JPS6317211B2 - - Google Patents

Info

Publication number
JPS6317211B2
JPS6317211B2 JP14853179A JP14853179A JPS6317211B2 JP S6317211 B2 JPS6317211 B2 JP S6317211B2 JP 14853179 A JP14853179 A JP 14853179A JP 14853179 A JP14853179 A JP 14853179A JP S6317211 B2 JPS6317211 B2 JP S6317211B2
Authority
JP
Japan
Prior art keywords
cylindrical
permanent magnets
excitation coil
magnetic pole
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
Application number
JP14853179A
Other languages
Japanese (ja)
Other versions
JPS5670612A (en
Inventor
Yoshio Takase
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 JP14853179A priority Critical patent/JPS5670612A/en
Publication of JPS5670612A publication Critical patent/JPS5670612A/en
Publication of JPS6317211B2 publication Critical patent/JPS6317211B2/ja
Granted legal-status Critical Current

Links

Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00—Magnets
    • H01F7/06—Electromagnets; Actuators including electromagnets
    • H01F7/08—Electromagnets; Actuators including electromagnets with armatures
    • H01F7/14—Pivoting armatures
    • H01F7/145—Rotary electromagnets with variable gap

Landscapes

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

Description

【発明の詳細な説明】 本発明は往復回転動作型回転電磁石に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a reciprocating rotating electromagnet.

従来この種の回転電磁石として第3図a,bに
示すように薄鉄板を積層し形成した筒状鉄芯10
の内周面に対向して設けられた突極11に励磁コ
イル12を巻装し、その突極11が互いに異磁極
に励磁されるようにしたステータSと直径方向に
磁化された筒状永久磁石13が出力軸4の中央部
に挿着されたロータRとよりなり、永久磁石13
とステータS内に嵌挿した状態でロータRを回転
自在軸受7に挿着したものがあり、励磁コイル1
2に電流を流すことによりステータSの両突極1
1がそれぞれ異磁極に励磁され、ロータRの永久
磁石13の両磁極がそれぞれ突極11に吸引され
てロータRが回転するようになつており、ロータ
Rの回転方向は励磁コイル12に流す電流の方向
により選択できるようになつていた。しかしなが
らこのような従来例にあつては複雑な形状の鉄芯
10が必要であり、しかも突極11に励磁コイル
12を巻装する作業が煩わしく、製造工程が複雑
化するとともに高コストになるという欠点をもつ
ていた。また動作角を変えるにはステータSの鉄
芯形状を変更する必要があり、容易に動作角の変
更ができないので、ストツパー14を用いて適宜
動作角を設定するようになつていたが、回転動作
時にストツパー14に衝撃が加わり機械的寿命が
短かくなるとともに、安定位置でのハウリングが
生じるという欠点をもつていた。一方小型の回転
電磁石においては鉄芯の加工および励磁コイルの
巻線作業が困難になるので、コアレス励磁コイル
を用いてステータSを構成していたが鉄芯を用い
た励磁コイルに比べて励磁コイル12間の磁束密
度が大巾に小さくなり、ステータSによるロータ
Rの吸引力が小さくなるので、出力軸4の回転ト
ルクが減少し出力効率が悪くなるという欠点をも
つていた。本発明は上記の欠点を解決することを
目的とするものである。
Conventionally, as this type of rotating electromagnet, there is a cylindrical iron core 10 formed by laminating thin iron plates as shown in FIGS. 3a and 3b.
A stator S has an exciting coil 12 wound around a salient pole 11 provided facing the inner circumferential surface of the stator S so that the salient poles 11 are mutually excited to different magnetic poles, and a cylindrical permanent magnet magnetized in the diametrical direction. The magnet 13 consists of a rotor R inserted into the center of the output shaft 4, and the permanent magnet 13
There is one in which the rotor R is inserted into the rotatable bearing 7 while being inserted into the stator S, and the excitation coil 1
By passing current through 2, both salient poles 1 of the stator S
1 are excited to have different magnetic poles, and both magnetic poles of the permanent magnets 13 of the rotor R are each attracted to the salient poles 11, so that the rotor R rotates, and the direction of rotation of the rotor R is determined by the current flowing through the excitation coil 12. It was possible to select depending on the direction. However, in such a conventional example, an iron core 10 with a complicated shape is required, and the work of winding the excitation coil 12 around the salient pole 11 is troublesome, which complicates the manufacturing process and increases costs. It had its drawbacks. In addition, in order to change the operating angle, it is necessary to change the iron core shape of the stator S, and since the operating angle cannot be easily changed, the operating angle has been set appropriately using a stopper 14. At times, impact is applied to the stopper 14, shortening its mechanical life, and it also has the disadvantage of causing howling at a stable position. On the other hand, with small rotating electromagnets, it is difficult to process the iron core and wind the excitation coil, so the stator S was constructed using a coreless excitation coil. Since the magnetic flux density between the output shafts 12 and 12 is greatly reduced, and the attraction force of the rotor R by the stator S is reduced, the rotational torque of the output shaft 4 is reduced, resulting in poor output efficiency. The present invention aims to solve the above-mentioned drawbacks.

