JPS5846608A - Polarized electromagnet - Google Patents

Polarized electromagnet

Info

Publication number
JPS5846608A
JPS5846608A JP56144967A JP14496781A JPS5846608A JP S5846608 A JPS5846608 A JP S5846608A JP 56144967 A JP56144967 A JP 56144967A JP 14496781 A JP14496781 A JP 14496781A JP S5846608 A JPS5846608 A JP S5846608A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic flux
armature
permanent magnet
coil
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.)
Granted
Application number
JP56144967A
Other languages
Japanese (ja)
Other versions
JPS634683B2 (en
Inventor
Hidetoshi Matsushita
松下 英敏
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 Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP56144967A priority Critical patent/JPS5846608A/en
Publication of JPS5846608A publication Critical patent/JPS5846608A/en
Publication of JPS634683B2 publication Critical patent/JPS634683B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/08Electromagnets; Actuators including electromagnets with armatures
    • H01F7/14Pivoting armatures

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Electromagnets (AREA)

Abstract

PURPOSE:To eliminate the loss of magnetic flux by making the magnetic flux of a coil reach magnetic gaps without passing through a permanent magnet. CONSTITUTION:When magnetic flux shown by the broken line is generated within a yoke 1 by exciting a coil 4, the magnetic flux polarization arises in magnetic gaps 10 at both sides of an armature 12 because a permanent magnet 7 produces its magnetic flux in the direction shown by the solid line. This polarization causes the free end part of the armature 12 to rotate in the direction indicated by the arrow and more a movable frame 13 engaging the armature in the same direction, thereby making contact between a fixed contact 22 and a movable contact 20 while breaking contact between a fixed contact 21 and a movable contact 19. At this time the magnetic flux by the coil 4 does not pass through the inside of the parmanent magnet 7, therefore, all the magnetic flux acts upon the magnetic gaps 10, reducing the loss of the magnetic flux and improving the electromagnet's sensitivity and responsiveness.

Description

【発明の詳細な説明】 本発明紘有極電磁石に関する。[Detailed description of the invention] The present invention relates to a polarized electromagnet.

近時、PC板上への実装に適した薄型かつ高感度の有極
継電器の提供が望まれているが、一般に従来の有極電磁
石においては、コイルによる、磁束が通過する磁路中に
永久磁石が存在する構造となってお9.かかる永久磁石
の磁気抵抗紘空気とほば同じ程度に高いことから、コイ
ルからの磁束の大部分は磁気的吸引力を発生する磁気ギ
ヤツブ以外oIl1分でロスされてしまい、これが電磁
石の高感度化を妨ける原因となってい丸。
Recently, there has been a desire to provide a thin and highly sensitive polarized relay that is suitable for mounting on a PC board, but in general, in conventional polarized electromagnets, there is a permanent wire in the magnetic path through which the magnetic flux passes through the coil. 9. The structure has a magnet. Since the magnetic resistance of such a permanent magnet is almost as high as that of the air, most of the magnetic flux from the coil is lost in 1 minute except for the magnetic gear that generates the magnetic attraction, and this is due to the high sensitivity of the electromagnet. The circle that is causing the obstruction.

本発明祉叙上の点に鍾み提案されたものであり、その目
的とするところはコイルによる磁束が永久磁石を通過す
ることなく磁気ギャップに到達するようにして磁束の有
効利用を図り、高感度化を可能ならしめた有極電磁石を
提供するにある。
This proposal was made in consideration of the points stated in the work description of the present invention, and its purpose is to effectively utilize the magnetic flux by allowing the magnetic flux from the coil to reach the magnetic gap without passing through the permanent magnet, and to increase the efficiency of the magnetic flux. The object of the present invention is to provide a polarized electromagnet that enables sensitivity.

しかして本発明は、第1図乃至第1O図に示す第1の発
明と、第11図乃至第u図に示す単安定動作可能な第2
の発明とを包含するもので、以下、181図乃至第10
図に沿って第1の発明の檀々の実施例を説明する。
Therefore, the present invention combines the first invention shown in FIGS. 1 to 1O and the second invention capable of monostable operation shown in FIGS. 11 to 1U.
181 to 10 below.
Embodiments of the first invention will be described along with the drawings.

