-09
JPH0113373Y2 true JPH0113373Y2 (en) 1989-04-19

Family

ID=30074711

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6469582U Granted JPS58168105U (en) 1982-04-30 1982-04-30 electromagnet device

Country Status (1)

Country Link
JP (1) JPS58168105U (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001307919A (en) * 2000-04-24 2001-11-02 Genesis:Kk Hybrid magnet
JP2002025819A (en) * 2000-05-01 2002-01-25 Genesis:Kk Magnetic attracting device using hybrid magnet
JP2002110418A (en) * 2000-09-29 2002-04-12 Genesis:Kk Basic suction structure
JP5969244B2 (en) * 2012-03-29 2016-08-17 東洋ゴム工業株式会社 Power generation element
JP5986773B2 (en) * 2012-03-29 2016-09-06 東洋ゴム工業株式会社 Power generation element
JP5894832B2 (en) * 2012-03-29 2016-03-30 東洋ゴム工業株式会社 Power generation element
JP6093573B2 (en) * 2013-01-07 2017-03-08 東洋ゴム工業株式会社 Power generation element cover
JP6153451B2 (en) * 2013-11-07 2017-06-28 東洋ゴム工業株式会社 Power generation element

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5844574Y2 (en) * 1978-04-18 1983-10-08 株式会社白金製作所 Structure of electromagnet

Also Published As

Publication number Publication date
JPS58168105U (en) 1983-11-09

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