JP6794907B2 - Engagement device - Google Patents
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- JP6794907B2 JP6794907B2 JP2017076495A JP2017076495A JP6794907B2 JP 6794907 B2 JP6794907 B2 JP 6794907B2 JP 2017076495 A JP2017076495 A JP 2017076495A JP 2017076495 A JP2017076495 A JP 2017076495A JP 6794907 B2 JP6794907 B2 JP 6794907B2
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Description
本発明は、永久磁石の極性反転を用いて係合状態の開放状態との切り替えが可能な、係合装置に関する。 The present invention relates to an engaging device capable of switching between an engaged state and an open state by using the polarity reversal of a permanent magnet.
従来から、特許文献1や2に開示されているように、2種類の永久磁石と電磁石とを用いた係合装置が知られている。例えば特許文献1では、図13に例示するように、相対的に着磁し難い極性固定磁石100、相対的に着磁し易い極性可変磁石102A,102B、及び極性反転させるためのコイル104A,104Bを用いた係合装置(ブレーキ装置)が開示されている。 Conventionally, as disclosed in Patent Documents 1 and 2, an engaging device using two types of permanent magnets and an electromagnet has been known. For example, in Patent Document 1, as illustrated in FIG. 13, the polarity fixing magnet 100 which is relatively difficult to magnetize, the polarity variable magnets 102A and 102B which are relatively easy to magnetize, and the coils 104A and 104B for reversing the polarity. The engaging device (brake device) using the above is disclosed.
極性可変磁石102A,102Bはそれぞれその外周に、コイル104A,104Bが巻き回されている。極性可変磁石102A,102B及びコイル104A,104Bは固定側ヨーク106とともに固定されている。極性可変磁石102A,102Bとその側面が接するようにして固定リング107が設けられる。固定リング107は円弧状ヨーク108と、隣り合う円弧状ヨーク108A,108Bを連結する極性固定磁石100を備える。固定リング107の内周面は、ギャップ(間隔)を空けて回転リング110が設けられる。 The polar variable magnets 102A and 102B have coils 104A and 104B wound around them, respectively. The variable polarity magnets 102A and 102B and the coils 104A and 104B are fixed together with the fixed side yoke 106. The fixing ring 107 is provided so that the polarity variable magnets 102A and 102B are in contact with the side surfaces thereof. The fixing ring 107 includes an arc-shaped yoke 108 and a polarity fixing magnet 100 that connects adjacent arc-shaped yokes 108A and 108B. Rotating rings 110 are provided on the inner peripheral surface of the fixing ring 107 with a gap (interval).
図14には開放状態の図が例示されている。極性固定磁石100の磁束と極性可変磁石102A,102Bの磁束とは順方向(直列)であり、両者の合成磁束が極性可変磁石102A→円弧状ヨーク108A→極性固定磁石100→円弧状ヨーク108B→極性可変磁石102B→固定側ヨーク106→極性可変磁石102A→とのループ経路L_OFFを通過する。 FIG. 14 illustrates a diagram in the open state. The magnetic flux of the polarity fixing magnet 100 and the magnetic flux of the polarity variable magnets 102A and 102B are in the forward direction (series), and the combined magnetic flux of both is the polarity variable magnet 102A → arcuate yoke 108A → polarity fixing magnet 100 → arcuate yoke 108B → It passes through the loop path L_OFF of the polarity variable magnet 102B → the fixed side yoke 106 → the polarity variable magnet 102A →.
図15には係合状態の図が例示されている。これはコイル104A,104Bから生じた磁界によって、極性可変磁石102A,102Bの極性が図14の状態から反転されたときの様子が例示されている。このとき、極性可変磁石102A,102Bの磁束は、固定側ヨーク106→極性可変磁石102B→円弧状ヨーク108B→回転リング110→円弧状ヨーク108A→極性可変磁石102Aとのループ経路L_ON1を通過する。また、極性固定磁石100の磁束は、円弧状ヨーク108B→回転リング110→円弧状ヨーク108A→極性固定磁石100とのループ経路L_ON2を通過する。 FIG. 15 illustrates a diagram of the engaged state. This is illustrated when the polarities of the polarity variable magnets 102A and 102B are reversed from the state shown in FIG. 14 by the magnetic field generated from the coils 104A and 104B. At this time, the magnetic flux of the polar variable magnets 102A and 102B passes through the loop path L_ON1 with the fixed side yoke 106 → the polar variable magnet 102B → the arc-shaped yoke 108B → the rotating ring 110 → the arc-shaped yoke 108A → the polar variable magnet 102A. Further, the magnetic flux of the polarity fixing magnet 100 passes through the loop path L_ON2 of the arc-shaped yoke 108B → the rotating ring 110 → the arc-shaped yoke 108A → the polarity fixing magnet 100.
円弧状ヨーク108A,108Bの内周面及び回転リング110の外周面には周方向に沿って凹凸が形成されている。そのため、両者のギャップは周方向に沿って異なるものとなる。ギャップの変動に応じて当該ギャップを通過する磁気抵抗も変化する。例えば円弧状ヨーク108A,108Bの内周面と回転リング110の外周面との凸部同士が対向すると磁気抵抗は最小値を取り、凹部同士が対向すると磁気抵抗は最大値を取る。この状態から円弧状ヨーク108A,108Bと回転リング110とが上記の状態から相対回転移動しようとすると磁束を維持しようとする力が働き、その結果回転リング110は固定リング107と係合状態となり回転リング110の回転移動が止められる。 The inner peripheral surfaces of the arc-shaped yokes 108A and 108B and the outer peripheral surface of the rotating ring 110 are formed with irregularities along the circumferential direction. Therefore, the gap between the two is different along the circumferential direction. The magnetic resistance passing through the gap changes according to the fluctuation of the gap. For example, when the convex portions of the inner peripheral surfaces of the arc-shaped yokes 108A and 108B and the outer peripheral surfaces of the rotating ring 110 face each other, the magnetic resistance takes the minimum value, and when the concave portions face each other, the magnetic resistance takes the maximum value. From this state, when the arcuate yokes 108A and 108B and the rotating ring 110 try to rotate relative to each other from the above state, a force for maintaining the magnetic flux acts, and as a result, the rotating ring 110 engages with the fixed ring 107 and rotates. The rotational movement of the ring 110 is stopped.
ところで、永久磁石の極性反転を用いた係合装置を、回転体同士の係合に適用することが考えられる。例えば図13のブレーキ装置について、固定リング107を回転可能とし(回転リング107’とし)、極性可変磁石102A,102Bとは所定のギャップを介して磁路を形成することが考えられる。 By the way, it is conceivable to apply an engaging device using the polarity reversal of a permanent magnet to the engagement between rotating bodies. For example, in the brake device of FIG. 13, it is conceivable that the fixing ring 107 is rotatable (rotating ring 107') and a magnetic path is formed with the polarity variable magnets 102A and 102B through a predetermined gap.
しかしながらそのような場合、図16に示すように、極性可変磁石102A,102B間で極性が反転しており、これを受ける回転リング107’も周方向(回転方向)に沿って極性が反転する。この状態で極性可変磁石102A,102Bと回転リング107’とが相対回転移動すると、磁束の変化に伴って渦電流が発生し、回転リング107’の回転を妨げるおそれがある。そこで本発明は、回転に伴う渦電流の発生を従来よりも抑制可能な、係合装置を提供することを目的とする。 However, in such a case, as shown in FIG. 16, the polarity is reversed between the polarity variable magnets 102A and 102B, and the polarity of the rotating ring 107 ′ receiving the polarity is also reversed along the circumferential direction (rotational direction). If the polar variable magnets 102A and 102B and the rotating ring 107'move relative to each other in this state, an eddy current is generated along with the change in the magnetic flux, which may hinder the rotation of the rotating ring 107'. Therefore, an object of the present invention is to provide an engaging device capable of suppressing the generation of eddy currents due to rotation as compared with the conventional case.