第1図は第1の実施例であり、図において略C字形のヨ
ーク10基片2にはコイル枠3を介してコイル4が巻装
されておシ、・ヨーク1の側片5゜6間には、この側片
5,6に接しかつ長さ方向の中央部と両端部が異極に着
磁された永久磁石7が配設されている。細片5.6に夫
々直交しかつ基片2に平行な一対の対向片8,9は磁気
ギャップ10i隔てて一直線上に配設され、この磁気ギ
ャップ10内には永久磁石7の中央部近傍に支点11を
有する反転型の囲動自在なアマチュアνが配設される。
FIG. 1 shows the first embodiment. In the figure, a substantially C-shaped yoke 10 has a coil 4 wound around the base piece 2 via a coil frame 3. A permanent magnet 7 is disposed in between, in contact with the side pieces 5 and 6, and whose center portion and both end portions in the longitudinal direction are magnetized with different polarities. A pair of opposing pieces 8 and 9, each perpendicular to the strip 5.6 and parallel to the base piece 2, are arranged in a straight line with a magnetic gap 10i between them. An inverted type movable armature ν having a fulcrum 11 is disposed.

第1図←)において、対向片8.9に平行にプラスチッ
ク勢の成製品からなる可動枠13が配設されており、そ
の長さ方向の略中央部に形成された凹部14がアマチュ
アνの自由゛端部に係合している。
In Fig. 1 ←), a movable frame 13 made of a plastic product is arranged parallel to the facing piece 8.9, and a recess 14 formed approximately at the center in the length direction is located in the armature ν. Engaged to the free end.

すなわちアマチュア臣の回動に伴ない、凹部14にて係
合している可動枠Uが図中、左右に移動し得るようにな
っている0 可動枠13はその両端部近傍に−#Iを係合させた保持
バネ「、16にてヨーク1の側片5,6に連結され支持
されている0また可動枠13の両端部には一端を一定し
てなる接点バネ17 、18の自由端部が係合しておシ
、かかる自由端部に夫々設けられた可動接点19 、2
0は固定接点21 、22に夫々対向している◎ しかしてその動作は、コイル4の励磁にょ9例えば第1
11N>中、破線で示す方向の磁束がヨーク1内に生じ
友とすると、この時永久磁石7による磁束の方向は実線
で示すとおりであるため、アマチュアUの両側の磁気ギ
ャップ10に祉磁束の偏シを生じ、ア!チェアシの自由
端部は図中矢印方向゛に回動することとなる。従ってア
マチュアνに係合している可動枠nも同方向に移動し、
固定接点nと可動接点加とを閉成し、他方、固定接点2
1と可動後点鱒とを開離せしめるものである。
In other words, as the amateur subject rotates, the movable frame U engaged in the recess 14 can move from side to side in the figure. The engaged holding springs 16 are connected to and supported by the side pieces 5 and 6 of the yoke 1, and the free ends of contact springs 17 and 18 are fixed at both ends of the movable frame 13. The movable contacts 19 and 2 are provided at the free ends of the movable contacts 19 and 2, respectively.
0 faces the fixed contacts 21 and 22, respectively.◎ However, the operation depends on the excitation of the coil 4, for example, the first
11N>, magnetic flux in the direction shown by the broken line is generated in the yoke 1, and the direction of the magnetic flux due to the permanent magnet 7 is as shown by the solid line. It causes bias, a! The free end of the chair will rotate in the direction of the arrow in the figure. Therefore, the movable frame n engaged with the armature ν also moves in the same direction,
The fixed contact n and the movable contact are closed, and the fixed contact 2 is closed.
1 and the movable rear point trout are separated.

この際、本発明ではコイル4による磁束が永久磁石7の
内部を通過することがないためはげ全ての磁束が磁気ギ
ャップ1Gに作用し、磁束のロスがなく、電磁石の感度
、即応性の向上が図れる利点がある。
At this time, in the present invention, since the magnetic flux from the coil 4 does not pass through the inside of the permanent magnet 7, all the magnetic flux acts on the magnetic gap 1G, so there is no loss of magnetic flux, and the sensitivity and responsiveness of the electromagnet are improved. There are advantages that can be achieved.