以下実施例について図を用いて説明する。第1
図および第2図は本発明の一実施例を示すもの
で、内周面に異磁極が交互に着磁された筒状永久
磁石1a,1bを磁性材よりなる筒状ケース3の
両端部に嵌挿するとともに筒状励磁コイル2を両
永久磁石1a,1b間に中心を一致させて配設す
ることによりステータSを形成し、筒状ケース3
の中心に回転自在に挿通した出力軸4に挿着固定
された筒状鉄芯5を励磁コイル2に内挿し、この
鉄芯5の両端部よりそれぞれ両永久磁石1a,1
bの内周面の各同磁極面に適当間隔をもつて対向
する磁極片6a,6bを突設することによりロー
タRを形成したものである。図中7は含油合金あ
るいはボールベアリングなどよりなる軸受、8は
ロータRの回転をスムースにするためのスラスト
ワツシヤで潤滑性のある非磁性体で形成されてい
る。なお筒状永久磁石1a,1bとしてフエライ
ト焼結成形品あるいは帯状のゴム磁石を環状に成
形したものを用いてもよく、実施例にあつては筒
状永久磁石1a,1bの4箇所を半径方向に着磁
し、相隣接する着磁箇所の着磁方向を互いに逆向
きとすることにより内周面の4箇所に異磁極が交
互に形成されているが、着磁箇所は4箇所に限定
されるものではなく、偶数箇所であれば良いもの
であり、また磁極片6a,6bの個数は永久磁石
1a,1bの同磁極面に対応するものであるから
着磁箇所の1/2となる。
Examples will be described below using figures. 1st
Figures 1 and 2 show an embodiment of the present invention, in which cylindrical permanent magnets 1a and 1b, whose inner circumferences are alternately magnetized with different magnetic poles, are attached to both ends of a cylindrical case 3 made of a magnetic material. The stator S is formed by fitting and arranging the cylindrical excitation coil 2 between both permanent magnets 1a and 1b with their centers coincident, and the cylindrical case 3
A cylindrical iron core 5 inserted and fixed to an output shaft 4 rotatably inserted through the center of the excitation coil 2 is inserted into the excitation coil 2, and both permanent magnets 1a, 1 are inserted from both ends of the iron core 5, respectively.
The rotor R is formed by protruding magnetic pole pieces 6a and 6b facing each other at an appropriate distance from each of the same magnetic pole faces on the inner circumferential surface of the rotor b. In the figure, 7 is a bearing made of an oil-impregnated alloy or a ball bearing, and 8 is a thrust washer for smoothing the rotation of the rotor R, which is made of a lubricating non-magnetic material. As the cylindrical permanent magnets 1a and 1b, sintered ferrite molded products or band-shaped rubber magnets formed into an annular shape may be used. Different magnetic poles are formed alternately at four locations on the inner circumferential surface by magnetizing adjacent magnetized locations in opposite directions, but the number of magnetized locations is limited to four locations. The number of magnetic pole pieces 6a, 6b corresponds to the same magnetic pole surface of the permanent magnets 1a, 1b, so the number of magnetic pole pieces 6a, 6b is 1/2 of the number of magnetized positions.

