JPH0423403B2 - - Google Patents
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- Publication number
- JPH0423403B2 JPH0423403B2 JP61115440A JP11544086A JPH0423403B2 JP H0423403 B2 JPH0423403 B2 JP H0423403B2 JP 61115440 A JP61115440 A JP 61115440A JP 11544086 A JP11544086 A JP 11544086A JP H0423403 B2 JPH0423403 B2 JP H0423403B2
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- Prior art keywords
- magnetic
- permanent magnet
- iron core
- core
- magnetic pole
- Prior art date
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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、機械的安定状態の保持および該機械
的安定状態からの変位を電磁的に操作する装置、
例えば、電磁施錠装置、弁棒操作装置、電磁継電
器、電磁クラツチ等に用いられる電磁アクチユエ
ータに関する。Detailed Description of the Invention [Field of Industrial Application] The present invention relates to a device for electromagnetically manipulating the maintenance of a mechanically stable state and displacement from the mechanically stable state;
For example, the present invention relates to electromagnetic actuators used in electromagnetic locking devices, valve stem operating devices, electromagnetic relays, electromagnetic clutches, and the like.
従来、PCT/JP84/00084、PCT/JP85/
00313、PCT/JP85/00314、PCT/JP85/
00536において本発明者は微小電流で大きな推力
を発生する電磁アクチユエータを提案した。
Previously, PCT/JP84/00084, PCT/JP85/
00313, PCT/JP85/00314, PCT/JP85/
In 00536, the present inventor proposed an electromagnetic actuator that generates a large thrust with a small current.
この電磁アクチユエータは第6図に示されるよ
うに固定鉄心1と、該固定鉄心1に対して矢印1
4aまたは14b方向に変移する可動鉄心2と、
通電時に該可動鉄心2に第1の磁束8を作用させ
るように巻回された電気巻線4と、該第1の磁束
8に第2の磁束9を分流させ、並列に作用させる
ように該固定鉄心1に設けられた永久磁石5とか
ら成るものである。 As shown in FIG. 6, this electromagnetic actuator has a fixed iron core 1 and an arrow mark
A movable iron core 2 that moves in the direction 4a or 14b,
An electric winding 4 is wound so that a first magnetic flux 8 acts on the movable iron core 2 when energized, and a second magnetic flux 9 is divided into the first magnetic flux 8 and applied in parallel. It consists of a permanent magnet 5 provided on a fixed iron core 1.
しかし、上述の従来装置は永久磁石による第2
の磁束の左右の分流比を所要範囲に限定する手段
を設けていないため、必ずしも高感度の特性を得
ることができないという問題点があつた。
However, the above-mentioned conventional device uses a permanent magnet to
Since there is no means for limiting the left and right branching ratio of the magnetic flux to a required range, there is a problem in that highly sensitive characteristics cannot necessarily be obtained.
そこで、本発明は上述の問題点を解決するため
に提案されたもので、より高感度の特性を有し、
微電流で大きな推力を発生する電磁アクチユエー
タを提供することを目的とする。 Therefore, the present invention was proposed to solve the above-mentioned problems, and has characteristics of higher sensitivity.
The purpose of this invention is to provide an electromagnetic actuator that generates a large thrust with a small current.
まず、第1図aを参照して本発明の原理を説明
する。
First, the principle of the present invention will be explained with reference to FIG. 1a.
永久磁石5による磁束9の左側の固定鉄心1へ
の分流をφma、右側の固定鉄心1への分流を
φmbとし、電気巻線4の通電による磁束8をφi
とする。 The shunt of the magnetic flux 9 caused by the permanent magnet 5 to the left fixed iron core 1 is φma, the shunt to the right fixed iron core 1 is φmb, and the magnetic flux 8 caused by energization of the electric winding 4 is φi.
shall be.
ここで、φiとφmbが同一方向に作用した場合、
可動鉄心2と左右各々の固定鉄心1との間の吸引
力Fa、Fbは次式で示される。 Here, if φi and φmb act in the same direction,
The attraction forces Fa and Fb between the movable iron core 2 and the left and right fixed iron cores 1 are expressed by the following equations.