第2図は第2の実施例を示しており、この例では永久磁
石を部分して互いの対向部が同極に着磁された永久磁石
7a 、7bとなし、反転型のアマチュアνの長さ方向
の中央部を支点11にて軸支すると共にアマチュア12
の自由一部辰芳を一気ギャップlO間および永久磁石r
*、tb相互間に位置せしめたもので、その動作および
図示されていない可動枠や接点尋の構造は第1の実施例
と同様である。   ′− 第3図は第3の実施例であり、この例では一対の永久磁
石7a、7bをコ字形の一片おにて連結し、この鉄片2
3t−磁極として使用するようにしたものである。
FIG. 2 shows a second embodiment. In this example, permanent magnets 7a and 7b are formed by dividing a permanent magnet into permanent magnets 7a and 7b whose opposing parts are magnetized with the same polarity, and the length of an inverted armature ν is The center part in the horizontal direction is pivotally supported at the fulcrum 11, and the armature 12
At once, move the free part of Tatsuyoshi between the gap lO and the permanent magnet r
*, tb, and its operation and structure of the movable frame and contact pads (not shown) are the same as in the first embodiment. '- Fig. 3 shows a third embodiment, in which a pair of permanent magnets 7a and 7b are connected by a U-shaped piece, and this iron piece 2
It is designed to be used as a 3t magnetic pole.

第4図は第4の実施例を示しており、アマチュア12’
kU字形となし、その湾曲部を永久磁石7a。
FIG. 4 shows a fourth embodiment, in which an amateur 12'
It has a kU-shape, and its curved part is a permanent magnet 7a.

7b相互間で支点11によシ支持して構成されている0
− 第5図社第5の実施例で69.との例でId w −り
1をコ字形に形成すると共に、このヨーク1の側片5,
6の開放端部相互間に亘る一片を有する丁字形Oアマチ
ュア12YI−永久磁石7m、7b相互間において支点
11によシ支持している。
7b supported by the fulcrum 11.
- 69 in the fifth embodiment of Figure 5. In this example, the Idw-ri 1 is formed into a U-shape, and the side pieces 5,
A T-shaped O armature 12YI having a piece extending between the open ends of 6 is supported on a fulcrum 11 between permanent magnets 7m and 7b.

第6図は第6の実施例を示しておシ、コ字形の薯−り1
の側片5,6の開放端部相互間に亘る長さを有し、かつ
中央部をU字形に湾曲させたアマチュアνを前記U字形
の湾曲部分にて支点11により1動自在に軸支したもの
である〇 これまでの各実施例では永久磁石7またFi7a。
FIG. 6 shows the sixth embodiment, and shows the C-shaped and U-shaped corners 1.
An armature ν having a length extending between the open ends of the side pieces 5 and 6 and having a central portion curved in a U-shape is pivotably supported by a fulcrum 11 at the curved portion of the U-shape. 〇In each of the previous embodiments, the permanent magnet 7 or Fi7a was used.

7bがヨーク1の内部空間に配設されているが、以下に
述べるように一対の永久磁石7a 、7btヨーク1の
外部の空間に配設することも可能であるO すなわち第7の実施例として、第7図に示すようにヨー
クlの対向片8,9上に対向片8,99Illが同極に
着磁された永久磁石7m、7bを載設すると共に、永久
磁石7m、7bの他極相互間に磁極片24を載設し、こ
の磁極片Uの略中央部に窓孔を穿設せしめて磁気ギャッ
プloに一端が配置されるアマチュアνの他端部を窓孔
から央出せしめてなる。なお、磁極片腕はこの実施例の
如く単一でなく一対形成して、各永久磁石7m、7b上
に夫夫型々に載設してもよい。しかしてその動作は、第
7図(イ)においてコイル4への通電によジョーク1内
を破線方向に磁束が通過すると、この時永久磁石7a 
、7bによる磁束は図中%実線で示す方向に生じるため
、アマチュアνの下端部の両飼にある磁気ギャップlO
で磁束が偏在し、アマチュア12の下端部は図中右側に
吸引され、上端部は図中の矢印方向に移動するものであ
る。
7b is arranged in the internal space of the yoke 1, but as described below, it is also possible to arrange the pair of permanent magnets 7a and 7b in the external space of the yoke 1. That is, as a seventh embodiment. As shown in FIG. 7, permanent magnets 7m and 7b, in which the opposing pieces 8 and 99Ill are magnetized to the same polarity, are mounted on the opposing pieces 8 and 9 of the yoke l, and the permanent magnets 7m and 7b have the other poles. A magnetic pole piece 24 is placed between them, a window hole is bored in the approximate center of the magnetic pole piece U, and the other end of the armature ν, one end of which is disposed in the magnetic gap lo, is made to protrude from the center of the window hole. . Incidentally, the magnetic pole arm is not single as in this embodiment, but may be formed in pairs and mounted on each of the permanent magnets 7m and 7b in a husband-and-wife pattern. However, the operation is such that when the coil 4 is energized and magnetic flux passes through the joke 1 in the direction of the broken line in FIG. 7(a), the permanent magnet 7a
, 7b is generated in the direction shown by the solid line in the figure, so the magnetic gap lO at the lower end of the armature ν
The magnetic flux is unevenly distributed, the lower end of the armature 12 is attracted to the right side in the figure, and the upper end moves in the direction of the arrow in the figure.