本発明は係合装置に関する。当該係合装置は、固定体、第1回転体、及び第2回転体を備える。固定体は、小径円柱部と、小径円柱部の軸方向両端に設けられた一対の大径円環部とを備えるボビンと、小径円柱部の一対の大径円環部の間に巻き回されたコイルと、を備える。第1回転体は、一対の大径円環部の一方の外周面とギャップを設けて内周面が対向する円環形状の第1回転体ヨークと、一対の大径円環部の他方とギャップを設けて内周面が対向する円環形状の第2回転体ヨークと、を備える。第2回転体は、第1及び第2回転体ヨークの外周面とのギャップ幅が周方向に沿って異なるように形成された内周面を備える。固定体及び第1回転体の少なくとも一方には、第1永久磁石と、第1永久磁石よりも着磁し易い第2永久磁石が設けられる。コイルから生じる磁界によって第2永久磁石の磁極が反転し、第2永久磁石の磁極反転に応じて、第1及び第2永久磁石の磁束が第2回転体を通過する係合状態と、第1及び第2永久磁石の磁束が第2回転体を通過しない開放状態とに切り替え可能となる。この構成において、一対の大径円環部の外周面と、第1及び第2回転体ヨークの内周面とのギャップ幅は、周方向に沿って等しくなるように形成される。また、一対の大径円環部の一方の外周面と第1回転体ヨークの内周面との間、及び、一対の大径円環部の他方と第2回転体ヨークの内周面との間には、周方向に沿って極性が同一の磁束のみが通過する。 The present invention relates to an engaging device. The engaging device includes a fixed body, a first rotating body, and a second rotating body. The fixed body is wound between a bobbin having a small-diameter cylindrical portion and a pair of large-diameter annular portions provided at both ends in the axial direction of the small-diameter cylindrical portion, and a pair of large-diameter annular portions of the small-diameter cylindrical portion. It is equipped with a coil. The first rotating body includes a ring-shaped first rotating body yoke having a gap with one outer peripheral surface of a pair of large-diameter ring portions and facing the inner peripheral surfaces, and the other of the pair of large-diameter ring portions. A ring-shaped second rotating body yoke having a gap and facing the inner peripheral surfaces is provided. The second rotating body includes an inner peripheral surface formed so that the gap width with the outer peripheral surface of the first and second rotating body yokes is different along the circumferential direction. At least one of the fixed body and the first rotating body is provided with a first permanent magnet and a second permanent magnet that is easier to magnetize than the first permanent magnet. The magnetic field generated from the coil reverses the magnetic poles of the second permanent magnet, and the magnetic fluxes of the first and second permanent magnets pass through the second rotating body in response to the magnetic pole reversal of the second permanent magnet. The magnetic field of the second permanent magnet can be switched to an open state in which the magnetic field does not pass through the second rotating body. In this configuration, the gap widths between the outer peripheral surfaces of the pair of large-diameter ring portions and the inner peripheral surfaces of the first and second rotating body yokes are formed to be equal along the circumferential direction. Further, between one outer peripheral surface of the pair of large-diameter annular portions and the inner peripheral surface of the first rotating body yoke, and between the other of the pair of large-diameter annular portions and the inner peripheral surface of the second rotating body yoke. Only magnetic fluxes of the same polarity pass along the circumferential direction between them.
また上記発明において、第1永久磁石は、第1回転体ヨークと第2回転体ヨークとを接続するようにして第1回転体に設けられてもよい。 Further, in the above invention, the first permanent magnet may be provided on the first rotating body so as to connect the first rotating body yoke and the second rotating body yoke.
また上記発明において、第2永久磁石は、一対の大径円環部に設けられ、相対的に外周側であって周方向に沿って設けられた一方の磁極と、相対的に内周側であって周方向に沿って設けられた他方の磁極とを備えてもよい。 Further, in the above invention, the second permanent magnet is provided on a pair of large-diameter ring portions, and is relatively on the outer peripheral side and relatively on the inner peripheral side with one magnetic pole provided along the circumferential direction. It may be provided with the other magnetic pole provided along the circumferential direction.
また上記発明において、第2永久磁石は、第1及び第2回転体ヨークに設けられ、相対的に外周側であって周方向に沿って設けられた一方の磁極と、相対的に内周側であって周方向に沿って設けられた他方の磁極とを備えてもよい。 Further, in the above invention, the second permanent magnet is provided on the first and second rotating body yokes, and is relatively on the outer peripheral side and relatively on the inner peripheral side with one magnetic pole provided along the circumferential direction. It may be provided with the other magnetic pole provided along the circumferential direction.
本発明の係合装置の別態様では、当該係合装置は、固定体、第1回転体、第2回転体、及びガイド部材を備える。固定体は、小径円柱部と、小径円柱部の軸方向両端に設けられた一対の大径円環部とを備えるボビンと、小径円柱部の一対の大径円環部の間に巻き回されたコイルと、を備える。第1回転体は円環形状であって、一対の大径円環部の一方の外周面とギャップを設けて内周面が対向する。第2回転体は円環形状であって、一対の大径円環部の他方の外周面とギャップを設けて内周面が対向する。ガイド部材は第1及び第2回転体の少なくとも一方を軸方向にガイドする。固定体には、第1永久磁石と、第1永久磁石よりも着磁し易い第2永久磁石が設けられる。コイルから生じる磁界によって第2永久磁石の磁極が反転し、第2永久磁石の磁極反転に応じて、第1及び第2永久磁石の磁束が第1及び第2回転体を通過して両者を係合させる係合状態と、第1及び第2永久磁石の磁束が第1及び第2回転体を通過しない開放状態とに切り替え可能となっている。この構成において、一対の大径円環部の外周面と、第1及び第2回転体の内周面とのギャップ幅は、周方向に沿って等しくなるように形成される。また、一対の大径円環部の一方の外周面と第1回転体の内周面との間、及び、一対の大径円環部の他方と第2回転体の内周面との間には、周方向に沿って極性が同一の磁束のみが通過する。 In another aspect of the engaging device of the present invention, the engaging device includes a fixed body, a first rotating body, a second rotating body, and a guide member. The fixed body is wound between a bobbin having a small-diameter cylindrical portion and a pair of large-diameter annular portions provided at both ends in the axial direction of the small-diameter cylindrical portion, and a pair of large-diameter annular portions of the small-diameter cylindrical portion. It is equipped with a coil. The first rotating body has an annular shape, and has a gap with one outer peripheral surface of a pair of large-diameter annular portions so that the inner peripheral surfaces face each other. The second rotating body has an annular shape, and has a gap with the other outer peripheral surface of the pair of large-diameter annular portions so that the inner peripheral surfaces face each other. The guide member guides at least one of the first and second rotating bodies in the axial direction. The fixed body is provided with a first permanent magnet and a second permanent magnet that is easier to magnetize than the first permanent magnet. The magnetic field generated from the coil reverses the magnetic poles of the second permanent magnet, and the magnetic fluxes of the first and second permanent magnets pass through the first and second rotating bodies in response to the magnetic pole reversal of the second permanent magnet and engage both. It is possible to switch between the engaged state of matching and the open state in which the magnetic fields of the first and second permanent magnets do not pass through the first and second rotating bodies. In this configuration, the gap widths between the outer peripheral surfaces of the pair of large-diameter ring portions and the inner peripheral surfaces of the first and second rotating bodies are formed to be equal along the circumferential direction. Further, between one outer peripheral surface of the pair of large-diameter annular portions and the inner peripheral surface of the first rotating body, and between the other of the pair of large-diameter annular portions and the inner peripheral surface of the second rotating body. Only magnetic fluxes of the same polarity pass along the circumferential direction.
また上記発明において、第1永久磁石は、コイルよりも外周側であって一対の大径円環部を接続するようにして固定体に設けられてもよい。 Further, in the above invention, the first permanent magnet may be provided on the fixed body on the outer peripheral side of the coil so as to connect a pair of large diameter ring portions.
また上記発明において、第2永久磁石は、一対の大径円環部に設けられ、相対的に外周側であって周方向に沿って設けられた一方の磁極と、相対的に内周側であって周方向に沿って設けられた他方の磁極とを備えてもよい。 Further, in the above invention, the second permanent magnet is provided on a pair of large-diameter ring portions, and is relatively on the outer peripheral side and relatively on the inner peripheral side with one magnetic pole provided along the circumferential direction. It may be provided with the other magnetic pole provided along the circumferential direction.
また上記発明において、第1回転体及び第2回転体のそれぞれの対向面には、互いに噛み合う突起列が形成されていてもよい。 Further, in the above invention, a row of protrusions that mesh with each other may be formed on the facing surfaces of the first rotating body and the second rotating body.
本発明によれば、固定体の一対の大径円環部の外周面と、第1及び第2回転体ヨークの内周面とのギャップ幅を、周方向に沿って等しくしている。さらに、一対の大径円環部の一方の外周面と前記第1回転体ヨークの内周面との間、及び、前記一対の大径円環部の他方と前記第2回転体ヨークの内周面との間には、周方向に沿って極性が同一の磁束のみが通過するようにしている。その結果、周方向すなわち回転方向に沿った磁束変化を抑制可能となり、渦電流の発生を抑制可能となる。 According to the present invention, the gap widths between the outer peripheral surfaces of the pair of large-diameter annular portions of the fixed body and the inner peripheral surfaces of the first and second rotating body yokes are made equal along the circumferential direction. Further, between one outer peripheral surface of the pair of large-diameter ring portions and the inner peripheral surface of the first rotating body yoke, and between the other of the pair of large-diameter ring portions and the inside of the second rotating body yoke. Only magnetic fluxes having the same polarity pass along the circumferential direction with the peripheral surface. As a result, the change in magnetic flux along the circumferential direction, that is, the rotation direction can be suppressed, and the generation of eddy current can be suppressed.
