JP2008160944A - Electromagnetic actuator - Google Patents

Electromagnetic actuator Download PDF

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JP2008160944A
JP2008160944A JP2006344865A JP2006344865A JP2008160944A JP 2008160944 A JP2008160944 A JP 2008160944A JP 2006344865 A JP2006344865 A JP 2006344865A JP 2006344865 A JP2006344865 A JP 2006344865A JP 2008160944 A JP2008160944 A JP 2008160944A
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magnetic
mover
electromagnetic
permanent magnet
electromagnetic block
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JP4950652B2 (en
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Tomohiro Izumi
智博 泉
Kenji Narita
憲二 成田
Tomohiro Ota
智浩 太田
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Panasonic Electric Works Co Ltd
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Matsushita Electric Works Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To improve magnetic efficiency by using magnetic flux unused due to magnetic saturation in a conventional system. <P>SOLUTION: An electromagnetic actuator comprises an electromagnetic block 1 where a coil 11 is wound on a core 10 equipped with a plurality of magnetic poles 11, and a moving member 2 which faces the electromagnetic block via a magnetic gap and also is driven to reciprocate by applying AC to the coil. A magnetic conductor of a mover comprising a permanent magnet and the magnetic conductor is equipped with projected pieces 23 which project to the side of the magnetic pole of the electromagnetic block in both ends in the direction of reciprocation of the permanent mover. One of the projected pieces 23 is arranged to form a closed circuit between itself and the electromagnetic block at both ends of the reciprocating stroke of the above mover and the other is arranged not to form a closed circuit. Magnetic flux flow is increased with the projected piece and the projected piece may not increase magnetoresistance. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

本発明は、電磁アクチュエータ、殊に可動子に往復動を行わせる振動型の電磁アクチュエータに関するものである。   The present invention relates to an electromagnetic actuator, and more particularly to a vibration type electromagnetic actuator that causes a mover to reciprocate.

往復式電気かみそりの駆動手段に用いている電磁アクチュエータとして、図15に示すものがある。これは3つの磁極11を備えるE字型コア10の中央磁極11にコイル12を巻回して中央磁極11と両端磁極11,11とを異極に磁化することができるようにした電磁ブロック1と、この電磁ブロック11によって往復駆動される可動子2とからなるもので、可動子2は上記複数の磁極11に対向する永久磁石21とバックヨークとしての導磁体22とからなるもので、図中左右方向に往復動自在に支持されている。そして可動子2における永久磁石21は、往復動方向である左右において異なる極を有している。なお、両極の中心間の距離は、コア10における中央磁極11と図中左方の磁極11との間の中心から、中央磁極11と図中右方の磁極11との間の中心までの距離にほぼ一致させてある。   As an electromagnetic actuator used for a reciprocating electric razor driving means, there is one shown in FIG. This is an electromagnetic block 1 in which a coil 12 is wound around a central magnetic pole 11 of an E-shaped core 10 having three magnetic poles 11 so that the central magnetic pole 11 and both end magnetic poles 11 and 11 can be magnetized to different polarities. The mover 2 is reciprocally driven by the electromagnetic block 11, and the mover 2 is composed of a permanent magnet 21 facing the magnetic poles 11 and a conductor 22 as a back yoke. It is supported so that it can reciprocate in the left-right direction. And the permanent magnet 21 in the needle | mover 2 has a pole which is different in right and left which is a reciprocation direction. The distance between the centers of both poles is the distance from the center between the central magnetic pole 11 in the core 10 and the left magnetic pole 11 in the figure to the center between the central magnetic pole 11 and the right magnetic pole 11 in the figure. Is almost matched.

図中3は可動子2の復帰と可動子2をばね振動系とすることを担うばねであり、対のばね3,3が可動子2の両端に夫々配されて互いに逆方向に可動子2を付勢している。   In the figure, reference numeral 3 denotes a spring responsible for returning the movable element 2 and making the movable element 2 a spring vibration system. A pair of springs 3 and 3 are arranged at both ends of the movable element 2 so that the movable element 2 is in the opposite direction. Is energized.

この電磁アクチュエータにおいては、電磁ブロック1のコイル12に一方向の電流を流せば図15(a)に示すように可動子2は一方向に駆動され、コイル12に他方向の電流を流せば可動子2は図15(b)に示すように他方向に駆動され、コイル12に電流を流さなければ可動子2は中央位置に復帰する。従って、コイル12に矩形波状の交番電流を流せば可動子2は左右の往復動を行う。   In this electromagnetic actuator, if a current in one direction is passed through the coil 12 of the electromagnetic block 1, the mover 2 is driven in one direction as shown in FIG. 15 (a), and is movable when a current in the other direction is passed through the coil 12. The child 2 is driven in the other direction as shown in FIG. 15B, and if no current is supplied to the coil 12, the movable member 2 returns to the center position. Therefore, if a rectangular wave-like alternating current is passed through the coil 12, the mover 2 performs a reciprocating motion to the left and right.