第8図は第8の実施例でアマチュア12t−逆U字形に
形成しかつ一対の磁極片24m、24bを採用したもの
、第9図は第9の実施例でアマチュア12ヲT字形にし
たもの、第1O図扛第1Oの実施例で磁極片−に対して
アマチュア12t−平行に配設し九例である。
Fig. 8 shows an eighth embodiment in which the armature 12t is formed in an inverted U shape and employs a pair of magnetic pole pieces 24m and 24b, and Fig. 9 shows an armature 12 in the ninth embodiment in a T-shape. In the embodiment shown in Fig. 1O, the armature 12t is disposed parallel to the magnetic pole piece.

以上説明した第1の発明の各実施例では、永久磁石7 
e 7 a * 7 bによる磁束はアマチュア12お
よび磁気ギャップlOt介して磁気ギャップ10’j−
形成するl−り1の両端部に均等匹通過するように構成
されている〇 次に上述した第1の発明と同様にコイルによる磁束が永
久磁石を通過しない構成を有し、かつ単安定動作を可能
ならしめる第2の発明につき第11図乃至第talII
t−参照しつつ説明する0第11図はその第1の実施例
を示している。同図において略C字形のヨーク1の対向
片8.9上に紘対向片8,9側を同極に*aした永久磁
石7m。
In each embodiment of the first invention described above, the permanent magnet 7
The magnetic flux due to e 7 a * 7 b passes through the armature 12 and the magnetic gap lOt to the magnetic gap 10'j-
It is configured so that the magnetic flux passes equally through both ends of the L-ri 1 to be formed.Similarly to the first invention described above, it has a configuration in which the magnetic flux from the coil does not pass through the permanent magnet, and has a monostable operation. 11 to tal II regarding the second invention that makes possible
FIG. 11 shows the first embodiment. In the figure, a permanent magnet 7m is placed on the opposing pieces 8 and 9 of the substantially C-shaped yoke 1, with the opposing pieces 8 and 9 having the same polarity *a.

7bが載設されている0このうち一方の永久磁石、例え
ば7&の上部にはL字形の磁極片24mが配設され、こ
の磁極片24mの一片とヨーク1端部との間には磁気ギ
ャップ器が形成される0また、磁極片24mの他片と磁
気ギャップを隔てて対向するように、他方の永久磁石7
b上に平板状の磁極片24bが載設されている0 この動作を説明すると、コイル4ft励磁していない状
態で祉永久磁石7aによる磁束の一部はL字形の磁極片
241.磁気ギャップ部およびヨーク10対向片8を介
してロスされており、永久磁石7aよりも他方の永久磁
石7bの磁気的吸引力が優ってアマチュアνは磁極片2
4bに安定して吸引されている。コイル4に通電されて
磁束が図中破線で示す方向にヨーク1内を通ると、アマ
チュアシ下端部内儒の磁気ギャップlGにおいて磁束が
偏在することになると共に、磁極片24mからの磁束が
アマチュアνに作用し、アマチュアνはその上端部が図
中矢印方向に回動して磁極片24mに吸引される。コイ
ル4の励磁を止めるとアマチュアル紘反転して再び磁極
片24bに吸引されるものであシ、以上のように単安定
動作が可能となる0第ν図は第2の実施例であり、C字
形のヨーク1の一方の側片6を延長し、一方の対向片9
を永久磁石7bの上端部に載設して磁気ギャップを介し
磁極片24hに対向させ、ま九他方の対向片8に磁気ギ
ャップlOを介して、永久磁石7bの下端部に設けた磁
極片24bt一対向させると共に、磁極片24bの端部
と側片6との間に磁気ギャップ26′を形成したもめで
ある。かかる構造によシ永久磁石7b〕 による閉磁路は形成されるが、磁気ギャップ%の丸め永
久磁石7aによる閉磁路は形成されず、コイル4が励磁
されない状態で社アマチュアνの上端部はヨーク10対
向片9側に吸引され、コイル4の励磁時には図示の如き
各磁束の方向によりアマチュア12の1端IB線磁極片
24a側に吸引されて単安定動作をなす・ 第13111IIi第3の実施例を示しており、磁極片
24a。
An L-shaped magnetic pole piece 24m is disposed above one of the permanent magnets, for example 7&, and a magnetic gap is formed between one piece of this magnetic pole piece 24m and the end of the yoke 1. In addition, the other permanent magnet 7 is placed so as to face the other piece of the magnetic pole piece 24m across a magnetic gap.
A flat magnetic pole piece 24b is mounted on the magnetic pole piece 241. The magnetic attraction force of the other permanent magnet 7b is superior to that of the permanent magnet 7a, and the armature ν is lost through the magnetic gap part and the opposing piece 8 of the yoke 10.
It is stably attracted to 4b. When the coil 4 is energized and the magnetic flux passes through the yoke 1 in the direction shown by the broken line in the figure, the magnetic flux is unevenly distributed in the magnetic gap lG of the lower end of the armature, and the magnetic flux from the magnetic pole piece 24m is The upper end of the armature ν rotates in the direction of the arrow in the figure and is attracted to the magnetic pole piece 24m. When the excitation of the coil 4 is stopped, the armature is reversed and the coil is attracted to the magnetic pole piece 24b again. As mentioned above, the monostable operation is possible as shown in Fig. 0, ν, which is the second embodiment. One side piece 6 of the C-shaped yoke 1 is extended, and one opposing piece 9
A magnetic pole piece 24b is placed on the upper end of the permanent magnet 7b and opposed to the magnetic pole piece 24h through a magnetic gap, and a magnetic pole piece 24b is placed on the lower end of the permanent magnet 7b with the other opposing piece 8 placed on the lower end of the permanent magnet 7b through a magnetic gap lO. This is a conflict in which a magnetic gap 26' is formed between the end of the magnetic pole piece 24b and the side piece 6 while facing each other. With such a structure, a closed magnetic path is formed by the permanent magnet 7b], but a closed magnetic path by the rounded permanent magnet 7a with a magnetic gap of % is not formed, and when the coil 4 is not excited, the upper end of the armature ν is It is attracted to the opposing piece 9 side, and when the coil 4 is energized, it is attracted to the one end IB wire magnetic pole piece 24a side of the armature 12 due to the direction of each magnetic flux as shown in the figure, thereby achieving a monostable operation. 13111IIi Third embodiment Shown is a magnetic pole piece 24a.

