JPS58131707A - Polarized electromagnet device - Google Patents

Polarized electromagnet device

Info

Publication number
JPS58131707A
JPS58131707A JP57014034A JP1403482A JPS58131707A JP S58131707 A JPS58131707 A JP S58131707A JP 57014034 A JP57014034 A JP 57014034A JP 1403482 A JP1403482 A JP 1403482A JP S58131707 A JPS58131707 A JP S58131707A
Authority
JP
Japan
Prior art keywords
yoke
armature
permanent magnet
piece
magnetic
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.)
Pending
Application number
JP57014034A
Other languages
Japanese (ja)
Inventor
Kenji Kawasaki
健司 川崎
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 JP57014034A priority Critical patent/JPS58131707A/en
Publication of JPS58131707A publication Critical patent/JPS58131707A/en
Pending 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 obtain easily the desired attracting force curve by varying freely thickness of the permanent magnet of the polarized electromagnet device by a method wherein the device is made to have structure in the manner that the edge faces of the edte parts of a pair of magnetic plates provided at both sides of the permanent magnet face respectively to yoke pieces. CONSTITUTION:At gaps formed between the upper part lateral piece 16 of a U-shaped yoke 15 and the edge faces 13a, 14a of the edge parts on one side of a pair of the magnetic plates 13, 14, and gaps formed between the lower part lateral piece 17 of the U- shaped yoke 15 and the edge faces 13b, 14b of the edge parts on another side of a pair of the magnetic plates 13, 14, attracting force is generated at the place where the directions of magnetic fluxes X, Y are in the same direction, and repulsion is generated at the place where the directions are in the opposite direction. Accordingly an armature 10 rotates in the anticlockwise direction centering around an axis 11. When the direction of the current in a coil 18 is changed to form magnetic flux Y thereof in the opposite direction to the direction mentioned above, the armature 10 rotates in the opposite direction to the direction mentioned above. The rotational stroke of the armature 10 is determined by an interval (d) between the upper part lateral piece 16 and the lower part lateral piece 17 of the yoke 15, and by length (c) of the magnetic plates 13, 14 of the armature 10, irrespective of the thickness of the permanent magnet 12.

Description

【発明の詳細な説明】 この発明は、有極型電磁石装置、特に4空隙有極型電磁
石装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a polarized electromagnet device, particularly a four-gap polarized electromagnet device.

従来の4空隙有極型電磁石装置11、jH1図に示すよ
うに、中央部が軸lによって+H枢支されている板状永
久磁石2のm軸に対して直交する両側部に一対の磁性板
3.4を設けてアーマチュア5を構成し、コ字状ヨー、
り6のコ字状のE片7の先端を上記一対の磁性板8.4
のそれぞれの上端部8λ。
Conventional 4-gap polarized electromagnet device 11, as shown in Figure jH1, a pair of magnetic plates are placed on both sides perpendicular to the m-axis of a plate-shaped permanent magnet 2 whose central portion is pivoted +H by an axis l. 3.4 is provided to constitute the armature 5, and the U-shaped yaw,
The tip of the U-shaped E piece 7 of the holder 6 is attached to the pair of magnetic plates 8.4.
The upper end portions 8λ of each.

41の間管で延ばすとともに、コ字状の下片8の先端を
上記一対の磁性板3.4のそれぞれの下端部Bb 、4
bの間まで延ばすことにより構成されている。9は、コ
イルでちる。この電磁石装置は、第1図の状態において
、永久磁石2の磁束Xが点線のように形成され、またコ
イル9の磁束Yが実線のように形成される。したかって
、ヨーク6のコ字状の一上片7の先端延長部と−ゾ・↑
の磁性板3.。
41 with a tube, and the tip of the U-shaped lower piece 8 is connected to the respective lower ends Bb, 4 of the pair of magnetic plates 3.4.
It is constructed by extending it to between b. 9 is a coil. In this electromagnet device, in the state shown in FIG. 1, the magnetic flux X of the permanent magnet 2 is formed as shown by the dotted line, and the magnetic flux Y of the coil 9 is formed as shown by the solid line. Therefore, the tip extension of the U-shaped upper piece 7 of the yoke 6 and -zo・↑
magnetic plate 3. .