しかし、上記構成の電磁アクチュエータにおいては、次のような課題を有している。すなわち、磁気回路の磁気効率は、磁気ギャップ間の磁気抵抗に決まるが、この磁気抵抗は永久磁石の起磁力とトレードオフの関係にあり、永久磁石を大きくして起磁力を大きくすれば、磁気抵抗が増加する。そして有効利用できない磁束は、可動子の導磁体の磁気飽和を引き起こし、これに伴って推力のサチュレーションが起こって磁気効率を低下させる。また永久磁石の起磁力を有効に使えないために、電磁ブロックの起磁力で磁束を補完しているのが現状であり、これ故に銅損などの損失が大きくなってアクチュエータ全体の走行効率が低減している。
特開平7−265560号公報 特開平7−313749号公報
However, the electromagnetic actuator having the above configuration has the following problems. In other words, the magnetic efficiency of the magnetic circuit is determined by the magnetoresistance between the magnetic gaps, but this magnetoresistance is in a trade-off relationship with the magnetomotive force of the permanent magnet. Resistance increases. The magnetic flux that cannot be used effectively causes magnetic saturation of the magnetic conductor of the mover, and this causes saturation of the thrust, which lowers the magnetic efficiency. In addition, since the magnetomotive force of the permanent magnet cannot be used effectively, the magnetic flux is supplemented by the magnetomotive force of the electromagnetic block, and therefore the loss such as copper loss increases and the travel efficiency of the entire actuator is reduced. is doing.
JP-A-7-265560 JP-A-7-313749

本発明は上記の従来の問題点に鑑みて発明したものであって、従来は磁気飽和によって利用できていなかった磁束の利用で磁気効率を向上させた電磁アクチュエータを提供することを課題とするものである。   The present invention has been invented in view of the above-described conventional problems, and an object of the present invention is to provide an electromagnetic actuator having improved magnetic efficiency by using magnetic flux that has not been used conventionally by magnetic saturation. It is.

上記課題を解決するために本発明に係る電磁アクチュエータは、複数の磁極を備えたコアにコイルを巻回している電磁ブロックと、電磁ブロックにおける磁極の先端面に磁気ギャップを介して対向するとともに、対向方向と直交する方向に往復動自在に支持されて電磁ブロックのコイルへの交番電流の印加で往復駆動される可動子とからなる電磁アクチュエータであり、上記可動子は一面が上記電磁ブロックの磁極に磁気ギャップを介して対向する永久磁石と、永久磁石の他面側に配された導磁体とからなり、上記導磁体は上記永久可動子の往復動方向の両端で且つ上記永久磁石の往復動方向の両端より外側位置に夫々電磁ブロックの磁極側に突出する突片を備えているとともに、これら突片は上記可動子の往復動ストロークの両端位置において、一方の突片が電磁ブロックとの間に閉回路を形成し且つ他方の突片が閉回路を形成しない位置に配置されていることに特徴を有している。突片を設けることでより多くの磁束が流れるようにするとともに、突片が磁気抵抗を増加させる存在とならないようにしたものである。   In order to solve the above problems, an electromagnetic actuator according to the present invention is opposed to an electromagnetic block in which a coil is wound around a core having a plurality of magnetic poles, with a magnetic gap at the tip surface of the magnetic pole in the electromagnetic block, An electromagnetic actuator comprising a mover supported reciprocally in a direction orthogonal to the opposing direction and driven to reciprocate by application of an alternating current to a coil of the electromagnetic block, wherein the mover has one surface with a magnetic pole of the electromagnetic block The permanent magnets are opposed to each other with a magnetic gap therebetween, and a magnetic conductor disposed on the other surface side of the permanent magnet, the magnetic conductors at both ends in the reciprocating direction of the permanent mover and the reciprocating motion of the permanent magnet. Projecting pieces projecting toward the magnetic pole side of the electromagnetic block, respectively, are provided at both ends of the reciprocating stroke of the mover. Te, one protrusion is characterized in that and the other protrusion to form a closed circuit is disposed in a position that does not form a closed circuit between the electromagnetic block. By providing the projecting piece, more magnetic flux flows, and the projecting piece is made not to increase the magnetic resistance.

特に上記電磁ブロックが3つの磁極を備えて少なくとも中央磁極にコイルが巻回されるE字型コアであり、上記可動子の永久磁石が可動子の往復動方向において異なる磁極を備え、上記永久磁石の可動子往復動方向における両端間の幅に可動子の往復動ストローク値を足した値が、電磁ブロックにおける両端の磁極間の最大幅以下であるものでは、これまで磁束が流れていなかったところに突片によって新たな磁気閉回路を形成することができる。   In particular, the electromagnetic block is an E-shaped core having three magnetic poles and a coil wound around at least the central magnetic pole, and the permanent magnet of the mover has different magnetic poles in the reciprocating direction of the mover, and the permanent magnet When the value obtained by adding the reciprocating stroke value of the mover to the width between both ends in the reciprocating direction of the mover is less than the maximum width between the magnetic poles at both ends of the electromagnetic block, the magnetic flux has not flowed so far A new magnetic closed circuit can be formed by the protruding piece.