Fa=K(φi−φma)2 ……(1)
Fb=K(φi+φmb)2 ……(2)
ここで、可動鉄心2の磁極面2a,2と、左右
の各々の固定鉄心1の磁極面1a,1bとの間隙
長を各々d1、d2および永久磁石5の磁極面5aと
の間隙長Δ、各磁極面の面積をS、間隙の透磁率
をμ、電気巻線4の通電電流をI、永久磁石5の
起磁力をHp、比例定数をKとする。 Fa=K(φi−φma) 2 ...(1) Fb=K(φi+φmb) 2 ...(2) Here, the magnetic pole faces 2a, 2 of the movable core 2 and the magnetic pole faces of the left and right fixed cores 1 1a and 1b respectively, the gap length Δ between the permanent magnet 5 and the magnetic pole surface 5a , the area of each magnetic pole surface S, the magnetic permeability of the gap μ, and the current flowing through the electric winding 4. is I, the magnetomotive force of the permanent magnet 5 is Hp, and the proportionality constant is K.
ここで、単純化するため、磁路を形成する磁性
体の磁気抵抗、および、漏洩磁束を無視すれば、
φi=N・I・μ・S/(d1+d2) ……(3)
φma=Hp・μ・S/(d1+Δ) ……(4)
φmb=Hp・μ・S/(d2+Δ) ……(5)
となる。 Here, for simplicity, if we ignore the magnetic resistance of the magnetic material forming the magnetic path and the leakage magnetic flux, we get φi=N・I・μ・S/(d 1 + d 2 )...(3) φma =Hp・μ・S/(d 1 +Δ) ...(4) φmb=Hp・μ・S/(d 2 +Δ) ...(5)
ここで電気巻線4の通電時に可動鉄心2に作用
する実効力をFtとすると、
Ft=Fb−Fa=
K{N・I・μ・S/(d1+d2)}2
×〔2(Hp/N・I)×{(d1+d2)/(d1+Δ)
+(d1+d2)/(d2+Δ)}
−{(d1+d2)/(d1+Δ)}2
−{(d1+d2)/(d2+Δ)}2(Hp/N・I)2〕
……(6)
ここで、本発明装置と同一形状、寸法の従来装
置のの可動鉄心2に作用する電磁力をFc、スプ
リングにより可動鉄心2に作用する抗力をFsと
すれば、周知のように電気巻線4通電時に可動鉄
心2に作用する実効力Foは、
Fo=Fc−Fs=K{(N・I・μ・S/(d1
+d2)}2−Fs ……(7)となる。 Here, if the effective force acting on the movable iron core 2 when the electric winding 4 is energized is Ft, then Ft = Fb - Fa = K{N・I・μ・S/(d 1 + d 2 )} 2 × [2( Hp / N.I ) _ _ _ _ _ _ −{(d 1 + d 2 )/(d 2 +Δ)} 2 (Hp/N・I) 2 ]
...(6) Here, if the electromagnetic force acting on the movable core 2 of the conventional device having the same shape and dimensions as the device of the present invention is Fc, and the drag force acting on the movable core 2 due to the spring is Fs, then as is well known, The effective force Fo acting on the movable iron core 2 when the electric winding 4 is energized is Fo = Fc - Fs = K {(N・I・μ・S/(d 1 + d 2 )} 2 −Fs ……(7) becomes.
ここで、単純化のためにFsを無視し、(6)式と
(7)式の比を求めれば、
Ft/Fo≒{A(Hp/N・I)2
+2B(Hp/N・I)} ……(8)
A={(d1+d2)/(d1+Δ)}2
−{(d1+d2)/(d2+Δ)}2 ……(9)
B=(d1+d2)/(d1+Δ)
+(d1+d2)/(d2+Δ) ……(10)
を得ることができる。 Here, for the sake of simplicity, we ignore Fs and use equation (6) as
If we find the ratio of equation (7), we get Ft/Fo≒{A(Hp/N・I) 2 +2B(Hp/N・I)}...(8) A={(d 1 +d 2 )/(d 1 + Δ)} 2 − {(d 1 + d 2 )/(d 2 + Δ)} 2 ...(9) B=(d 1 + d 2 )/(d 1 + Δ) + (d 1 + d 2 )/(d 2 + Δ) ...(10) can be obtained.
ここで、以上の関係をHp/N・Iをパラメー
タとして、(d1+Δ)/(d1+d2)の変化で、
Ft/Foをグラフにて求めると第5図に示される
ようになる。 Here, the above relationship is changed by changing (d 1 + Δ)/(d 1 + d 2 ) with Hp/N・I as a parameter,
When Ft/Fo is calculated graphically, it is shown in Figure 5.