<第1実施形態>
図1に、第1実施形態に係る係合装置10を例示する。係合装置10は、固定体12、第1回転体14、及び第2回転体16を備える。係合装置10は、例えば第1回転体14と第2回転体16とを連結させて駆動力を伝達させるクラッチ装置として機能する。なお、図1以降、図面には互いに直交するX軸、Y軸、Z軸が示される。Y軸は回転軸と平行な軸である。X軸、Z軸は回転軸に直交する径方向の軸である。X軸及びZ軸もまた直交関係にある。
<First Embodiment>
FIG. 1 illustrates the engaging device 10 according to the first embodiment. The engaging device 10 includes a fixed body 12, a first rotating body 14, and a second rotating body 16. The engaging device 10 functions as, for example, a clutch device that connects the first rotating body 14 and the second rotating body 16 to transmit a driving force. From FIG. 1, the drawings show X-axis, Y-axis, and Z-axis that are orthogonal to each other. The Y-axis is an axis parallel to the rotation axis. The X-axis and Z-axis are radial axes orthogonal to the rotation axis. The X-axis and Z-axis are also orthogonal.
固定体12は、ボビン18、コイル20、及び極性可変磁石22A,22B(第2永久磁石)を備える。ボビン18は側面視(Z軸方向)H型の部材であり、回転軸方向(Y軸方向)に延設される小径円柱部26と、その両端に設けられる一対の大径円環部24A,24Bを備える。ボビン18の少なくとも一部は高透磁率材料から構成され、例えば低炭素鋼等の軟質磁性材料から構成される。 The fixed body 12 includes a bobbin 18, a coil 20, and variable polarity magnets 22A and 22B (second permanent magnets). The bobbin 18 is an H-shaped member viewed from the side (Z-axis direction), and has a small-diameter cylindrical portion 26 extending in the rotation axis direction (Y-axis direction) and a pair of large-diameter annular portions 24A provided at both ends thereof. It is equipped with 24B. At least a part of the bobbin 18 is made of a high magnetic permeability material, for example, a soft magnetic material such as low carbon steel.
ボビン18の小径円柱部26にはコイル20が巻き回される。コイル20は接続配線28を介して外部の電源(図示せず)に接続される。コイル20の小径円柱部26への巻数は1回でも複数回でもよい。 A coil 20 is wound around the small-diameter cylindrical portion 26 of the bobbin 18. The coil 20 is connected to an external power source (not shown) via the connection wiring 28. The number of turns of the coil 20 around the small-diameter cylindrical portion 26 may be one or a plurality of turns.
極性可変磁石22A,22Bは、それぞれ大径円環部24A,24Bの少なくとも一部を構成する。例えば、大径円環部24A,24Bのそれぞれ全体が極性可変磁石22A,22Bから構成されてもよい。この場合、小径円柱部26を高透磁率材料から形成してこれをヨークとする。また、極性可変磁石22Aの外周面は、大径円環部24Aの外周面を構成し、極性可変磁石22Bの外周面は、大径円環部24Bの外周面を構成する。 The variable polarity magnets 22A and 22B form at least a part of the large-diameter ring portions 24A and 24B, respectively. For example, the entire large diameter ring portions 24A and 24B may be composed of the polarity variable magnets 22A and 22B, respectively. In this case, the small-diameter cylindrical portion 26 is formed of a high magnetic permeability material and used as a yoke. The outer peripheral surface of the variable polarity magnet 22A constitutes the outer peripheral surface of the large-diameter annular portion 24A, and the outer peripheral surface of the variable polarity magnet 22B constitutes the outer peripheral surface of the large-diameter annular portion 24B.
極性可変磁石22A,22Bは、周方向に沿って同一の磁極のみが揃うように構成される。例えば極性可変磁石22Aは、図1に破線で示すように、相対的に外周側にはその周方向に沿って一方の磁極23A(例えばS極)が配置され、相対的に内周側にはその周方向に沿って他方の磁極23B(例えばN極)が配置される。このようにすることで、周方向に沿って磁性が同一の磁束のみが通過することになる。 The polarity variable magnets 22A and 22B are configured so that only the same magnetic poles are aligned along the circumferential direction. For example, in the polarity variable magnet 22A, as shown by a broken line in FIG. 1, one magnetic pole 23A (for example, S pole) is relatively arranged on the outer peripheral side along the circumferential direction, and relatively on the inner peripheral side. The other magnetic pole 23B (for example, N pole) is arranged along the circumferential direction. By doing so, only magnetic fluxes having the same magnetism pass along the circumferential direction.
極性可変磁石22Bは、極性可変磁石22Aとは磁極が反転するように配置される。すなわち、相対的に外周側にはその周方向に沿って一方の磁極23B(例えばN極)が配置され、相対的に内周側にはその周方向に沿って他方の磁極23A(例えばS極)が配置される。 The polarity variable magnet 22B is arranged so that the magnetic poles are reversed from those of the polarity variable magnet 22A. That is, one magnetic pole 23B (for example, N pole) is relatively arranged on the outer peripheral side along the circumferential direction, and the other magnetic pole 23A (for example, S pole) is relatively arranged on the inner peripheral side along the circumferential direction. ) Is placed.
極性可変磁石22A,22Bはともに、円筒形状もよい。また図2に示すように、円弧形状の極性可変磁石22A,22Bを複数組み立てて円筒形状としてもよい。 Both the polarity variable magnets 22A and 22B may have a cylindrical shape. Further, as shown in FIG. 2, a plurality of arc-shaped variable polarity magnets 22A and 22B may be assembled to form a cylindrical shape.
極性可変磁石22A,22Bは、後述する極性固定磁石32(第1永久磁石)よりも着磁し易いという特性を備える。つまり、極性固定磁石32よりも磁極を反転させ易い特性を備える。図3には磁界(横軸)と磁束密度(縦軸)からなる磁石特性グラフが例示されている。 The variable polarity magnets 22A and 22B have a characteristic that they are easier to magnetize than the polarity fixing magnet 32 (first permanent magnet) described later. That is, it has a characteristic that the magnetic poles are more easily inverted than the polarity fixing magnet 32. FIG. 3 illustrates a magnet characteristic graph composed of a magnetic field (horizontal axis) and a magnetic flux density (vertical axis).
一般的に、磁石の動作点はパーミアンス直線(磁石形状や磁気回路などで決まる直線)と減磁曲線の交点で決まる。例えば、図3に示すようなパーミアンス直線を仮定した場合、アルニコ磁石(Alnico5)の動作点は点A,ネオジム磁石は点Bとなる。このグラフから、アルニコ磁石はネオジム磁石の1/3程度の磁束密度しか得られないことが分かる。 Generally, the operating point of a magnet is determined by the intersection of a permeance straight line (a straight line determined by the shape of a magnet or a magnetic circuit) and a demagnetization curve. For example, assuming a permeance straight line as shown in FIG. 3, the operating point of the alnico magnet (Alnico5) is point A, and that of the neodymium magnet is point B. From this graph, it can be seen that the alnico magnet can obtain only about 1/3 of the magnetic flux density of the neodymium magnet.
このことから、アルニコ磁石(Almico5)は着磁が容易だが磁力が弱く,ネオジム磁石(Ne−Fe−B)は着磁が困難だが磁力が強い特性を有していることが導かれる。上記を踏まえて、極性可変磁石22A,22Bは例えばアルニコ磁石から構成され、極性固定磁石32は例えばネオジム磁石から構成される。 This leads to the fact that the alnico magnet (Almico5) is easy to magnetize but has a weak magnetic force, and the neodymium magnet (Ne-Fe-B) is difficult to magnetize but has a strong magnetic force. Based on the above, the polarity variable magnets 22A and 22B are composed of, for example, alnico magnets, and the polarity fixing magnet 32 is composed of, for example, neodymium magnets.