上記突片は、永久磁石の可動子往復動方向の両端に接する位置に配置されたものであっても、永久磁石の可動子往復動方向の両端から離れた位置に配置されたものであってもよい。   Even if the protruding piece is arranged at a position in contact with both ends of the permanent magnet in the reciprocating direction of the mover, it is arranged at a position away from both ends of the moving direction of the permanent magnet in the reciprocating direction. Also good.

上記突片は、電磁ブロックの磁極における可動子往復動方向の外側面と対向する部分を備えたものとしてもよい。上記永久磁石は導磁体に設けた凹部に嵌め込まれているものとするのも好ましい。   The protruding piece may include a portion facing the outer surface of the magnetic pole of the electromagnetic block in the reciprocating direction of the mover. It is also preferable that the permanent magnet is fitted in a recess provided in the magnetic conductor.

また、上記導磁体における永久磁石との接合面に凹部を設けたり、上記突片の端面と上記コアの磁極の端面との少なくとも一方に凹凸を形成したり、上記突片の先端部と上記コアの磁極の先端部とのの少なくとも一方に面取りを施して斜面を形成しても、好ましい結果を得ることができる。   In addition, a concave portion is provided on the surface of the magnetic conductor to be bonded to the permanent magnet, an unevenness is formed on at least one of the end face of the protruding piece and the end face of the magnetic pole of the core, or the tip of the protruding piece and the core Even if the inclined surface is formed by chamfering at least one of the tip of the magnetic pole, a preferable result can be obtained.

更に上記突片の可動子往復動方向における幅は、電磁ブロックのコアの各磁極の可動子往復動方向における幅以上の大きさであることが望ましい。   Further, the width of the projecting piece in the reciprocating direction of the mover is preferably larger than the width of each magnetic pole of the core of the electromagnetic block in the reciprocating direction of the mover.

本発明は、導磁体に設けた一方の突片が電磁ブロックとの間に閉回路を形成してより多くの磁束を流すものであり、可動子の往復動のストローク端において他方の突片は閉回路を形成せず、このために突片が磁気抵抗を増加させる存在とはならないものであり、このために磁気効率を向上させることができる。   In the present invention, one projecting piece provided on the magnetic conductor forms a closed circuit with the electromagnetic block to flow more magnetic flux, and at the stroke end of the reciprocation of the mover, the other projecting piece is A closed circuit is not formed, and for this reason, the projecting piece does not exist to increase the magnetic resistance, so that the magnetic efficiency can be improved.

以下、本発明を添付図面に示す実施形態に基いて説明すると、図1及び図2に示すものは上記従来例と同じ基本的構成を有するもので、電磁ブロック1と可動子2とからなるとともに、電磁ブロック1は3つの磁極11を備えるE字型コア10の中央磁極11にコイル12を巻回している。上記複数の磁極11の端面に磁気ギャップを介して対向するとともに磁極11が並ぶ方向に往復動自在に支持されている可動子2は、永久磁石21とバックヨークとしての導磁体22とからなり、上記永久磁石21は、往復動方向である左右において異なる極を有している。なお、永久磁石11の幅W1は図2に示すように、電磁ブロック1の左右両端の磁極11,11の最大幅W2より小さく、また上記幅W1に可動子2とストロークSTの和も、上記最大幅W2以下(W2≧W1+ST)としてある。   Hereinafter, the present invention will be described with reference to the embodiments shown in the accompanying drawings. The structure shown in FIGS. 1 and 2 has the same basic configuration as the above-described conventional example, and includes an electromagnetic block 1 and a mover 2. The electromagnetic block 1 has a coil 12 wound around a central magnetic pole 11 of an E-shaped core 10 having three magnetic poles 11. A mover 2 that faces the end faces of the plurality of magnetic poles 11 via a magnetic gap and is supported so as to reciprocate in the direction in which the magnetic poles 11 are arranged is composed of a permanent magnet 21 and a magnetic conductor 22 as a back yoke. The permanent magnet 21 has different poles on the left and right in the reciprocating direction. As shown in FIG. 2, the width W1 of the permanent magnet 11 is smaller than the maximum width W2 of the magnetic poles 11 and 11 at the left and right ends of the electromagnetic block 1, and the sum of the mover 2 and the stroke ST is equal to the width W1. The maximum width is W2 or less (W2 ≧ W1 + ST).