この第5図から本発明装置は該電気巻線通電
時、(d1+Δ)/(d1+d2)の数値が0.2以上1.0以
下の範囲で、かつ、Hp/N・Iの数値が0.2以上
2.0以下の場合高感度の特性を得ることができる
を知見した。 As shown in FIG. 5, when the electric winding is energized, the device of the present invention has a value of (d 1 +Δ)/(d 1 +d 2 ) in the range of 0.2 or more and 1.0 or less, and a value of Hp/N·I of 0.2. that's all
It was found that high sensitivity characteristics can be obtained when the value is 2.0 or less.
次に、(6)式を変形すると、 Ft=K{μ・S/(d1+d2)}2(2B ・Hp・N・I−A・Hp2) ……(11) となる。 Next, when formula (6) is transformed, it becomes Ft=K{μ・S/(d 1 +d 2 )} 2 (2B・Hp・N・I−A・Hp 2 ) (11).
ここで、K、μ、S、d1+d2、Hp、Nを設計
上設定すれば、実効力は電流Iに比例し、しか
も、ある電流値で動作する電磁アクチユエータを
製作できるので、過電流継電器の瞬時引き外し装
置等に応用できる。 Here, if K, μ, S, d 1 + d 2 , Hp, and N are set in the design, the effective force is proportional to the current I, and since it is possible to manufacture an electromagnetic actuator that operates at a certain current value, the overcurrent It can be applied to instantaneous tripping devices for relays, etc.
本発明は上述の知見に基づいて成立するもの
で、固定鉄心と、該固定鉄心に対して変移する可
動鉄心と、通電時に該可動鉄心に第1の磁束を作
用させるように巻回された電気巻線と、該第1の
磁束に第2の磁束を並列に分流させて作用させる
ように該固定鉄心または該可動鉄心に設けた永久
磁石とから成る電磁アクチユエータを改良するも
ので、
該可動鉄心の一方の端面側磁極面から対面する
該固定鉄心の磁極面間の磁気抵抗値および該可動
鉄心の側面側磁極面から該永久磁石の磁極面間の
磁気抵抗値の和と、該可動鉄心の両端面側磁極面
から各々対面する該固定鉄心の磁極面間の磁気抵
抗値の和との比が0.2以上1.0以下で、かつ、該永
久磁石起磁力と、該電気巻線の通電による起磁力
の比が0.2以上2.0以下とする手段を設けることを
特徴とする電磁アクチユエータである。 The present invention was established based on the above-mentioned knowledge, and includes a fixed iron core, a movable iron core that moves with respect to the fixed iron core, and an electric wire wound so as to apply a first magnetic flux to the movable iron core when energized. This is an improvement to an electromagnetic actuator comprising a winding and a permanent magnet provided on the fixed iron core or the movable iron core so that a second magnetic flux is shunted in parallel to the first magnetic flux, and the permanent magnet is provided on the fixed iron core or the movable iron core. The sum of the magnetic resistance value between the magnetic pole surfaces of the fixed core facing from one end side magnetic pole surface of the movable iron core and the magnetic resistance value between the side magnetic pole surface of the movable iron core and the magnetic pole surface of the permanent magnet, and The ratio of the sum of the magnetic resistance values between the magnetic pole surfaces of the fixed iron core facing each other from the magnetic pole surfaces on both end faces is 0.2 or more and 1.0 or less, and the magnetomotive force of the permanent magnet and the magnetomotive force due to energization of the electric winding. The electromagnetic actuator is characterized in that it is provided with means for setting the ratio of 0.2 to 2.0.
〔作用〕
本発明によれば、可動鉄心の一方の端面側磁極
面から対面する固定鉄心の磁極面間の磁気抵抗値
および該可動鉄心の側面側磁極面から該永久磁石
の磁極面間の磁気抵抗値の和と、該可動鉄心の両
端面側磁極面から各々対面する該固定鉄心の磁極
面間の磁気抵抗値の和との比が0.2以上1.0以下
で、かつ、該永久磁石起磁力と、該電気巻線通電
による起磁力の比が0.2以上2.0以下とする手段を
設けるため、常に高特性の特性を得る。[Function] According to the present invention, the magnetic resistance value between the magnetic pole faces of the fixed iron facing from one end side magnetic pole face of the movable iron core, and the magnetic resistance between the side magnetic pole face of the movable iron core and the magnetic pole face of the permanent magnet. The ratio of the sum of the resistance values to the sum of the magnetic resistance values between the magnetic pole surfaces of the fixed iron core facing each other from the magnetic pole surfaces on both end surfaces of the movable iron core is 0.2 or more and 1.0 or less, and the magnetomotive force of the permanent magnet Since a means is provided to ensure that the ratio of magnetomotive force due to energization of the electric winding is 0.2 or more and 2.0 or less, high characteristics are always obtained.