24bの板厚、幅、長さ、材質等を変えることで両磁極
24 m 、 241)とアマチュアνとの間の磁気抵
抗を変え、或祉永久磁石の外形や材質勢を変えて起磁力
を変化させ、:tイル4の無励磁時には左右何れかの磁
極片24a、24bにアマチュア12を吸引させるよう
にし、コイル4の励磁と共にアマチュア12を反転せし
めるようにしたものである。このようにかかる第2の発
明の各実施例では、永久磁石7m、7bによる磁束を永
久磁石7m、7bに連設された磁極片24m、24b、
アマチュアUおよび磁気ギャップ10を介して磁気ギャ
ップ10を形成するヨーク1の両端部に不均等に通過せ
しめるように構成されている@ 以上のように本発明によれば、第1および第2の発明の
何れにおいても?イルによる磁束が永久磁石を通過する
ことなく磁気ギャップに到達するように構成したから、
ディルからの磁束のロスがなく殆んど全ての磁束がアマ
チュアの駆動に寄与でき、有極電磁石および有極−電器
の高感度化が図れる効果があり、単安定動作用の有極電
磁石も容易に構成できる尋のオリ点がある。
By changing the plate thickness, width, length, material, etc. of 24b, the magnetic resistance between both magnetic poles 24 m, 241) and the armature ν can be changed, and the magnetomotive force can be increased by changing the external shape and material of the permanent magnet. When the coil 4 is not energized, the armature 12 is attracted to either the left or right magnetic pole pieces 24a, 24b, and when the coil 4 is energized, the armature 12 is reversed. In this way, in each embodiment of the second invention, the magnetic flux from the permanent magnets 7m, 7b is transferred to the magnetic pole pieces 24m, 24b, which are connected to the permanent magnets 7m, 7b.
According to the present invention, as described above, the first and second inventions In any of these? Because the magnetic flux from the coil reaches the magnetic gap without passing through the permanent magnet,
There is no loss of magnetic flux from the dill, and almost all the magnetic flux can contribute to the drive of the armature, which has the effect of increasing the sensitivity of polarized electromagnets and polarized electric appliances, and it is easy to create polarized electromagnets for monostable operation. There is a basic origin that can be constructed as follows.