そして本願発明に係る電磁アクチュエータにおいては、可動子2の往復動方向において永久磁石21よりも外側に位置するところに、バックヨークである導磁体22から電磁ブロック1側に向けて突出する突片23を設けている。導磁体22の往復動方向両端部で且つ可動子2の往復動ストロークの一端側で一方の突片23が、ストロークの他端側で他方の突片23が両端の磁極11との対向位置よりも往復動方向において外側にずれるところに設けた上記突片23,23は、次のように機能する。   And in the electromagnetic actuator which concerns on this invention, the protrusion 23 which protrudes toward the electromagnetic block 1 side from the magnetic conductor 22 which is a back yoke in the location located outside the permanent magnet 21 in the reciprocating direction of the needle | mover 2 is provided. Is provided. From one end of the reciprocating direction of the magnet 22 and one end of one end of the reciprocating stroke of the mover 2, and the other end 23 of the other end of the stroke facing the magnetic pole 11 at both ends. The protrusions 23, 23 provided at positions deviating outward in the reciprocating direction also function as follows.

すなわち、可動子2が電磁ブロック1による電磁力で一方向に駆動されて図2上段に示すようにそのストロークの一方端に達した時、中央磁極11から永久磁石21、一端側の磁極11という閉回路が形成されているが、この時、他端側の磁極11、他端側の突片23、永久磁石21、中央磁極11という閉回路も形成される。また、この時には一端側の突片23を通る閉回路は形成されない。逆に可動子2が電磁ブロック1による電磁力で他方向に駆動されて図2下段に示すようにそのストロークの他方端に達した時、他端側の磁極11から永久磁石21、中央磁極11という閉回路が形成されると同時に、一端側の磁極11、一端側の突片23、永久磁石21、中央磁極11という閉回路も形成され、この時、他端側の突片23を通る閉回路は形成されない。   That is, when the mover 2 is driven in one direction by the electromagnetic force from the electromagnetic block 1 and reaches one end of its stroke as shown in the upper part of FIG. A closed circuit is formed. At this time, a closed circuit including the magnetic pole 11 on the other end side, the projecting piece 23 on the other end side, the permanent magnet 21 and the central magnetic pole 11 is also formed. At this time, a closed circuit passing through the protruding piece 23 on one end side is not formed. Conversely, when the mover 2 is driven in the other direction by the electromagnetic force from the electromagnetic block 1 and reaches the other end of the stroke as shown in the lower part of FIG. 2, the permanent magnet 21 and the central magnetic pole 11 are changed from the magnetic pole 11 on the other end side. At the same time, a closed circuit consisting of the magnetic pole 11 at one end, the projecting piece 23 at one end, the permanent magnet 21 and the central magnetic pole 11 is also formed. At this time, the closed circuit passing through the projecting piece 23 at the other end is formed. A circuit is not formed.

ここにおいて、上記突片23を通る閉回路は、従来のものでは得られなかった磁路であって、突片23を設けたことで磁束が流れる経路が増えるものであり、しかも上記閉回路を形成する突片23と異なる他方の突片23はストローク端において閉回路を形成しないために、突片23を設けたことが磁気抵抗を増加させることにはならないものであり、このために磁気突極性を利用した磁気力(リラクタンス力)を有効利用できて磁気効率が向上し、磁気ギャップ間の磁気吸引力の増加、強いては往復動方向の推力の増加を得られるものである。また、バックヨークである導磁体22に突片23を設けるものであるために、コストが高くなることもない。   Here, the closed circuit passing through the projecting piece 23 is a magnetic path that cannot be obtained by a conventional one, and the path through which the magnetic flux flows is increased by providing the projecting piece 23. Since the other projecting piece 23 different from the projecting piece 23 to be formed does not form a closed circuit at the stroke end, the provision of the projecting piece 23 does not increase the magnetic resistance. The magnetic force (reluctance force) utilizing the polarity can be effectively used to improve the magnetic efficiency, and the magnetic attraction force between the magnetic gaps can be increased, and the thrust in the reciprocating direction can be increased. Further, since the projecting piece 23 is provided on the magnetic conductor 22 that is the back yoke, the cost does not increase.

上記突片23,23は、永久磁石21の両端に接している必要はなく、図3に示すように、永久磁石21の両端から離れたところに位置させて、可動子2内の磁気短絡経路にギャップを設けてもよい。磁気回路の磁気抵抗をコントロールできるとともに、ギャップによって可動子2と電磁ブロック1との間に集中して磁束を流すことができて磁気効率が向上する。   The projecting pieces 23 and 23 do not need to be in contact with both ends of the permanent magnet 21, but are positioned away from both ends of the permanent magnet 21 as shown in FIG. A gap may be provided. The magnetic resistance of the magnetic circuit can be controlled, and the magnetic flux can be caused to flow between the movable element 2 and the electromagnetic block 1 by the gap, thereby improving the magnetic efficiency.