このため、常に微電力で大きな推力を発生す
る。 Therefore, a large thrust is always generated with a small amount of electric power.
以下、本発明を図面を参照してその実施例に基
づいて説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below based on embodiments with reference to the drawings.
第1図a,b,cは本発明の第1の実施例の説
明図である。 FIGS. 1a, b, and c are explanatory diagrams of a first embodiment of the present invention.
本実施例は固定鉄心1と、該固定鉄心1に対し
て変移する可動鉄心2と、通電時に該可動鉄心2
に第1の磁束8を作用させるように巻回された電
気巻線4と、第1の磁束8に第2の磁束9を並列
に分流させて作用させるように固定鉄心1または
可動鉄心2に設けた永久磁石5とから成る。 This embodiment includes a fixed core 1, a movable core 2 that moves relative to the fixed core 1, and a movable core 2 that moves when energized.
The electric winding 4 is wound so that the first magnetic flux 8 acts on the fixed iron core 1 or the movable iron core 2 so that the second magnetic flux 9 is shunted and applied in parallel to the first magnetic flux 8. It consists of a permanent magnet 5 provided.
さらに、可動鉄心2の一方の端面側磁極面2a
または2bから対面する固定鉄心1の磁極面1a
または1b間の磁気抵抗値および可動鉄心2の側
面側磁極面2cから永久磁石5の磁極面5a間の
磁気抵抗値の和と、可動鉄心2の両端面側磁極面
2a,2bから各々対面する固定鉄心1の磁極面
1a,1b間の磁気抵抗値の和との比が0.2以上
1.0以下とする手段であるスプリング3を可動鉄
心2の両側に配設する。 Furthermore, one end face side magnetic pole face 2a of the movable iron core 2
Or magnetic pole face 1a of fixed iron core 1 facing from 2b
Or, the sum of the magnetic resistance value between 1b and the magnetic resistance value between the side magnetic pole surface 2c of the movable core 2 and the magnetic pole surface 5a of the permanent magnet 5, and the magnetic resistance value between the magnetic pole surfaces 2a and 2b on both end surfaces of the movable core 2, respectively. The ratio of the sum of the magnetic resistance values between the magnetic pole faces 1a and 1b of the fixed iron core 1 is 0.2 or more
Springs 3 are provided on both sides of the movable iron core 2 as a means for keeping the value to 1.0 or less.
これにより、永久磁石5の磁束9の分流比が所
範囲に限定される。 Thereby, the division ratio of the magnetic flux 9 of the permanent magnet 5 is limited to a predetermined range.
さらに、永久磁石5の起磁力と、電気巻線4の
通電による起磁力の比が0.2以上2.0以下とする手
段として電気巻線4の巻数を調整する。 Furthermore, the number of turns of the electric winding 4 is adjusted as a means for making the ratio of the magnetomotive force of the permanent magnet 5 and the magnetomotive force caused by energization of the electric winding 4 to be 0.2 or more and 2.0 or less.
あるいは永久磁石5の起磁力が所要のものを用
いてもよい。 Alternatively, a permanent magnet 5 having a required magnetomotive force may be used.
本実施例は、三位置安定で高感度電磁アクチユ
エータとし適用できる。 This embodiment can be applied as a three-position stable and highly sensitive electromagnetic actuator.
次に、本発明の第2の実施例を第2図を参照し
て説明する。 Next, a second embodiment of the present invention will be described with reference to FIG.
永久磁石5による第2の磁束9の左右の分流比
を所要範囲に限定する手段は可動鉄心2の片方の
スプリング3と反対側の非磁性体6aとにより構
成される。 A means for limiting the left and right branching ratio of the second magnetic flux 9 by the permanent magnet 5 to a required range is constituted by the spring 3 on one side of the movable iron core 2 and the non-magnetic body 6a on the opposite side.
永久磁石5は非磁性体6aに接触し、可動鉄心
2は非磁性体6aに対して接離する。 The permanent magnet 5 contacts the non-magnetic material 6a, and the movable iron core 2 moves toward and away from the non-magnetic material 6a.
次に、本発明の第3の実施例を第3図を参照し
て説明する。 Next, a third embodiment of the present invention will be described with reference to FIG.