4の上端部8a、4aとでつくられるギャップおよび目
−り6のコ字状の下片8の先端延長部と一対の磁性板8
,4の丁端部Bb 、 4bとでつくられるギャップに
おいて、磁束X、Yの方向が同方向のところで吸引力か
生じ、逆方向のところで反発力が生じる。そのため図示
の状態では、アーマチェアロは、軸l全中心に反時計方
向に回動する。コイル9の電流方向を変えればコイル9
の磁束Yが上記と逆方向に形成され、アーマチュア5は
上記と逆方向に回動する。この場合、アーマチュア50
回動ストロークは、永久磁石2の大きさく厚み)をbと
し、ヨーク6の厚みをlとすると、(b−1)/2とな
り、永久磁石2の厚みbとヨーク6の厚みaで決まる。
4 and the gap formed by the upper end portions 8a, 4a of the mesh 6 and the end extension of the U-shaped lower piece 8 of the eye 6 and the pair of magnetic plates 8.
, 4, an attractive force is generated where the directions of the magnetic fluxes X and Y are the same, and a repulsive force is generated where the directions are opposite. Therefore, in the illustrated state, the armchair rotates counterclockwise around the axis l. If you change the current direction of coil 9, coil 9
A magnetic flux Y is formed in the opposite direction to the above, and the armature 5 rotates in the opposite direction to the above. In this case, armature 50
The rotation stroke is (b-1)/2, where b is the size and thickness of the permanent magnet 2 and l is the thickness of the yoke 6, and is determined by the thickness b of the permanent magnet 2 and the thickness a of the yoke 6.

したかって、電磁石装置を構成するうえで、アーマチュ
ア5の回動ストロークおよび永久磁石2の厚みがおのず
と限定されていた。
Therefore, in configuring the electromagnet device, the rotation stroke of the armature 5 and the thickness of the permanent magnet 2 are naturally limited.

この発明は、このような事情に鑑みなされたもので、中
央部が軸枢支されている板状永久磁石とこの板状永久磁
石の磁軸に対して直交する両側部に設けられている一対
の磁性板とからなるアーマチュアと、一方および他方の
ヨーク片とこれらを連結する連結片とからなり上記一対
の磁性板のそれぞれの板の一方の端部の端面に一方のヨ
ーク片が対面しそれぞれの板の他方の端部の端面に他方
のヨーク片が対面した状態で配設されているヨークと、
上記ヨークに装着されているコイルを備えた有極型電磁
石装置をその要旨とするものである。
This invention was made in view of the above circumstances, and consists of a plate-shaped permanent magnet whose central portion is pivotally supported, and a pair of plate-shaped permanent magnets provided on both sides perpendicular to the magnetic axis of the plate-shaped permanent magnet. an armature consisting of a magnetic plate; one yoke piece and the other yoke piece; and a connecting piece connecting them; one yoke piece facing the end face of one end of each of the pair of magnetic plates; a yoke disposed with the other yoke piece facing the end surface of the other end of the plate;
The gist of the present invention is a polarized electromagnet device including a coil mounted on the yoke.

すなわち、この有極型電磁石装置は、アーマチュアの回
動ストロークが永久(ホ)石の厚みとは無関係に決まる
ため、永久磁石の厚みを自由に変えて所望の吸引力カー
ブを容易に得ることができるようになる。
In other words, in this polarized electromagnet device, the rotation stroke of the armature is determined independently of the thickness of the permanent magnet, so the thickness of the permanent magnet can be freely changed to easily obtain the desired attraction force curve. become able to.

つぎに、この発明を実施例にもとづいて説明する。Next, the present invention will be explained based on examples.