図4に示すように、電磁ブロック1の両端の磁極11,11の外側面に対向する対向突片23a,23aを可動子2の導磁体22が備えているものとしてもよい。電磁ブロック1の利用されていない空間となる側面の磁気抵抗を低下させて磁束が通過できる面積が増加するものであり、この結果、漏れインダクタンスが減少して磁気効率が向上する。   As shown in FIG. 4, the magnetic conductor 22 of the mover 2 may include opposing projecting pieces 23 a and 23 a that face the outer surfaces of the magnetic poles 11 and 11 at both ends of the electromagnetic block 1. The area through which the magnetic flux can pass is increased by reducing the magnetic resistance of the side surface, which is an unused space of the electromagnetic block 1, and as a result, the leakage inductance is reduced and the magnetic efficiency is improved.

図5に示すように、永久磁石21を導磁体22に設けた凹所に嵌め込むようにして取り付けたものも好適に利用できる。この場合、永久磁石21の配置が容易となる。   As shown in FIG. 5, a permanent magnet 21 attached so as to be fitted in a recess provided in the magnetic conductor 22 can be suitably used. In this case, the arrangement of the permanent magnet 21 is facilitated.

図6に示すものは、可動子2の導磁体22に突片23及び対向突片23a設けたものにおいて、これら突片23及び対向突片23における磁極11との対向面に、可動子2が駆動されて変位する際の磁気力(リラクタンス力)を変化させることになる凹凸24を設けたもので、凹凸24の位置や大きさ並びに配置に応じて推力を自由に制御することができるために、コギングの低減を図ることが容易となる。このような凹凸は、磁極11側に設けることも有効である。   In the structure shown in FIG. 6, the projecting piece 23 and the opposed projecting piece 23 a are provided on the magnetic conductor 22 of the movable element 2. Since the projections and depressions 24 that change the magnetic force (reluctance force) when displaced by being driven are provided, the thrust can be freely controlled according to the position, size, and arrangement of the projections and depressions 24. It becomes easy to reduce cogging. It is also effective to provide such irregularities on the magnetic pole 11 side.

図7に示すように、導磁体22における永久磁石21の接合面に凹部25,25を設けても、凹部25の位置や大きさ並びに配置に応じて推力を自由に制御することができるためにコギング低減に有利である。   As shown in FIG. 7, the thrust can be freely controlled in accordance with the position, size, and arrangement of the recess 25 even if the recess 25 is provided on the joint surface of the permanent magnet 21 in the magnetic conductor 22. It is advantageous for cogging reduction.

図8に示すものは、可動子2の導磁体22に設けた突片23の先端に面取りを施すことで可動子2の往復動方向側の角に斜面を形成して、可動子2と電磁ブロック1との間の磁束を斜めに発生させることができるようにしたものであり、この場合、磁気抵抗を変化させつつ往復動方向の推力を発生させることができるために磁気効率が向上する。なお、面取りを施すことは磁極11に対して行うことも有効である。   In the structure shown in FIG. 8, a chamfer is formed on the tip of the projecting piece 23 provided on the magnetic conductor 22 of the mover 2 to form a slope at a corner on the reciprocating direction side of the mover 2. The magnetic flux between the block 1 and the block 1 can be generated obliquely. In this case, the thrust in the reciprocating direction can be generated while changing the magnetic resistance, so that the magnetic efficiency is improved. The chamfering is also effective for the magnetic pole 11.

上記の各例で示した構成は任意に組み合わせて実施することができる。図9〜図12はこのような組み合わせの例を示しており、図9に示すものでは突片23先端に面取りを施すとともに先端面に凹凸24を設け、更に凹部25を導磁体22に設けている。この場合、可動子2の往復動方向の推力が増加するとともに可動子2と電磁ブロック1との対向方向の磁気吸引力を軽減することができるために、この磁気吸引力に対抗する可動子2の支持機構への応力の緩和による耐久性の向上を磁気効率の向上と同時に得ることができる。   The configurations shown in the above examples can be implemented in any combination. 9 to 12 show examples of such combinations. In the example shown in FIG. 9, the tip of the projecting piece 23 is chamfered, an unevenness 24 is provided on the front end surface, and a recess 25 is provided on the magnetic conductor 22. Yes. In this case, since the thrust in the reciprocating direction of the mover 2 increases and the magnetic attractive force in the opposing direction of the mover 2 and the electromagnetic block 1 can be reduced, the mover 2 that opposes this magnetic attractive force. The durability can be improved simultaneously with the improvement of the magnetic efficiency by relaxing the stress on the support mechanism.