第2図の実施例と同様に、永久磁石5による第
2の磁束9の左右の分流比を所要範囲に限定する
手段は可動鉄心2の片方のスプリング3と反対側
の非磁性体6bとにより構成される。 Similar to the embodiment shown in FIG. 2, the means for limiting the left and right branching ratio of the second magnetic flux 9 by the permanent magnet 5 to a required range is provided by the spring 3 on one side of the movable iron core 2 and the non-magnetic body 6b on the opposite side. configured.
永久磁石5は非磁性体6bとは接触せずに、離
隔して配設されるのでラツチング特性を得やす
い。 Since the permanent magnet 5 is placed apart from the non-magnetic material 6b without contacting it, it is easy to obtain a latching characteristic.
第4図a,b,c,dは、本実施例の永久磁石
磁極面の模式構造図である。 FIGS. 4a, b, c, and d are schematic structural diagrams of the permanent magnet pole faces of this embodiment.
第2図、第3図の実施例と同様に永久磁石5の
周期には磁性体は配設されていない。 Similar to the embodiments shown in FIGS. 2 and 3, no magnetic material is arranged in the period of the permanent magnet 5.
第4図aは第1図の実施例の永久磁石5の説明
図で、永久磁石5の周囲には磁性体は配設されて
いない。 FIG. 4a is an explanatory diagram of the permanent magnet 5 of the embodiment shown in FIG. 1, and no magnetic material is arranged around the permanent magnet 5. FIG.
これに対して第4図bの実施例では永久磁石5
の全面に磁性体7aを接して配設される。 On the other hand, in the embodiment shown in FIG. 4b, the permanent magnet 5
The magnetic material 7a is placed in contact with the entire surface of the magnetic material 7a.
第4図cの実施例では永久磁石5の両側面に接
して磁性体7bが配設される。 In the embodiment shown in FIG. 4c, magnetic bodies 7b are disposed in contact with both side surfaces of the permanent magnet 5.
第4図dの実施例では永久磁石5と所要間隙を
介して磁性体7cが配設される。 In the embodiment shown in FIG. 4d, a magnetic body 7c is disposed with a required gap between the permanent magnet 5 and the magnetic body 7c.
従つて、永久磁石5の磁束9の一部分または大
部分は、磁性体7a,7b,7cに分流し、ラツ
チング保磁力を減少させる。 Therefore, a part or most of the magnetic flux 9 of the permanent magnet 5 is shunted to the magnetic bodies 7a, 7b, and 7c, reducing the latching coercive force.
特に、第4図bの実施例では保磁力は消去し、
通電時動作、停電時スプリング力による復帰特性
を有する。 In particular, in the embodiment of FIG. 4b, the coercive force disappears,
It operates when the power is turned on, and has a spring force recovery characteristic when the power goes out.
さらに、ソレノイド通電による磁束8も磁性体
7a,7b,7cに分流し、永久磁石5の磁束を
相殺する方向に作用するため、高感度特性を発揮
する。 Furthermore, the magnetic flux 8 caused by the energization of the solenoid is also shunted to the magnetic bodies 7a, 7b, and 7c, acting in a direction that cancels out the magnetic flux of the permanent magnet 5, thereby exhibiting high sensitivity characteristics.
本発明は以上説明したように、磁気回路におけ
る磁気抵抗値および永久磁石および電磁石起磁力
を所要範囲に限定する手段を設けるため、常に高
特性の特性を得る。
As described above, the present invention provides means for limiting the magnetic resistance value and the magnetomotive force of the permanent magnets and electromagnets in the magnetic circuit to the required ranges, so that high characteristics are always obtained.
このため、常に微電流で大きな推力を発生する
という効果を奏する。 Therefore, it is possible to always generate a large thrust with a small current.
第1図a,b,cは本発明の第1の実施例の説
明図、第2図は本発明の第2の実施例の説明図、
第3図は本発明の第3の実施例の説明図、第4図
a,b,c,dは本実施例を構成する永久磁石の
取付状態説明図、第5図は電磁アクチユエータの
特性説明図、第6図は従来装置の説明図である。
1……固定鉄心、2……可動鉄心、3……スプ
リング、4……電気巻線、5……永久磁石、6
a,6b……非磁性体、7a,7b,7c……磁
性体、8……第1の磁束、9……第2の磁束。
Figures 1a, b, and c are explanatory diagrams of the first embodiment of the present invention, and Figure 2 is an explanatory diagram of the second embodiment of the present invention.