第2図はこの発明の−’!廁例の構成図である。Figure 2 shows -’! of this invention! FIG. 2 is a configuration diagram of an example.

図において、lOはアーマチュアで、中央部が軸ltm
よって軸枢支されている板状永久磁石12とその永久磁
石12の磁軸にl↑し−C直交する両側部に設けられて
いる一対の磁性板18.14とからなる。15はコ字状
のヨークで、その上部横片16が上記磁性板18.14
の−すの端部の端面111.141に対面し、下部横片
17が上記磁性板18.14の他方の端部の端面18b
、14bK対面している。Cは上記一対の磁性板18.
14の長さ、dは上記ヨーク16の上部横片16と下部
横片17との間隔を示す。18はコイルで、上記コ字状
のヨーク15のコ字状の縦片19に巻装されている。
In the figure, lO is the armature, and the center part is the shaft ltm
Therefore, it consists of a plate-shaped permanent magnet 12 which is pivotally supported and a pair of magnetic plates 18, 14 provided on both sides of the permanent magnet 12, which are perpendicular to the magnetic axis of the permanent magnet 12 at 1↑ and -C. 15 is a U-shaped yoke, the upper horizontal piece 16 of which is connected to the magnetic plate 18.14.
The lower horizontal piece 17 faces the end surface 111.141 of the end of the magnetic plate 18.14.
, 14bK are facing each other. C is the pair of magnetic plates 18.
The length d of 14 indicates the distance between the upper horizontal piece 16 and the lower horizontal piece 17 of the yoke 16. A coil 18 is wound around the U-shaped vertical piece 19 of the U-shaped yoke 15.

第2図において、上記板状永久磁石12の磁束Xは点線
で示すように形成され、コイル18の磁束Yは実線で示
すように形成される。したがって、コ字状ヨーク15の
上部横片16と一対の磁性板18.14の一方の端部の
端面1B8,141でつくられるギャップ、およびコ字
状ヨーク16の下部横片17と一対の磁性板18.14
の他方の端部の端面18b、14bでつくられるギャッ
プにおいて、磁束X、Yの方向が同方向のところで吸引
力が生じ、逆方向のところで反撥力が生じる。そのため
、図示の状態では、アーマチュア10は、軸11を中心
に反時計方向に回動する。コイル18の電流方向を変え
その磁束Yを上記と逆方向に形成すると、アーマチュア
10は上記と逆方向に回動する。すなわち、コイル18
に直流を交互に印加することにより、アーマチュアlO
が軸11を中心に交互に正逆に回動する。
In FIG. 2, the magnetic flux X of the plate-shaped permanent magnet 12 is formed as shown by a dotted line, and the magnetic flux Y of the coil 18 is formed as shown by a solid line. Therefore, a gap is formed between the upper horizontal piece 16 of the U-shaped yoke 15 and the end surface 1B8, 141 at one end of the pair of magnetic plates 18.14, and the gap between the lower horizontal piece 17 of the U-shaped yoke 16 and the pair of magnetic plates 18. Board 18.14
In the gap formed by the end surfaces 18b and 14b at the other end, an attractive force is generated where the directions of the magnetic fluxes X and Y are the same, and a repulsive force is generated where the directions are opposite. Therefore, in the illustrated state, the armature 10 rotates counterclockwise about the shaft 11. When the current direction of the coil 18 is changed to form its magnetic flux Y in the opposite direction, the armature 10 rotates in the opposite direction. That is, the coil 18
By alternately applying direct current to the armature lO
rotates around the shaft 11 in forward and reverse directions alternately.