また、図10に示すものでは図9に示したものに加えて、磁極11の先端面に凹凸14を設けており、図11に示すものでは図9に示したものに加えて、磁極11の先端に面取りを施することによる斜面の形成を行っており、図12に示すものでは図9に示したものに加えて、磁極11の先端に面取りによる斜面の形成と同時に磁極11の先端面に凹凸14を設けている。いずれも推力を自由を制御することができ、コギングの低減及び磁気効率の向上を図ることができる。   In addition to the one shown in FIG. 9, the tip shown in FIG. 10 is provided with irregularities 14 on the tip surface of the magnetic pole 11, and the one shown in FIG. The slope is formed by chamfering the tip. In the case shown in FIG. 12, in addition to the one shown in FIG. 9, the slope of the magnetic pole 11 is formed on the tip of the magnetic pole 11 simultaneously with the formation of the slope by chamfering. Concavities and convexities 14 are provided. In any case, the thrust can be freely controlled, and cogging can be reduced and magnetic efficiency can be improved.

ところで、可動子2の導磁体22に設けた突片の23の幅(可動子2の往復動方向の幅)L2は、図13に示すように、電磁ブロック1における各磁極11の幅(可動子2の往復方向の幅)L1以上の値となるようにしておくと、可動子2の磁気飽和を解消して磁束利用率を向上させる点で有利である。   By the way, as shown in FIG. 13, the width of the protrusion 23 provided on the magnetic conductor 22 of the mover 2 (width in the reciprocating direction of the mover 2) L2 is the width of each magnetic pole 11 in the electromagnetic block 1 (movable). It is advantageous in that the magnetic saturation of the mover 2 is eliminated and the magnetic flux utilization rate is improved by setting the value to be equal to or larger than the width L1 of the reciprocating direction of the child 2.

図14は電磁ブロック1が2つの磁極11,11を有するU字型コア10と各磁極11に巻回した2つのコイル12,12とからなり、可動子2は電磁ブロック1との対向方向において着磁された永久磁石21と導磁体22とからなるもので、このタイプにおける導磁体22は永久磁石21の背面側磁極(磁極11と反対側の磁極)を利用するために、元々突片23,23を備えているが、ここでは上記のものと同様に突片23の幅を各磁極11の幅以上のものとし、更に可動子2の往復動ストロークの両端において、一方の突片23が電磁ブロック1との間で形成される閉回路から外れた位置にくるように配置している。   FIG. 14 shows that the electromagnetic block 1 includes a U-shaped core 10 having two magnetic poles 11, 11 and two coils 12, 12 wound around the magnetic poles 11. The permanent magnet 21 is composed of a magnetized permanent magnet 21 and a magnetic conductor 22, and the magnetic conductor 22 in this type uses a back side magnetic pole (a magnetic pole opposite to the magnetic pole 11) of the permanent magnet 21. , 23, here, the width of the projecting piece 23 is equal to or greater than the width of each magnetic pole 11, and one projecting piece 23 is provided at both ends of the reciprocating stroke of the mover 2. It arrange | positions so that it may come in the position remove | deviated from the closed circuit formed between the electromagnetic blocks 1. FIG.

このものにおいても可動子2の磁気飽和を解消して磁束利用効率を高めることができるものであり、磁気効率及び総合効率を向上することができる。   In this case, the magnetic saturation of the mover 2 can be eliminated and the magnetic flux utilization efficiency can be increased, and the magnetic efficiency and the overall efficiency can be improved.

また、ここでは可動子2が一つであるものの例を上げたが、単一の電磁ブロック1に対して複数の可動子2,2を平行並列に並べて、全可動子2,2を同時に往復駆動させるものにおいても適用することができるのはもちろんである。この場合、平行並列に並ぶ可動子2,2の永久磁石21の磁極の配置を同じとすれば、2つの可動子2,2を同位相で往復駆動することができ、2つの可動子2,2の永久磁石21の磁極の配置を逆にすれば、2つの可動子2,2を逆位相で往復駆動することができる。   Also, here, an example is given in which there is one mover 2, but a plurality of movers 2, 2 are arranged in parallel and parallel to a single electromagnetic block 1, and all the movers 2, 2 reciprocate simultaneously. Needless to say, the present invention can also be applied to a driving device. In this case, if the arrangement of the magnetic poles of the permanent magnets 21 of the movers 2 and 2 arranged in parallel and parallel is the same, the two movers 2 and 2 can be reciprocally driven in the same phase. If the arrangement of the magnetic poles of the two permanent magnets 21 is reversed, the two movers 2 and 2 can be driven back and forth in opposite phases.

なお、本発明に係る各例では図示を省略したが、従来例のものと同様にばね3,3を配したものであってもよい。また、電磁ブロック1を固定とし、可動子2が往復駆動されるもので説明したが、電磁ブロック1と可動子2との動きは相対的なものであるために、両者が相互に逆方向に動くものや、可動子2が固定されて電磁ブロック1が動くものであってもよい。   Although not shown in each example according to the present invention, springs 3 and 3 may be provided as in the conventional example. Further, the electromagnetic block 1 is fixed and the movable element 2 is reciprocally driven. However, since the movements of the electromagnetic block 1 and the movable element 2 are relative, they are opposite to each other. It may be one that moves or one that moves the electromagnetic block 1 while the mover 2 is fixed.