以下実施例の動作について説明する。いま実施
例において左右対称構造になつているので左側部
分の動作について説明すると、励磁コイル2に電
流が流れていない場合、鉄芯5は磁化されず鉄芯
5の端部に突設した極磁片6aは単なる磁性体片
として作用することになり、磁極片6aは第2図
aに示すように永久磁石1aの内周面の異磁極間
の磁気抵抗が最も小さくなる位置すなわち異磁極
間の中央で安定している。次に鉄芯5の永久磁石
1aがわ端部がN極となるように励磁コイル2に
電流が流れると、両磁極片6aがN極となり、両
磁極片6aはそれぞれ永久磁石1aのS極に吸引
されて矢印Aの方向に略45゜回動して第2図bに
示す位置で安定し、一方励磁コイル2に流す電流
の方向を逆転することにより、両磁極片6aはS
極となり永久磁石1aのN極に吸引されて矢印B
の方向に略45゜回動して第2図cに示す位置にて
安定するようになつている。なお励磁コイル2に
流れる電流をしや断すればロータRは第2図aに
示す位置に自己復帰することになるが、渦巻きば
ねなどを用いて自己復帰を確実にするように構成
しても良い。ところで励磁コイル2の右側部分に
おいても以上の動作と全く同様の動作が行なわれ
ることになり、出力軸4から両部分にて発生する
回転トルクが加え合わされて得られるようになつ
ている。なお左右の永久磁石1a,1bおよび磁
極片6a,6bの形状、配置を適宜変更すること
により種々の出力特性の回転電磁石が得られるこ
とになる。
The operation of the embodiment will be explained below. Since the present embodiment has a symmetrical structure, the operation of the left side part will be explained. When no current flows through the excitation coil 2, the iron core 5 is not magnetized and the pole magnet protruding from the end of the iron core 5. The piece 6a acts as a mere magnetic piece, and the magnetic pole piece 6a is located at the position where the magnetic resistance between the different magnetic poles on the inner peripheral surface of the permanent magnet 1a is the smallest, that is, between the different magnetic poles, as shown in FIG. 2a. Stable in the center. Next, when current flows through the excitation coil 2 so that the end of the iron core 5 near the permanent magnet 1a becomes the north pole, both magnetic pole pieces 6a become the north pole, and both magnetic pole pieces 6a become the south pole of the permanent magnet 1a. is attracted by the magnet, rotates approximately 45 degrees in the direction of arrow A, and stabilizes at the position shown in FIG.
It becomes a pole and is attracted to the N pole of the permanent magnet 1a, and the arrow B
It is designed to rotate approximately 45 degrees in the direction of , and stabilize at the position shown in FIG. 2c. Note that if the current flowing through the excitation coil 2 is suddenly cut off, the rotor R will self-return to the position shown in Fig. 2a, but even if a spiral spring or the like is used to ensure self-return. good. Incidentally, the same operation as described above is performed on the right side portion of the excitation coil 2, and the rotational torque generated in both portions from the output shaft 4 is obtained by adding them together. Note that by appropriately changing the shape and arrangement of the left and right permanent magnets 1a, 1b and the magnetic pole pieces 6a, 6b, rotating electromagnets with various output characteristics can be obtained.