Fig. 3 is an explanatory diagram of the third embodiment of the present invention, Fig. 4 a, b, c, and d are explanatory diagrams of the installation state of the permanent magnets constituting this embodiment, and Fig. 5 is an explanation of the characteristics of the electromagnetic actuator. 6 are explanatory diagrams of a conventional device. 1... Fixed iron core, 2... Movable iron core, 3... Spring, 4... Electric winding, 5... Permanent magnet, 6
a, 6b...Nonmagnetic material, 7a, 7b, 7c...Magnetic material, 8...First magnetic flux, 9...Second magnetic flux.
Claims (1)
動鉄心と、通電時に該可動鉄心に第1の磁束を作
用させるように巻回された電気巻線と、該第1の
磁束に第2の磁束を並列に分流させて作用させる
ように該固定鉄心または該可動鉄心に設けた永久
磁石とから成る電磁アクチユエータにおいて、 該可動鉄心の一方の端面側磁極面から対面する
該固定鉄心の磁極面間の磁気抵抗値および該可動
鉄心の側面磁極面から該永久磁石の磁極面間の磁
気抵抗値の和と、該可動鉄心の両端面側磁極面か
ら各々対面する該固定鉄心の磁極面間の磁気抵抗
値の和との比が0.2以上1.0以下で、かつ、該永久
磁石起磁力と、該電気巻線の通電による起磁力の
比が0.2以上2.0以下とする手段を設けることを特
徴とする電磁アクチユエータ。 2 該永久磁石の全面に磁性体を接して配設した
特許請求の範囲第1項記載の電磁アクチユエー
タ。 3 該永久磁石の両側面に接して磁性体を配設し
た特許請求の範囲第1項記載の電磁アクチユエー
タ。 4 該永久磁石と所要間隙を介して磁性体を配設
した特許請求の範囲第1項記載の電磁アクチユエ
ータ。[Scope of Claims] 1. A fixed core, a movable core that moves with respect to the fixed core, an electric winding wound so as to apply a first magnetic flux to the movable core when energized, and the first In an electromagnetic actuator comprising a permanent magnet provided on the fixed iron core or the movable iron core so as to shunt a second magnetic flux in parallel to the magnetic flux of The sum of the magnetic resistance value between the magnetic pole surfaces of the fixed iron core and the magnetic resistance value between the side magnetic pole surfaces of the movable iron core and the magnetic pole surfaces of the permanent magnet, and the fixed iron core facing each other from the magnetic pole surfaces of both end surfaces of the movable iron core. and the sum of the magnetic resistance values between the magnetic pole faces is 0.2 or more and 1.0 or less, and the ratio of the magnetomotive force of the permanent magnet to the magnetomotive force caused by energization of the electric winding is 0.2 or more and 2.0 or less. An electromagnetic actuator characterized by: 2. The electromagnetic actuator according to claim 1, wherein a magnetic material is disposed in contact with the entire surface of the permanent magnet. 3. The electromagnetic actuator according to claim 1, wherein a magnetic body is disposed in contact with both side surfaces of the permanent magnet. 4. The electromagnetic actuator according to claim 1, wherein a magnetic body is disposed with a required gap between the permanent magnet and the permanent magnet.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61115440A JPS62271404A (en) | 1986-05-20 | 1986-05-20 | Electromagnetic actuator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61115440A JPS62271404A (en) | 1986-05-20 | 1986-05-20 | Electromagnetic actuator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62271404A JPS62271404A (en) | 1987-11-25 |
| JPH0423403B2 true JPH0423403B2 (en) | 1992-04-22 |
Family
ID=14662611
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61115440A Granted JPS62271404A (en) | 1986-05-20 | 1986-05-20 | Electromagnetic actuator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62271404A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0427132Y2 (en) * | 1988-01-27 | 1992-06-30 | ||
| JP5229182B2 (en) * | 2009-10-12 | 2013-07-03 | 株式会社デンソー | Clutch mechanism |
| JP2014101902A (en) * | 2012-11-16 | 2014-06-05 | Denso Corp | Clutch mechanism |
| JP5910472B2 (en) * | 2012-11-23 | 2016-04-27 | 株式会社デンソー | Clutch mechanism |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57186312A (en) * | 1981-05-11 | 1982-11-16 | Kamiya Denshi Kogyo Kk | Bistable keep solenoid |
-
1986
- 1986-05-20 JP JP61115440A patent/JPS62271404A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62271404A (en) | 1987-11-25 |
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