本発明の実施の形態の一例を示すもので、(a)は正面図、(b)は斜視図である。FIG. 1 shows an example of an embodiment of the present invention, where (a) is a front view and (b) is a perspective view. 同上の動作を示す説明図である。It is explanatory drawing which shows operation | movement same as the above. 他例の正面図である。It is a front view of another example. 更に他例の正面図である。Furthermore, it is a front view of another example. 別の例の正面図である。It is a front view of another example. 更に別の正面図である。It is another front view. 他の例の正面図である。It is a front view of another example. 更に他の例の正面図である。It is a front view of another example. 異なる例の正面図である。It is a front view of a different example. 更に異なる例の正面図である。It is a front view of a further different example. 別の例の正面図である。It is a front view of another example. 更に別の例の正面図である。It is a front view of another example. 他の例の正面図である。It is a front view of another example. 更に他の例を示しており、(a)は正面図、(b)は斜視図である。Furthermore, the other example is shown, (a) is a front view, (b) is a perspective view. (a)(b)は従来例の正面図である。(a) (b) is a front view of a conventional example.

符号の説明Explanation of symbols

1 電磁ブロック
2 可動子
10 コア
11 磁極
12 コイル
21 永久磁石
22 導磁体
23 突片
DESCRIPTION OF SYMBOLS 1 Electromagnetic block 2 Movable element 10 Core 11 Magnetic pole 12 Coil 21 Permanent magnet 22 Magnetic conductor 23 Protrusion piece

Claims (10)

複数の磁極を備えたコアにコイルを巻回している電磁ブロックと、電磁ブロックにおける磁極の先端面に磁気ギャップを介して対向するとともに、対向方向と直交する方向に往復動自在に支持されて電磁ブロックのコイルへの交番電流の印加で往復駆動される可動子とからなる電磁アクチュエータであり、上記可動子は一面が上記電磁ブロックの磁極に磁気ギャップを介して対向する永久磁石と、永久磁石の他面側に配された導磁体とからなり、上記導磁体は上記永久可動子の往復動方向の両端で且つ上記永久磁石の往復動方向の両端より外側位置に夫々電磁ブロックの磁極側に突出する突片を備えているとともに、これら突片は上記可動子の往復動ストロークの両端位置において、一方の突片が電磁ブロックとの間に閉回路を形成し且つ他方の突片が閉回路を形成しない位置に配置されていることを特徴とする電磁アクチュエータ。   An electromagnetic block in which a coil is wound around a core having a plurality of magnetic poles, and opposed to a tip surface of the magnetic pole in the electromagnetic block through a magnetic gap, and is supported by a reciprocating motion in a direction orthogonal to the opposing direction. An electromagnetic actuator comprising a mover that is reciprocally driven by application of an alternating current to the coil of the block, the mover having a permanent magnet whose one surface faces the magnetic pole of the electromagnetic block via a magnetic gap, and a permanent magnet A magnetic conductor disposed on the other surface side, and the magnetic conductor projects to both ends of the permanent mover in the reciprocating direction and to positions outside the both ends of the permanent magnet in the reciprocating direction on the magnetic pole side of the electromagnetic block. The projecting pieces have a closed circuit at one end of the reciprocating stroke of the movable element, and one projecting piece forms a closed circuit with the electromagnetic block. An electromagnetic actuator, wherein a projecting piece is disposed in a position that does not form a closed circuit. 上記突片は、永久磁石の可動子往復動方向の両端に接する位置に配置されていることを特徴とする請求項1記載の電磁アクチュエータ。   The electromagnetic actuator according to claim 1, wherein the projecting piece is disposed at a position in contact with both ends of the permanent magnet in the reciprocating direction of the mover. 上記突片は、永久磁石の可動子往復動方向の両端から離れた位置に配置されていることを特徴とする請求項1記載の電磁アクチュエータ。   The electromagnetic actuator according to claim 1, wherein the projecting piece is disposed at a position away from both ends of the permanent magnet in the reciprocating direction of the mover. 上記電磁ブロックは3つの磁極を備えて少なくとも中央磁極にコイルが巻回されるE字型コアであり、上記可動子の永久磁石は可動子の往復動方向において異なる磁極を備え、上記永久磁石の可動子往復動方向における両端間の幅に可動子の往復動ストローク値を足した値が、電磁ブロックにおける両端の磁極間の最大幅以下であることを特徴とする請求項1〜3のいずれか1項に記載の電磁アクチュエータ。   The electromagnetic block is an E-shaped core having three magnetic poles and a coil wound around at least a central magnetic pole, and the permanent magnet of the mover has different magnetic poles in the reciprocating direction of the mover, The value obtained by adding the reciprocating stroke value of the mover to the width between both ends in the reciprocating direction of the mover is equal to or less than the maximum width between the magnetic poles at both ends of the electromagnetic block. The electromagnetic actuator according to item 1. 上記突片は、電磁ブロックの磁極における可動子往復動方向の外側面と対向する部分を備えていることを特徴とする請求項1〜4のいずれか1項に記載の電磁アクチュエータ。   5. The electromagnetic actuator according to claim 1, wherein the projecting piece includes a portion facing an outer surface of a magnetic pole of the electromagnetic block in a reciprocating direction of the mover. 上記永久磁石は導磁体に設けた凹部に嵌め込まれていることを特徴とする請求項1〜5のいずれか1項に記載の電磁アクチュエータ。   The electromagnetic actuator according to any one of claims 1 to 5, wherein the permanent magnet is fitted in a recess provided in the magnetic conductor. 上記導磁体における永久磁石との接合面に凹部が設けられていることを特徴とする請求項1〜6のいずれか1項に記載の電磁アクチュエータ。   The electromagnetic actuator according to claim 1, wherein a concave portion is provided on a joint surface of the magnetic conductor with the permanent magnet. 上記突片の端面と上記コアの磁極の端面との少なくとも一方に凹凸が形成されていることを特徴とする請求項1〜7のいずれか1項に記載の電磁アクチュエータ。   The electromagnetic actuator according to any one of claims 1 to 7, wherein irregularities are formed on at least one of an end face of the protruding piece and an end face of the magnetic pole of the core. 上記突片の先端部と上記コアの磁極の先端部とのの少なくとも一方に面取りが施されて斜面が形成されていることを特徴とする請求項1〜8のいずれか1項に記載の電磁アクチュエータ。   9. The electromagnetic wave according to claim 1, wherein an inclined surface is formed by chamfering at least one of a tip portion of the protruding piece and a tip portion of the magnetic pole of the core. Actuator. 上記突片の可動子往復動方向における幅は、電磁ブロックのコアの各磁極の可動子往復動方向における幅以上の大きさであることを特徴とする請求項1〜9のいずれか1項に記載の電磁アクチュエータ。   The width of the projecting piece in the reciprocating direction of the mover is larger than the width of each magnetic pole of the core of the electromagnetic block in the reciprocating direction of the mover. The electromagnetic actuator described.
JP2006344865A 2006-12-21 2006-12-21 Electromagnetic actuator Expired - Fee Related JP4950652B2 (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101919513B1 (en) * 2011-02-23 2018-11-16 무빙 마그네트 테크놀로지스 Electromagnetic actuator having improved force density and use thereof for an electric razor
CN111756210A (en) * 2019-03-28 2020-10-09 日本电产三协株式会社 Actuator