との有極型電磁石装置は、F記のように、アーマチュア
10をコ字状ヨーク15のコ字状の内部に配設し、そこ
で回動運動させるようにするため、アーマチュア1Gの
回動ストロークは、ヨーク16の上部横片16とF部横
片17との間隔dおよびアーマチュア10の磁性板ta
、Zの長さCで決まり、永久磁石12の厚みは無関係に
なる。
In the polarized electromagnet device, as shown in F, the armature 10 is disposed inside the U-shaped yoke 15 and rotated there, so that the rotation stroke of the armature 1G is are the distance d between the upper horizontal piece 16 of the yoke 16 and the F section horizontal piece 17 and the magnetic plate ta of the armature 10.
, Z is determined by the length C, and the thickness of the permanent magnet 12 is irrelevant.

したがって、永久磁石の厚みを自由に変えて、自由な吸
引力カーブを得ることができるようになる。
Therefore, it becomes possible to freely change the thickness of the permanent magnet and obtain a free attractive force curve.

第8図は他の実施例の構成図である。すなわち、この有
極型電磁石装置は、コ字状のヨーク15(第2図)に代
えて、一対のヨーク片20.21の中央部を連結片21
@で連結して構成された略H字状のヨーク22を用い、
そのヨーク22の一方のヨーク片20をアーマチュアl
Oの磁性板111.14の一方の端部の端面181,1
41に対面させるとともに、他方のヨーク片21を磁性
板18.14の他方の端部の端面13b、14bに対面
させ、アーマチュア10を一方および他方のヨーク片2
0.21の間で軸11を中心に回動じつるようにしてい
る。それ以外の部分は第2図の有極型電磁石装置dと同
じであり、作用効果も同じである。
FIG. 8 is a block diagram of another embodiment. That is, in this polarized electromagnet device, instead of the U-shaped yoke 15 (FIG. 2), the center part of the pair of yoke pieces 20 and 21 is connected to the connecting piece 21.
Using a substantially H-shaped yoke 22 connected by @,
One yoke piece 20 of the yoke 22 is connected to the armature l.
End surface 181,1 of one end of magnetic plate 111.14 of O
41, and the other yoke piece 21 faces the end surfaces 13b, 14b of the other end of the magnetic plate 18.
It is designed to be able to rotate around the shaft 11 within a range of 0.21. The other parts are the same as the polarized electromagnet device d shown in FIG. 2, and the effects are also the same.

なお、第3図のヨーク片20.21を第4図に示すよう
に略コ字状に形成し、そのコ字状の横片28.24.2
5.26の端面を一対の磁性板18.14の一方および
他方の端部の端面!B鳳。
The yoke pieces 20.21 in FIG. 3 are formed into a substantially U-shape as shown in FIG. 4, and the U-shaped horizontal pieces 28.24.2
The end faces of 5.26 are the end faces of one and the other end of a pair of magnetic plates 18.14! B Otori.

14a 、 13b 、 14bに対面させるようにし
てもよい。
14a, 13b, and 14b may face each other.

以上のように、この発明の有極型電磁石装置は、永久磁
石の両側部に設けられた一対の磁性板のそれぞれ板の一
方の端部の端面が、ヨーク片の一方に対面し、それぞれ
の板の他方の端部の端面がヨーク片の他方に対面した構
造になっているため、アーマチュアの回動ストロークが
、一方および他方のヨーク片の間隔と磁性板の長さとの
差により生じるヨーク片・磁性板端部端曲間のp隙の入
車によって決まり、永久磁石の厚本J二は、(I(F、
関係になる。したがって、永久磁石の厚みを自由に変え
て所望の吸引力カーブを6易F mることかでへるよ−
うになる。
As described above, in the polarized electromagnet device of the present invention, the end surface of one end of each of the pair of magnetic plates provided on both sides of the permanent magnet faces one of the yoke pieces, and the end face of each plate faces one of the yoke pieces. Because the end surface of the other end of the plate faces the other yoke piece, the rotation stroke of the armature is caused by the difference between the distance between the one and other yoke pieces and the length of the magnetic plate.・Determined by the entry of the p gap between the end bends of the magnetic plate, the permanent magnet Atsushi J2 is (I(F,
Become a relationship. Therefore, it is possible to freely change the thickness of the permanent magnet to obtain the desired attraction force curve by 6 Fm.
I'm going to growl.