本発明は上述のよう磁性材よりなる筒状ケース
の両端部に嵌挿され、内周面に異磁極が交互に着
磁された筒状永久磁石にてステータを形成し、両
端部に両永久磁石の内周面の同磁極に適宜間隔を
もつて対向する磁極片をそれぞれ突設した円筒状
鉄芯を両永久磁石間に装着した筒状励磁コイルに
内挿することによりロータを形成しており、鉄芯
の形状が簡単であり、しかも励磁コイルとしてコ
アレスコイルを用いているので従来例のように励
磁コイルの巻装作業が煩わしいということがな
く、製造が容易であるという利点をもつており、
また永久磁石の着磁箇所を適宜設定することによ
り、往復回転動作時において任意の動作角を得る
ことができ、従来例のように動作角を設定するス
トツパーを必要としないので、構造が簡単になる
とともにストツパーを設けたことによる機械的寿
命の短縮、あるいはハウリングの発生など不都合
が起きないものである。また鉄芯の両端部に突設
した磁極片と筒状ケースの両端部に嵌挿した永久
磁石により回転トルクを得るようになつているの
で、出力効率が良くなるという利点をもつている
ものである。
As described above, the present invention forms a stator with cylindrical permanent magnets that are fitted into both ends of a cylindrical case made of a magnetic material and have different magnetic poles alternately magnetized on the inner circumferential surface. A rotor is formed by inserting a cylindrical iron core with protruding magnetic pole pieces facing the same magnetic pole on the inner peripheral surface of the magnet at appropriate intervals into a cylindrical excitation coil installed between both permanent magnets. The iron core has a simple shape, and since a coreless coil is used as the excitation coil, there is no need to wind the excitation coil as in the conventional case, and it has the advantage of being easy to manufacture. Ori,
In addition, by appropriately setting the magnetized point of the permanent magnet, any operating angle can be obtained during reciprocating rotation, and unlike conventional examples, there is no need for a stopper to set the operating angle, resulting in a simpler structure. At the same time, problems such as shortening of mechanical life and occurrence of howling due to the provision of the stopper do not occur. In addition, since rotational torque is obtained by magnetic pole pieces protruding from both ends of the iron core and permanent magnets inserted into both ends of the cylindrical case, it has the advantage of improved output efficiency. be.

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

第1図は本発明一実施例の断面図、第2図a〜
cは第1図のX−X線断面図にて示す動作説明
図、第3図aは従来例の断面図第3図bは同上の
Y−Y線断面図である。 1a,1bは永久磁石、2は励磁コイル、3は
筒状ケース、4は出力軸、5は鉄芯、6a,6b
は磁極片である。
Fig. 1 is a sectional view of one embodiment of the present invention, Fig. 2 a~
3c is an explanatory diagram of the operation shown in a sectional view taken along the line X--X of FIG. 1, FIG. 3a is a sectional view of the conventional example, and FIG. 3b is a sectional view taken along the Y-Y line of the same. 1a and 1b are permanent magnets, 2 is an exciting coil, 3 is a cylindrical case, 4 is an output shaft, 5 is an iron core, 6a, 6b
is a magnetic pole piece.

Claims (1)

【特許請求の範囲】[Claims] 1 内周面に異磁極が交互に着磁された筒状永久
磁石を磁性材よりなる筒状ケースの両端部に嵌挿
するとともに筒状励磁コイルを両永久磁石間に中
心を一致させて配設し、筒状ケースの中心に回転
自在に挿通した出力軸に挿着固定された筒状鉄芯
を励磁コイルに内挿し、上記鉄芯の両端部よりそ
れぞれ両永久磁石の内周面の同磁極面に適当間隔
をもつて対向する磁極片を突設したことを特徴と
する回転電磁石。
1 Cylindrical permanent magnets with different magnetic poles alternately magnetized on the inner circumferential surface are inserted into both ends of a cylindrical case made of a magnetic material, and a cylindrical excitation coil is arranged between both permanent magnets with their centers aligned. A cylindrical iron core inserted and fixed to an output shaft rotatably inserted through the center of a cylindrical case is inserted into the excitation coil, and the inner peripheral surfaces of both permanent magnets are A rotating electromagnet characterized by having opposing magnetic pole pieces protruding from the magnetic pole face at an appropriate interval.
JP14853179A 1979-11-15 1979-11-15 Rotary electromagnet Granted JPS5670612A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14853179A JPS5670612A (en) 1979-11-15 1979-11-15 Rotary electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14853179A JPS5670612A (en) 1979-11-15 1979-11-15 Rotary electromagnet

Publications (2)

Publication Number Publication Date
JPS5670612A JPS5670612A (en) 1981-06-12
JPS6317211B2 true JPS6317211B2 (en) 1988-04-13

Family

ID=15454860

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14853179A Granted JPS5670612A (en) 1979-11-15 1979-11-15 Rotary electromagnet

Country Status (1)

Country Link
JP (1) JPS5670612A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62131414U (en) * 1986-02-13 1987-08-19
JP2005286283A (en) * 2004-03-30 2005-10-13 Toshiaki Miyasaka Rotary solenoid

Also Published As

Publication number Publication date
JPS5670612A (en) 1981-06-12

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