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JPS5658773A (en) * 1979-10-19 1981-05-21 Brother Ind Ltd Swing type step driving device
JPH08308201A (en) * 1995-04-27 1996-11-22 Foster Electric Co Ltd Vibration actuator
JP2001016837A (en) * 1999-06-25 2001-01-19 Matsushita Electric Works Ltd Oscillation type linear actuator
JP2001179178A (en) * 1999-12-24 2001-07-03 Teikoku Tsushin Kogyo Co Ltd Vibration generator
JP2001224157A (en) * 2000-02-08 2001-08-17 Twinbird Corp Electromagnetic reciprocal drive mechanism
JP2002112519A (en) * 2000-09-29 2002-04-12 Hitachi Metals Ltd Electromagnetially reciprocating driver

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5658773A (en) * 1979-10-19 1981-05-21 Brother Ind Ltd Swing type step driving device
JPH08308201A (en) * 1995-04-27 1996-11-22 Foster Electric Co Ltd Vibration actuator
JP2001016837A (en) * 1999-06-25 2001-01-19 Matsushita Electric Works Ltd Oscillation type linear actuator
JP2001179178A (en) * 1999-12-24 2001-07-03 Teikoku Tsushin Kogyo Co Ltd Vibration generator
JP2001224157A (en) * 2000-02-08 2001-08-17 Twinbird Corp Electromagnetic reciprocal drive mechanism
JP2002112519A (en) * 2000-09-29 2002-04-12 Hitachi Metals Ltd Electromagnetially reciprocating driver

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101919513B1 (en) * 2011-02-23 2018-11-16 무빙 마그네트 테크놀로지스 Electromagnetic actuator having improved force density and use thereof for an electric razor
CN111756210A (en) * 2019-03-28 2020-10-09 日本电产三协株式会社 Actuator
CN111756210B (en) * 2019-03-28 2023-03-21 日本电产三协株式会社 Actuator

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