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

第1図は従来例の横1〕y図、;′41: 2区はこの
発明の一実施例の構成図、第3図は他のN鴨例の構成図
、第4図はその変彰例の119明図である。 lO・・・了−マチュア 11・・・磁+lqI++2
・・・永久磁石 18.14・・・磁性板 15・・コ
字状三J−り特許出願人 松下電工株式会社 代理人 弁理士 松  本  武  彦第1図 七 第2図 第4図
Figure 1 is a horizontal 1]y diagram of a conventional example, ;'41: Section 2 is a configuration diagram of an embodiment of the present invention, Figure 3 is a configuration diagram of another N duck example, and Figure 4 is a modification thereof. It is a 119-light diagram of an example. lO...Complete-Mature 11...Magnetic+lqI++2
... Permanent magnet 18.14 ... Magnetic plate 15 ... U-shaped three J-ri Patent applicant Matsushita Electric Works Co., Ltd. Agent Patent attorney Takehiko Matsumoto Figure 1, 7, 2, 4

Claims (1)

【特許請求の範囲】 (1)  中央部が軸枢支されている板状永久磁石とこ
の板状永久磁石の磁軸に対して直交する両側部に設けら
れている一対の磁性板とからなるアーマチュアと、一方
および他方のヨーク片とこれらを連結する連結片とから
なり上記一対の磁性板のそれぞれの板の一方の端部の端
面に一方のヨーク片が対面しそれぞれの板の他方の端部
の端面に他方のヨーク片が対面した状態で配設されてい
るヨークと、上記ヨークに装着されているコイルを備え
たことを特徴とする有極型電磁石装置。 (2)  ヨークが、一方のヨーク片と他方のヨーク片
とをそれぞれその端部において連結片により連結するこ
とよりコ字状になっている特許請求の範囲第1項記載の
有極型電磁石装置。 (8)  ヨークか、一方のヨーク片と他方のヨーク片
と管それぞれその中央部において連結片により連結する
ことにより略■字状にな一ノ゛〔いる特許請求の範囲第
1項記載の41+ji型電磁石装置i1t 。
[Scope of Claims] (1) Consisting of a plate-shaped permanent magnet whose central portion is pivotally supported and a pair of magnetic plates provided on both sides of the plate-shaped permanent magnet perpendicular to the magnetic axis. It consists of an armature, one yoke piece and the other yoke piece, and a connecting piece that connects them, one yoke piece facing the end face of one end of each of the pair of magnetic plates, and the other end of each plate. 1. A polarized electromagnet device comprising: a yoke disposed with the other yoke piece facing an end face of the part; and a coil attached to the yoke. (2) The polarized electromagnet device according to claim 1, wherein the yoke has a U-shape by connecting one yoke piece and the other yoke piece by connecting pieces at their respective ends. . (8) The yoke, one yoke piece, the other yoke piece, and the pipe are connected at their central portions by a connecting piece, so that the yoke has a substantially ■-shaped shape. type electromagnet device i1t.
JP57014034A 1982-01-30 1982-01-30 Polarized electromagnet device Pending JPS58131707A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57014034A JPS58131707A (en) 1982-01-30 1982-01-30 Polarized electromagnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57014034A JPS58131707A (en) 1982-01-30 1982-01-30 Polarized electromagnet device

Publications (1)

Publication Number Publication Date
JPS58131707A true JPS58131707A (en) 1983-08-05

Family

ID=11849852

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57014034A Pending JPS58131707A (en) 1982-01-30 1982-01-30 Polarized electromagnet device

Country Status (1)

Country Link
JP (1) JPS58131707A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4941234A (en) * 1988-09-22 1990-07-17 Yoshida Kogyo K. K. Button collet

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4941234A (en) * 1988-09-22 1990-07-17 Yoshida Kogyo K. K. Button collet

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