第1回転体14は、第1回転体ヨーク30A、第2回転体ヨーク30B、及び極性固定磁石32を備える。第1回転体14は、固定体12の外周側に設けられ、かつ、第2回転体16の内周側に設けられる、略円環形状の部材である。第1回転体14は、その周方向に沿って(言い換えるとY軸回りに)回転可能となっている。 The first rotating body 14 includes a first rotating body yoke 30A, a second rotating body yoke 30B, and a polarity fixing magnet 32. The first rotating body 14 is a substantially ring-shaped member provided on the outer peripheral side of the fixed body 12 and on the inner peripheral side of the second rotating body 16. The first rotating body 14 can rotate along its circumferential direction (in other words, around the Y axis).
第1回転体ヨーク30Aは、高透磁率材料から構成され、例えば低炭素鋼等の軟質磁性材料から構成される。第1回転体ヨーク30Aは略円環形状であって、その内周面はギャップ(間隔)を設けて大径円環部24A(極性可変磁石22A)の外周面と対向する。また、第1回転体ヨーク30Aの軸方向長さは大径円環部24A(極性可変磁石22A)の軸方向長さと略等しく形成される。 The first rotating body yoke 30A is made of a high magnetic permeability material, and is made of a soft magnetic material such as low carbon steel. The first rotating body yoke 30A has a substantially annular shape, and its inner peripheral surface is provided with a gap (interval) so as to face the outer peripheral surface of the large-diameter annular portion 24A (polarity variable magnet 22A). Further, the axial length of the first rotating body yoke 30A is formed to be substantially equal to the axial length of the large-diameter annular portion 24A (polarity variable magnet 22A).
さらに、第1回転体ヨーク30Aの内周面と大径円環部24A(極性可変磁石22A)の外周面のギャップ幅W1は、周方向に沿って等しくなるように形成される。これにより、周方向に沿ってギャップによる磁気抵抗が一様となるので、周方向に沿った磁束変化が抑制され、その結果、渦電流の発生が抑制される。 Further, the gap width W1 between the inner peripheral surface of the first rotating body yoke 30A and the outer peripheral surface of the large-diameter annular portion 24A (polarity variable magnet 22A) is formed so as to be equal along the circumferential direction. As a result, the magnetic resistance due to the gap becomes uniform along the circumferential direction, so that the change in magnetic flux along the circumferential direction is suppressed, and as a result, the generation of eddy current is suppressed.
例えば、大径円環部24A(極性可変磁石22A)の外周面と第1回転体ヨーク30Aの内周面は、側面視(Y軸方向視)で同心円となるように形成される。第1回転体14は図示しない軸受け等により、第1回転体ヨーク30Aと大径円環部24A(極性可変磁石22A)の外周面のギャップ幅W1が維持される。 For example, the outer peripheral surface of the large-diameter annular portion 24A (polarity variable magnet 22A) and the inner peripheral surface of the first rotating body yoke 30A are formed so as to be concentric circles in a side view (Y-axis direction view). The first rotating body 14 maintains a gap width W1 between the first rotating body yoke 30A and the outer peripheral surface of the large-diameter annular portion 24A (polarity variable magnet 22A) by a bearing or the like (not shown).
第2回転体ヨーク30Bは、高透磁率材料から構成され、例えば低炭素鋼等の軟質磁性材料から構成される。第2回転体ヨーク30Bも第1回転体ヨーク30Aと同様に略円環形状であって、その軸方向長さは大径円環部24B(極性可変磁石22B)の軸方向長さに略等しい。また第2回転体ヨーク30Bの内周面はギャップ(間隔)を設けて大径円環部24B(極性可変磁石22B)の外周面と対向する。 The second rotating body yoke 30B is made of a high magnetic permeability material, and is made of a soft magnetic material such as low carbon steel. The second rotating body yoke 30B also has a substantially annular shape like the first rotating body yoke 30A, and its axial length is substantially equal to the axial length of the large-diameter annular portion 24B (polarity variable magnet 22B). .. Further, the inner peripheral surface of the second rotating body yoke 30B is provided with a gap (interval) so as to face the outer peripheral surface of the large-diameter annular portion 24B (polarity variable magnet 22B).
さらに、第2回転体ヨーク30Bの内周面と大径円環部24B(極性可変磁石22B)の外周面のギャップ幅W1は、周方向に沿って等しくなるように形成される。これにより、周方向に沿って磁気抵抗が一様となるので、周方向に沿ったギャップによる磁束変化が抑制され、その結果、渦電流の発生が抑制される。 Further, the gap width W1 between the inner peripheral surface of the second rotating body yoke 30B and the outer peripheral surface of the large-diameter annular portion 24B (polarity variable magnet 22B) is formed to be equal along the circumferential direction. As a result, the magnetic resistance becomes uniform along the circumferential direction, so that the change in magnetic flux due to the gap along the circumferential direction is suppressed, and as a result, the generation of eddy current is suppressed.
例えば、大径円環部24B(極性可変磁石22B)の外周面と第2回転体ヨーク30Bの内周面は、側面視(Y軸方向視)で同心円となるように形成される。第1回転体14は図示しない軸受け等により、第2回転体ヨーク30Bの内周面と大径円環部24B(極性可変磁石22B)の外周面のギャップ幅W1が維持される。 For example, the outer peripheral surface of the large-diameter annular portion 24B (polarity variable magnet 22B) and the inner peripheral surface of the second rotating body yoke 30B are formed so as to be concentric circles in a side view (Y-axis direction view). The first rotating body 14 maintains a gap width W1 between the inner peripheral surface of the second rotating body yoke 30B and the outer peripheral surface of the large-diameter annular portion 24B (polarity variable magnet 22B) by a bearing or the like (not shown).
一方、第1及び第2回転体ヨーク30A,30Bの外周面と、第2回転体16の内周面とのギャップは、周方向に沿って異なるように形成される。例えば、第1及び第2回転体ヨーク30A,30Bの外周面には、周方向に沿って凹凸部31Aが形成され、第2回転体16の内周面にも周方向に沿って凹凸部31Bが形成される。このような形状とすることで、第1及び第2回転体ヨーク30A,30Bの外周面と、第2回転体16の内周面との間の磁気抵抗が周方向に沿って異なることになる。この結果、第1及び第2回転体ヨーク30A,30Bと、第2回転体16との相対回転が妨げられ、両者は同期して回転可能となる。 On the other hand, the gaps between the outer peripheral surfaces of the first and second rotating bodies 30A and 30B and the inner peripheral surfaces of the second rotating body 16 are formed so as to be different along the circumferential direction. For example, uneven portions 31A are formed on the outer peripheral surfaces of the first and second rotating body yokes 30A and 30B along the circumferential direction, and the uneven portions 31B are also formed on the inner peripheral surfaces of the second rotating body 16 along the circumferential direction. Is formed. With such a shape, the magnetic resistance between the outer peripheral surfaces of the first and second rotating body yokes 30A and 30B and the inner peripheral surface of the second rotating body 16 is different along the circumferential direction. .. As a result, the relative rotation between the first and second rotating body yokes 30A and 30B and the second rotating body 16 is hindered, and both can rotate in synchronization.
極性固定磁石32(第1永久磁石)は、上述したように極性可変磁石22A,22Bと比較して着磁し難い特性を備えている。例えば極性固定磁石32はネオジム磁石から構成される。極性固定磁石32は、第1回転体ヨーク30Aと第2回転体ヨーク30Bとの間を接続(連結)するように設けられる。つまり、第1回転体ヨーク30Aと第2回転体ヨーク30Bとのギャップを連絡(接続)する機能を極性固定磁石32が備えている。極性固定磁石32は例えば円環状に形成される。 As described above, the polarity fixed magnet 32 (first permanent magnet) has a characteristic that it is difficult to magnetize as compared with the polarity variable magnets 22A and 22B. For example, the polarity fixing magnet 32 is composed of a neodymium magnet. The polarity fixing magnet 32 is provided so as to connect (connect) between the first rotating body yoke 30A and the second rotating body yoke 30B. That is, the polarity fixing magnet 32 has a function of communicating (connecting) the gap between the first rotating body yoke 30A and the second rotating body yoke 30B. The polarity fixing magnet 32 is formed, for example, in an annular shape.
極性固定磁石32は固定体12及び第1回転体14の少なくとも一方に設けられればよい。この点について、極性固定磁石32(第1磁石)が、第1回転体14に設けられることで、第2回転体16との磁束ループを形成する際に乗り越えるギャップの数は2で済むというメリットが得られる。比較例として固定体12に極性固定磁石32を設ける場合、固定体12と第1回転体14との間に形成されたギャップを含んで、第2回転体16との磁束ループを形成する際に乗り越えるギャップの数は4となる。このように、乗り越えるギャップ数が相対的に少ない第1回転体14に極性固定磁石32を設けることで、ギャップを乗り越える際の磁気抵抗による磁力の減少を抑制可能となる。 The polarity fixing magnet 32 may be provided on at least one of the fixed body 12 and the first rotating body 14. Regarding this point, since the polarity fixing magnet 32 (first magnet) is provided on the first rotating body 14, there is an advantage that the number of gaps to be overcome when forming a magnetic flux loop with the second rotating body 16 is only two. Is obtained. As a comparative example, when a polar fixing magnet 32 is provided on the fixed body 12, when a magnetic flux loop with the second rotating body 16 is formed including a gap formed between the fixed body 12 and the first rotating body 14. The number of gaps to overcome is four. In this way, by providing the polar fixing magnet 32 on the first rotating body 14 having a relatively small number of gaps to be overcome, it is possible to suppress a decrease in magnetic force due to magnetic resistance when the gap is overcome.