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

第1図乃至第1O図は第1の発明の各実施例を示してお
り、第1図0)は第1の実施例、の要部の賜明図、同図
(ロ)は同じく装部の断面図、第2図乃至第6図は夫々
第2乃至第6の実施例の要部の説明図、第7図(イ)は
第7の実施例の要部のl1I2明図、同図(ロ)は同じ
く斜視図、第8図乃至第io図は夫々第′8乃至第1O
の実施例の要部の説明図、@11図乃至第13図は第2
の発明、の夫々第、l、乃至第3の7実施例を示す要部
の説明図である。      、1・・・・・・ヨーク
、4・・・・・・コイル、7,7、J、7b・・・・・
・永久磁石、10・・・・・・磁気ギャップ、ル・・・
・・・アマチュア、24m、24b・・・・・・磁極片
゛特許出願人 松下電工株式会社 才10図 、T12閏
1 to 1O show each embodiment of the first invention, FIG. 10) is a diagram showing the main part of the first embodiment, and FIG. FIGS. 2 to 6 are explanatory diagrams of the main parts of the second to sixth embodiments, respectively. FIG. 7(A) is a clear view of the main parts of the seventh embodiment. (B) is also a perspective view, and Figures 8 to io are 8th to 10th views, respectively.
11 to 13 are explanatory diagrams of the main parts of the embodiment.
FIG. 3 is an explanatory view of the main parts of seven embodiments of the invention, respectively. , 1... Yoke, 4... Coil, 7, 7, J, 7b...
・Permanent magnet, 10...Magnetic gap, Le...
...Amateur, 24m, 24b...Magnetic pole piece Patent applicant: Matsushita Electric Works Co., Ltd.

Claims (2)

【特許請求の範囲】[Claims] (1)  コイルを巻装してなる略C字形のヨークの磁
気ギャップ内に回動自在なアマチュアの−Sを配設する
と共I′c%前記アマチュアを中立状態にて待機させる
べく着磁され良永久磁石を前記磁気ギャップの外部に配
設し、前記永久磁石による磁束を前記アマチュアおよび
前記磁気ギャップを介して該磁気ギャップを形成する前
記ヨークの両端部に均郷に通過せしめるように構成した
ことを特徴とする有極電磁石。
(1) When a rotatable armature -S is disposed within the magnetic gap of a substantially C-shaped yoke formed by winding a coil, the armature is magnetized so as to standby in a neutral state. A good permanent magnet is disposed outside the magnetic gap, and the magnetic flux from the permanent magnet is configured to uniformly pass through the armature and the magnetic gap to both ends of the yoke forming the magnetic gap. A polar electromagnet characterized by:
(2)  コイルを巻装してなる略C字形のヨークの磁
気ギャップ内に回動自在なアマチュアの一部を配役する
と共に、一対の永久磁石を前記磁気ギャップの外部にお
いて前記アマチュアの両翻に配赦し、前記永久磁石によ
る磁束を該永久磁石に連設された磁極片、前記アマチュ
ア、および磁気ギャップを介して咳磁気ギャップを形成
する前記日−りの両端部に不均尋に通過せしめるように
構成したことを特徴とする有極電磁石。
(2) A part of a rotatable armature is placed within the magnetic gap of a substantially C-shaped yoke formed by winding a coil, and a pair of permanent magnets are placed outside the magnetic gap on both sides of the armature. so that the magnetic flux from the permanent magnet is passed unevenly through the magnetic pole pieces connected to the permanent magnet, the armature, and the magnetic gap to both ends of the magnetic field forming the magnetic gap. A polarized electromagnet characterized by having the following structure.
JP56144967A 1981-09-14 1981-09-14 Polarized electromagnet Granted JPS5846608A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56144967A JPS5846608A (en) 1981-09-14 1981-09-14 Polarized electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56144967A JPS5846608A (en) 1981-09-14 1981-09-14 Polarized electromagnet

Publications (2)

Publication Number Publication Date
JPS5846608A true JPS5846608A (en) 1983-03-18
JPS634683B2 JPS634683B2 (en) 1988-01-30

Family

ID=15374349

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56144967A Granted JPS5846608A (en) 1981-09-14 1981-09-14 Polarized electromagnet

Country Status (1)

Country Link
JP (1) JPS5846608A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61125012U (en) * 1985-01-25 1986-08-06
JPS62163906U (en) * 1986-04-08 1987-10-17

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61125012U (en) * 1985-01-25 1986-08-06
JPS62163906U (en) * 1986-04-08 1987-10-17

Also Published As

Publication number Publication date
JPS634683B2 (en) 1988-01-30

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