第2回転体16は、第1回転体14の外周側に設けられる、円柱形状の部材である。第2回転体16は高透磁率材料から構成され、例えば低炭素鋼等の軟質磁性材料から構成される。第2回転体16は図示しない軸受等によりその軸(Y軸)回りに回転可能に支持されている。 The second rotating body 16 is a cylindrical member provided on the outer peripheral side of the first rotating body 14. The second rotating body 16 is made of a high magnetic permeability material, and is made of a soft magnetic material such as low carbon steel. The second rotating body 16 is rotatably supported around its axis (Y axis) by a bearing or the like (not shown).
図4〜図6には、第1実施形態に係る係合装置10の開放状態、磁極反転時、及び係合状態の様子が例示されている。なお図4〜図6はいずれも、図1または図2の斜視図のZ−Y平面を示している。 4 to 6 illustrate the open state, the magnetic pole reversal, and the engaged state of the engaging device 10 according to the first embodiment. In addition, each of FIGS. 4 to 6 shows the ZZ plane of the perspective view of FIG. 1 or FIG.
図4には開放時の例が示されている。開放時には、第1回転体14及び第2回転体16の係合が解かれる。具体的には図4に示すように、極性可変磁石22A,22Bと極性固定磁石32の極性が揃っており(直列状態であり)、これらの磁石の磁束は合成磁束となって破線で示すループ経路L_OFFを通過する。具体的には、極性可変磁石22A,22B及び極性固定磁石32の磁束は、極性固定磁石32→第1回転体ヨーク30A→極性可変磁石22A→ボビン18(小径円柱部26)→極性可変磁石22B→第2回転体ヨーク30B→極性固定磁石32との経路を通過する。 FIG. 4 shows an example at the time of opening. At the time of opening, the first rotating body 14 and the second rotating body 16 are disengaged. Specifically, as shown in FIG. 4, the polar variable magnets 22A and 22B and the polar fixed magnets 32 have the same polarity (in a series state), and the magnetic fluxes of these magnets become a combined magnetic flux and are loops shown by broken lines. It passes through the path L_OFF. Specifically, the magnetic fluxes of the polar variable magnets 22A and 22B and the polar fixed magnet 32 are the polar fixed magnet 32 → the first rotating body yoke 30A → the polar variable magnet 22A → the bobbin 18 (small diameter columnar portion 26) → the polar variable magnet 22B. → Second rotating body yoke 30B → Passes through the path with the polarity fixing magnet 32.
図5には極性反転時の様子が例示されている。コイル20に電流を供給して磁界を発生させることで、極性可変磁石22A,22Bの極性を反転させる。例えば図3のグラフより、動作点AとBの中間値を取る磁界をコイル20に発生させて、選択的に極性可変磁石22A,22Bの極性を反転させる。 FIG. 5 illustrates the state at the time of polarity reversal. By supplying an electric current to the coil 20 to generate a magnetic field, the polarities of the variable polarity magnets 22A and 22B are reversed. For example, from the graph of FIG. 3, a magnetic field having an intermediate value between the operating points A and B is generated in the coil 20, and the polarities of the polar variable magnets 22A and 22B are selectively inverted.
図6には極性反転後の係合時の様子が例示されている。この図の破線で示されているように、極性可変磁石22A,22Bの磁束と極性固定磁石32の磁束とが逆極性となるために、概念上並列に2種類のループ経路L_ON1,L_ON2が発生する。 FIG. 6 illustrates the state at the time of engagement after the polarity is reversed. As shown by the broken line in this figure, the magnetic fluxes of the variable polarity magnets 22A and 22B and the magnetic fluxes of the fixed polarity magnets 32 have opposite polarities, so that two types of loop paths L_ON1 and L_ON2 are conceptually generated in parallel. To do.
すなわち、極性固定磁石32→第1回転体ヨーク30A→第2回転体16→第2回転体ヨーク30B→極性固定磁石32との経路を通過するループ経路L_ON1が形成される。また、極性可変磁石22A→第1回転体ヨーク30A→第2回転体16→第2回転体ヨーク30B→極性可変磁石22B→ボビン18(小径円柱部26)→極性可変磁石22Aとの経路を通過するループ経路L_ON2が形成される。 That is, a loop path L_ON1 that passes through the path of the polarity fixing magnet 32 → the first rotating body yoke 30A → the second rotating body 16 → the second rotating body yoke 30B → the polarity fixing magnet 32 is formed. Further, it passes through the path of the polarity variable magnet 22A → the first rotating body yoke 30A → the second rotating body 16 → the second rotating body yoke 30B → the polarity variable magnet 22B → the bobbin 18 (small diameter cylindrical portion 26) → the polarity variable magnet 22A. Loop path L_ON2 is formed.
ループ経路L_ON1,L_ON2は第1回転体14及び第2回転体16を通過(鎖交)することから、両者は磁気的に結合される。さらに上述したように両者の対向面は周方向(回転方向)に沿ってギャップ幅W2が変化するように形成されているため、磁束変化を阻害するように、第1回転体14及び第2回転体16が同期して回転する。すなわち両者が係合される。 Since the loop paths L_ON1 and L_ON2 pass through (chain) the first rotating body 14 and the second rotating body 16, they are magnetically coupled to each other. Further, as described above, since the facing surfaces of the two are formed so that the gap width W2 changes along the circumferential direction (rotation direction), the first rotating body 14 and the second rotating body 14 and the second rotation so as to hinder the change in magnetic flux. The body 16 rotates synchronously. That is, they are engaged.
また、ループ経路L_ON1,L_ON2は固定体12と第1回転体14を通過(鎖交)することから、両者は磁気的に結合される。しかしながら上述したように、ボビン18の大径円環部24A(極性可変磁石22A)の外周面と第1回転体ヨーク30Aの内周面は周方向に沿って極性が同一の磁束のみが通過し、同様にしてボビン18の大径円環部24B(極性可変磁石22B)の外周面と第2回転体ヨーク30Bの内周面も周方向(回転方向)に沿って極性が同一の磁束のみが通過する。 Further, since the loop paths L_ON1 and L_ON2 pass through (chain) the fixed body 12 and the first rotating body 14, they are magnetically coupled to each other. However, as described above, only magnetic fluxes having the same polarity pass along the circumferential direction on the outer peripheral surface of the large-diameter annular portion 24A (variable polarity magnet 22A) of the bobbin 18 and the inner peripheral surface of the first rotating body yoke 30A. Similarly, the outer peripheral surface of the large-diameter annular portion 24B (variable polarity magnet 22B) of the bobbin 18 and the inner peripheral surface of the second rotating body yoke 30B also have only magnetic fluxes having the same polarity along the circumferential direction (rotation direction). pass.
その上、ボビン18の大径円環部24A(極性可変磁石22A)の外周面と第1回転体ヨーク30Aの内周面、及び、ボビン18の大径円環部24B(極性可変磁石22B)の外周面と第2回転体ヨーク30Bの内周面とのギャップ幅W1は周方向(回転方向)に沿って一定となるように形成される。その結果、周方向に沿った磁束分布が発生しないため、回転の「引っ掛かり」となるような渦電流の発生が抑制され、第1回転体14及び第2回転体16の円滑な回転が可能となる。 Further, the outer peripheral surface of the large-diameter annular portion 24A (polarity variable magnet 22A) of the bobbin 18 and the inner peripheral surface of the first rotating body yoke 30A, and the large-diameter annular portion 24B (polarity variable magnet 22B) of the bobbin 18 The gap width W1 between the outer peripheral surface of the magnet and the inner peripheral surface of the second rotating body yoke 30B is formed to be constant along the circumferential direction (rotational direction). As a result, since the magnetic flux distribution along the circumferential direction is not generated, the generation of eddy currents that cause "catch" of rotation is suppressed, and the first rotating body 14 and the second rotating body 16 can be smoothly rotated. Become.
<第1実施形態の変形例>
図1に示す例では、固定体12に極性可変磁石22A,22Bを設けていたが、この形態に限らない。例えば図7に例示するように、第1回転体14に極性可変磁石22A,22Bを設けてもよい。
<Modified example of the first embodiment>
In the example shown in FIG. 1, the fixed body 12 is provided with the polarity variable magnets 22A and 22B, but the present invention is not limited to this form. For example, as illustrated in FIG. 7, the first rotating body 14 may be provided with the polarity variable magnets 22A and 22B.
図7に示す例では、第1回転体ヨーク30Aの内周側に極性可変磁石22Aが設けられ、第1回転体ヨーク30Aの内周側に極性可変磁石22Bが設けられる。ここで便宜的に、第1回転体ヨーク30Aの一部として極性可変磁石22Aが含まれ、第2回転体ヨーク30Bの一部として極性可変磁石22Bが含まれるものとすると、第1回転体ヨーク30A(極性可変磁石22A)の内周面と大径円環部24Aの外周面のギャップ幅W1は、周方向に沿って等しくなるように形成される。同様にして、第2回転体ヨーク30B(極性可変磁石22B)の内周面と大径円環部24Bの外周面のギャップ幅W1は、周方向に沿って等しくなるように形成される。 In the example shown in FIG. 7, the polarity variable magnet 22A is provided on the inner peripheral side of the first rotating body yoke 30A, and the polarity variable magnet 22B is provided on the inner peripheral side of the first rotating body yoke 30A. Here, for convenience, assuming that the polarity variable magnet 22A is included as a part of the first rotating body yoke 30A and the polarity variable magnet 22B is included as a part of the second rotating body yoke 30B, the first rotating body yoke is included. The gap width W1 between the inner peripheral surface of the 30A (variable polarity magnet 22A) and the outer peripheral surface of the large-diameter annular portion 24A is formed so as to be equal along the circumferential direction. Similarly, the gap width W1 between the inner peripheral surface of the second rotating body yoke 30B (polarity variable magnet 22B) and the outer peripheral surface of the large-diameter annular portion 24B is formed so as to be equal along the circumferential direction.
また図1の例と同様に、極性可変磁石22A,22Bは、周方向に沿って同一の磁極のみが揃うように構成される。例えば極性可変磁石22Aは、図7に破線で示すように、相対的に外周側にはその周方向に沿って一方の磁極23A(例えばS極)が配置され、相対的に内周側にはその周方向に沿って他方の磁極23B(例えばN極)が配置される。 Further, as in the example of FIG. 1, the polarity variable magnets 22A and 22B are configured so that only the same magnetic poles are aligned along the circumferential direction. For example, in the variable polarity magnet 22A, as shown by a broken line in FIG. 7, one magnetic pole 23A (for example, S pole) is relatively arranged on the outer peripheral side along the circumferential direction, and relatively on the inner peripheral side. The other magnetic pole 23B (for example, N pole) is arranged along the circumferential direction.
極性可変磁石22Bは、極性可変磁石22Aとは磁極が反転するように配置される。すなわち、相対的に外周側にはその周方向に沿って一方の磁極23B(例えばN極)が配置され、相対的に内周側にはその周方向に沿って他方の磁極23A(例えばS極)が配置される。 The polarity variable magnet 22B is arranged so that the magnetic poles are reversed from those of the polarity variable magnet 22A. That is, one magnetic pole 23B (for example, N pole) is relatively arranged on the outer peripheral side along the circumferential direction, and the other magnetic pole 23A (for example, S pole) is relatively arranged on the inner peripheral side along the circumferential direction. ) Is placed.
図8の上段には図7の実施形態に係る係合装置10の開放時の例が示されており、図8下段には当該係合装置10の係合時の例が示されている。 The upper part of FIG. 8 shows an example when the engaging device 10 according to the embodiment of FIG. 7 is open, and the lower part of FIG. 8 shows an example when the engaging device 10 is engaged.
図8上段では、極性可変磁石22A,22Bと極性固定磁石32の極性が揃っており、これらの磁石の磁束は直列となり合成磁束となって破線で示すループ経路L_OFFを通過する。具体的には、極性可変磁石22A,22B及び極性固定磁石32の磁束は、極性固定磁石32→第1回転体ヨーク30A(極性可変磁石22A)→ボビン18→第2回転体ヨーク30B(極性可変磁石22B)→極性固定磁石32との経路を通過する。 In the upper part of FIG. 8, the polarities of the variable polarity magnets 22A and 22B and the polarity fixing magnet 32 are aligned, and the magnetic fluxes of these magnets are in series to form a combined magnetic flux and pass through the loop path L_OFF shown by the broken line. Specifically, the magnetic fluxes of the polar variable magnets 22A and 22B and the polar fixed magnet 32 are the polar fixed magnet 32 → the first rotating body yoke 30A (polarity variable magnet 22A) → bobbin 18 → the second rotating body yoke 30B (variable polarity). Magnet 22B) → Passes through the path with the polarity fixing magnet 32.
図8下段には極性反転後の係合時の様子が例示されている。この図の破線で示されているように、極性可変磁石22A,22Bの磁束と極性固定磁石32の磁束とが逆極性となるために、概念上並列に2種類のループ経路L_ON1,L_ON2が発生する。 The lower part of FIG. 8 illustrates the state of engagement after polarity reversal. As shown by the broken line in this figure, the magnetic fluxes of the variable polarity magnets 22A and 22B and the magnetic fluxes of the fixed polarity magnets 32 have opposite polarities, so that two types of loop paths L_ON1 and L_ON2 are conceptually generated in parallel. To do.
すなわち、極性固定磁石32→第1回転体ヨーク30A→第2回転体16→第2回転体ヨーク30B→極性固定磁石32との経路を通過するループ経路L_ON1が形成される。また、第1回転体ヨーク30A(極性可変磁石22A)→第2回転体16→第2回転体ヨーク30B(極性可変磁石22B)→ボビン18→第1回転体ヨーク30A(極性可変磁石22A)との経路を通過するループ経路L_ON2が形成される。 That is, a loop path L_ON1 that passes through the path of the polarity fixing magnet 32 → the first rotating body yoke 30A → the second rotating body 16 → the second rotating body yoke 30B → the polarity fixing magnet 32 is formed. Further, the first rotating body yoke 30A (polarity variable magnet 22A) → the second rotating body 16 → the second rotating body yoke 30B (polarity variable magnet 22B) → bobbin 18 → the first rotating body yoke 30A (polarity variable magnet 22A). The loop path L_ON2 that passes through the path of the above is formed.
ループ経路L_ON1,L_ON2は第1回転体14及び第2回転体16を通過(鎖交)することから、両者は磁気的に結合される。さらに上述したように両者の対向面は周方向(回転方向)に沿ってギャップ幅W2が変化するように形成されているため、磁束変化を阻害するように、第1回転体14及び第2回転体16が同期して回転する。すなわち両者が係合される。 Since the loop paths L_ON1 and L_ON2 pass through (chain) the first rotating body 14 and the second rotating body 16, they are magnetically coupled to each other. Further, as described above, since the facing surfaces of the two are formed so that the gap width W2 changes along the circumferential direction (rotation direction), the first rotating body 14 and the second rotating body 14 and the second rotation so as to hinder the change in magnetic flux. The body 16 rotates synchronously. That is, they are engaged.
一方、ループ経路L_ON1,L_ON2は固定体12と第1回転体14を通過(鎖交)することから、両者は磁気的に結合される。しかしながら上述したように、ボビン18の大径円環部24Aの外周面と第1回転体ヨーク30A(極性可変磁石22A)の内周面は周方向に沿って極性が同一の磁束のみが通過し、同様にしてボビン18の大径円環部24Bの外周面と第2回転体ヨーク30B(極性可変磁石22B)の内周面も周方向(回転方向)に沿って極性が同一の磁束のみが通過する。 On the other hand, since the loop paths L_ON1 and L_ON2 pass through (chain) the fixed body 12 and the first rotating body 14, they are magnetically coupled. However, as described above, only magnetic fluxes having the same polarity pass along the circumferential direction on the outer peripheral surface of the large-diameter annular portion 24A of the bobbin 18 and the inner peripheral surface of the first rotating body yoke 30A (polarity variable magnet 22A). Similarly, the outer peripheral surface of the large-diameter annular portion 24B of the bobbin 18 and the inner peripheral surface of the second rotating body yoke 30B (polarity variable magnet 22B) also have only magnetic fluxes having the same polarity along the circumferential direction (rotation direction). pass.
その上、ボビン18の大径円環部24Aの外周面と第1回転体ヨーク30A(極性可変磁石22A)の内周面、及び、ボビン18の大径円環部24Bの外周面と第2回転体ヨーク30B(極性可変磁石22B)の内周面とのギャップ幅W1は周方向(回転方向)に沿って一定となるように形成される。その結果、周方向に沿った磁束分布が発生しないため、回転の「引っ掛かり」となるような渦電流の発生が抑制され、第1回転体14及び第2回転体16の円滑な回転が可能となる。 Further, the outer peripheral surface of the large-diameter annular portion 24A of the bobbin 18, the inner peripheral surface of the first rotating body yoke 30A (polarity variable magnet 22A), and the outer peripheral surface of the large-diameter annular portion 24B of the bobbin 18 and the second. The gap width W1 of the rotating body yoke 30B (variable polarity magnet 22B) with the inner peripheral surface is formed so as to be constant along the circumferential direction (rotation direction). As a result, since the magnetic flux distribution along the circumferential direction is not generated, the generation of eddy currents that cause "catch" of rotation is suppressed, and the first rotating body 14 and the second rotating body 16 can be smoothly rotated. Become.
<第2実施形態>
図9には、第2実施形態に係る係合装置50が例示されている。係合装置50は第1回転体52と第2回転体54とを軸方向(Y軸方向)に相対移動可能なアクチュエータ装置として機能する。係合装置50は、固定体56、第1回転体52、第2回転体54、及びガイド部材58を備える。
<Second Embodiment>
FIG. 9 illustrates the engaging device 50 according to the second embodiment. The engaging device 50 functions as an actuator device capable of relatively moving the first rotating body 52 and the second rotating body 54 in the axial direction (Y-axis direction). The engaging device 50 includes a fixed body 56, a first rotating body 52, a second rotating body 54, and a guide member 58.
固定体56は、ボビン60、コイル62、極性固定磁石64(第1永久磁石)、及び、極性可変磁石66A,66B(第2永久磁石)を備える。ボビン60は、小径円柱部68とその軸方向(Y軸方向)両端に大径円環部70A,70Bを備える。また大径円環部70Aの一部として極性可変磁石66Aが設けられ、大径円環部70Bの一部として極性可変磁石66Bが設けられる。ボビン60の、極性可変磁石66A,66B以外の部分はヨークとして機能する。すなわち当該部分は高透磁率材料から構成され、例えば低炭素鋼等の軟質磁性材料から構成される。 The fixed body 56 includes a bobbin 60, a coil 62, a polarity fixing magnet 64 (first permanent magnet), and polarity variable magnets 66A and 66B (second permanent magnet). The bobbin 60 includes a small-diameter cylindrical portion 68 and large-diameter annular portions 70A and 70B at both ends in the axial direction (Y-axis direction) thereof. Further, a polarity variable magnet 66A is provided as a part of the large diameter ring portion 70A, and a polarity variable magnet 66B is provided as a part of the large diameter ring portion 70B. The portion of the bobbin 60 other than the variable polarity magnets 66A and 66B functions as a yoke. That is, the portion is made of a high magnetic permeability material, and is made of a soft magnetic material such as low carbon steel.
極性可変磁石66A,66Bは、極性固定磁石64よりも着磁し易いという特性を有する。後述するように、極性可変磁石66A,66Bは、コイル62から生じる磁界によってその極性が反転させられる。極性可変磁石66A,66Bは、例えばアルニコ磁石から構成される。 The variable polarity magnets 66A and 66B have a characteristic that they are easier to magnetize than the fixed polarity magnets 64. As will be described later, the polarities of the variable polarity magnets 66A and 66B are reversed by the magnetic field generated from the coil 62. The variable polarity magnets 66A and 66B are composed of, for example, alnico magnets.
また極性可変磁石66A,66Bは、周方向に沿って同一の磁極のみが揃うように構成される。例えば極性可変磁石66Aは、図9に破線で示すように、相対的に外周側にはその周方向に沿って一方の磁極67A(例えばS極)が配置され、相対的に内周側にはその周方向に沿って他方の磁極67B(例えばN極)が配置される。この構成によって、ボビン60の大径円環部70Aの外周面と第1回転体52の内周面は周方向に沿って極性が同一の磁束のみが通過するようになる。 Further, the polarity variable magnets 66A and 66B are configured so that only the same magnetic poles are aligned along the circumferential direction. For example, in the variable polarity magnet 66A, as shown by the broken line in FIG. 9, one magnetic pole 67A (for example, S pole) is relatively arranged on the outer peripheral side along the circumferential direction, and relatively on the inner peripheral side. The other magnetic pole 67B (for example, N pole) is arranged along the circumferential direction. With this configuration, only magnetic fluxes having the same polarity pass along the circumferential direction on the outer peripheral surface of the large-diameter annular portion 70A of the bobbin 60 and the inner peripheral surface of the first rotating body 52.
極性可変磁石66Bは、極性可変磁石66Aとは磁極が反転するように配置される。すなわち、相対的に外周側にはその周方向に沿って一方の磁極67B(例えばN極)が配置され、相対的に内周側にはその周方向に沿って他方の磁極67A(例えばS極)が配置される。この構成によって、ボビン60の大径円環部70Bの外周面と第2回転体54の内周面は周方向(回転方向)に沿って極性が同一の磁束のみが通過する。 The polarity variable magnet 66B is arranged so that the magnetic poles are reversed from those of the polarity variable magnet 66A. That is, one magnetic pole 67B (for example, N pole) is relatively arranged on the outer peripheral side along the circumferential direction, and the other magnetic pole 67A (for example, S pole) is relatively arranged on the inner peripheral side along the circumferential direction. ) Is placed. With this configuration, only magnetic fluxes having the same polarity pass along the circumferential direction (rotational direction) on the outer peripheral surface of the large-diameter annular portion 70B of the bobbin 60 and the inner peripheral surface of the second rotating body 54.
コイル62は、ボビン60の小径円柱部68に巻き回される。コイル62は接続配線72を介して外部の電源(図示せず)に接続される。コイル62の小径円柱部68への巻数は1回でも複数回でもよい。 The coil 62 is wound around the small-diameter cylindrical portion 68 of the bobbin 60. The coil 62 is connected to an external power source (not shown) via the connection wiring 72. The number of turns of the coil 62 around the small-diameter cylindrical portion 68 may be one or a plurality of turns.
極性固定磁石64は、例えばコイル62よりも外周側に設けられる。例えば極性固定磁石64は、大径円環部70Aと大径円環部70Bとの間を軸方向に接続(連結)するように設けられる。つまり、大径円環部70A,70B間のギャップを連絡(接続)する機能を極性固定磁石64が備えている。極性固定磁石64は例えば円環状に形成される。極性固定磁石64は例えばネオジム磁石から構成される。 The polarity fixing magnet 64 is provided on the outer peripheral side of the coil 62, for example. For example, the polarity fixing magnet 64 is provided so as to connect (connect) the large-diameter ring portion 70A and the large-diameter ring portion 70B in the axial direction. That is, the polarity fixing magnet 64 has a function of connecting (connecting) the gap between the large diameter ring portions 70A and 70B. The polarity fixing magnet 64 is formed, for example, in an annular shape. The polarity fixing magnet 64 is composed of, for example, a neodymium magnet.
第1回転体52は、ボビン60と同軸(Y軸)の略円環部材である。その内周面はギャップを設けて(介して)固定体56の大径円環部70Aの外周面と対向している。第1回転体52の内周面と大径円環部70Aの外周面とのギャップ幅W1は周方向に沿って一定となる(等しくなる)ように構成される。これにより、周方向に沿って磁気抵抗が一様となるので、周方向に沿ったギャップによる磁束変化が抑制され、その結果、渦電流の発生が抑制される。 The first rotating body 52 is a substantially annular member coaxial (Y-axis) with the bobbin 60. The inner peripheral surface thereof is provided with a gap (via) and faces the outer peripheral surface of the large-diameter annular portion 70A of the fixed body 56. The gap width W1 between the inner peripheral surface of the first rotating body 52 and the outer peripheral surface of the large-diameter annular portion 70A is configured to be constant (equal) along the circumferential direction. As a result, the magnetic resistance becomes uniform along the circumferential direction, so that the change in magnetic flux due to the gap along the circumferential direction is suppressed, and as a result, the generation of eddy current is suppressed.
例えば、大径円環部70Aの外周面と第1回転体52の内周面は、側面視(Y軸方向視)で同心円となるように形成される。第1回転体52は図示しない軸受け等により、その内周面と大径円環部70Aの外周面のギャップ幅W1が維持される。 For example, the outer peripheral surface of the large-diameter annular portion 70A and the inner peripheral surface of the first rotating body 52 are formed so as to be concentric circles in a side view (Y-axis direction view). The gap width W1 between the inner peripheral surface of the first rotating body 52 and the outer peripheral surface of the large-diameter annular portion 70A is maintained by a bearing or the like (not shown).
第1回転体52は、軸周り(Y軸周り)に回転可能である他に、軸方向(Y軸方向)に沿って直動可能となっている。例えば第1回転体52は、ガイド部材58にガイドされつつ、軸方向に直動する。第1回転体52はリターンスプリング76によって第2回転体54とは離間する側に付勢される。後述するように、係合装置50の係合時には、この付勢力に抗するように第1回転体52が第2回転体54に向かって直動する。 The first rotating body 52 can rotate around an axis (around the Y axis) and can move linearly along the axial direction (Y axis direction). For example, the first rotating body 52 moves linearly in the axial direction while being guided by the guide member 58. The first rotating body 52 is urged by the return spring 76 to a side separated from the second rotating body 54. As will be described later, when the engaging device 50 is engaged, the first rotating body 52 moves linearly toward the second rotating body 54 so as to resist this urging force.
また第1回転体52の、第2回転体54と対向する側面73には、周方向に沿って複数の突起(ドグ)が設けられた突起列74Aが設けられている。突起列74Aにおける突起幅は、第2回転体54の側面(対向面)に設けられた突起列74Bのピッチ(間隔)と同一であり、また突起列74Aにおけるピッチは、突起列74Bの突起幅と同一であることが好適である。このような構成を備えることで、第1回転体52と第2回転体54とが軸方向に沿って近接したときに突起列74A,74B同士が噛み合い、同期した回転駆動が可能となる。 Further, on the side surface 73 of the first rotating body 52 facing the second rotating body 54, a protrusion row 74A provided with a plurality of protrusions (dogs) along the circumferential direction is provided. The protrusion width in the protrusion row 74A is the same as the pitch (interval) of the protrusion row 74B provided on the side surface (opposing surface) of the second rotating body 54, and the pitch in the protrusion row 74A is the protrusion width of the protrusion row 74B. It is preferable that it is the same as. By providing such a configuration, when the first rotating body 52 and the second rotating body 54 are close to each other along the axial direction, the projection rows 74A and 74B mesh with each other, and synchronous rotation driving becomes possible.
ガイド部材58は、第1回転体52の外周面を覆うように設けられる略円筒形の部材である。ガイド部材58の内周面と第1回転体52の外周面とは例えば摺動によって相対移動可能となっている。つまり第1回転体52はガイド部材58によって軸方向にその動きをガイドされる。ガイド部材58のフランジ78にはリターンスプリング76の一端が接続される。リターンスプリング76は周方向に複数設けられていてもよい。またガイド部材58は、第1回転体52と同期して回転可能となっている。 The guide member 58 is a substantially cylindrical member provided so as to cover the outer peripheral surface of the first rotating body 52. The inner peripheral surface of the guide member 58 and the outer peripheral surface of the first rotating body 52 can be moved relative to each other by, for example, sliding. That is, the movement of the first rotating body 52 is guided in the axial direction by the guide member 58. One end of the return spring 76 is connected to the flange 78 of the guide member 58. A plurality of return springs 76 may be provided in the circumferential direction. Further, the guide member 58 can rotate in synchronization with the first rotating body 52.
第2回転体54は、ボビン60と同軸(Y軸)の略円筒部材である。その内周面はギャップを設けて固定体56の大径円環部70Bの外周面と対向している。第2回転体54の内周面と大径円環部70Bの外周面とのギャップ幅W1は周方向に沿って一定となる(等しくなる)ように構成される。これにより、周方向に沿って磁気抵抗が一様となるので、周方向に沿ったギャップによる磁束変化が抑制され、その結果、渦電流の発生が抑制される。 The second rotating body 54 is a substantially cylindrical member coaxial (Y-axis) with the bobbin 60. The inner peripheral surface thereof is provided with a gap and faces the outer peripheral surface of the large-diameter annular portion 70B of the fixed body 56. The gap width W1 between the inner peripheral surface of the second rotating body 54 and the outer peripheral surface of the large-diameter annular portion 70B is configured to be constant (equal) along the circumferential direction. As a result, the magnetic resistance becomes uniform along the circumferential direction, so that the change in magnetic flux due to the gap along the circumferential direction is suppressed, and as a result, the generation of eddy current is suppressed.
例えば、大径円環部70Bの外周面と第2回転体54の内周面は、側面視(Y軸方向視)で同心円となるように形成される。第2回転体54は図示しない軸受け等により、その内周面と大径円環部70Bの外周面のギャップ幅W1が維持される。 For example, the outer peripheral surface of the large-diameter annular portion 70B and the inner peripheral surface of the second rotating body 54 are formed so as to be concentric circles in a side view (Y-axis direction view). The gap width W1 between the inner peripheral surface of the second rotating body 54 and the outer peripheral surface of the large-diameter annular portion 70B is maintained by a bearing or the like (not shown).
第2回転体54は、軸方向(Y軸方向)に第1回転体52と隣接する。また第2回転体54は、軸周り(Y軸周り)に回転可能となっている。一方、第2回転体54は、第1回転体52とは異なり、軸方向の直動は規制される。 The second rotating body 54 is adjacent to the first rotating body 52 in the axial direction (Y-axis direction). Further, the second rotating body 54 is rotatable around an axis (around the Y axis). On the other hand, unlike the first rotating body 52, the second rotating body 54 is restricted from linear movement in the axial direction.
なおこの形態に限らずに、第2回転体54にもガイド部材58を設けて軸方向に直動可能としてもよい。また、第2回転体54のみにガイド部材58を設けて、第1回転体52の直動を規制してもよい。 Not limited to this form, the second rotating body 54 may also be provided with a guide member 58 so that it can move linearly in the axial direction. Further, the guide member 58 may be provided only on the second rotating body 54 to regulate the linear motion of the first rotating body 52.
第2回転体54の第1回転体52と対向する側面(対向面)には、周方向に沿って複数の突起(ドグ)が設けられた突起列74Bが設けられている。上述したように、突起列74Bにおける突起幅は、突起列74Aのピッチ(間隔)と同一であり、また突起列74Bにおけるピッチは、突起列74Aの突起幅と同一であることが好適である。 On the side surface (opposing surface) of the second rotating body 54 facing the first rotating body 52, a protrusion row 74B provided with a plurality of protrusions (dogs) along the circumferential direction is provided. As described above, it is preferable that the protrusion width in the protrusion row 74B is the same as the pitch (interval) of the protrusion row 74A, and the pitch in the protrusion row 74B is the same as the protrusion width of the protrusion row 74A.
図10〜図12には、第2実施形態に係る係合装置50の開放状態、磁極反転時、及び係合状態の様子が例示されている。なお図10〜図12はいずれも、図9の斜視図のZ−Y平面を示している。 10 to 12 illustrate the open state, the magnetic pole reversal, and the engaged state of the engaging device 50 according to the second embodiment. It should be noted that FIGS. 10 to 12 all show the ZZ plane of the perspective view of FIG.
図10には開放時の例が示されている。開放時には、第1回転体52及び第2回転体54の係合が解かれる。 FIG. 10 shows an example at the time of opening. At the time of opening, the first rotating body 52 and the second rotating body 54 are disengaged.
図10に示すように、極性可変磁石66A,66Bと極性固定磁石64の極性が揃っており、これらの磁石の磁束は直列に合成磁束となって破線で示すループ経路L_OFFを通過する。具体的には、極性可変磁石66A,66B及び極性固定磁石64の磁束は、極性固定磁石64→大径円環部70A→極性可変磁石66A→小径円柱部68→極性可変磁石66B→大径円環部70B→極性固定磁石64との経路を通過する。 As shown in FIG. 10, the polar variable magnets 66A and 66B and the polarity fixed magnet 64 have the same polarity, and the magnetic fluxes of these magnets form a combined magnetic flux in series and pass through the loop path L_OFF shown by the broken line. Specifically, the magnetic fluxes of the polar variable magnets 66A and 66B and the polar fixed magnet 64 are as follows: polar fixed magnet 64 → large diameter ring portion 70A → polar variable magnet 66A → small diameter cylindrical portion 68 → polar variable magnet 66B → large diameter circle. It passes through the path from the ring portion 70B to the polarity fixing magnet 64.
このように、極性可変磁石66A,66B及び極性固定磁石64の磁束は第1回転体52及び第2回転体54を通過(鎖交)しない。このため磁力によって両者は引き合わずに、リターンスプリング76によって第1回転体52は第2回転体54から軸方向(Y軸方向)に離間させられる。 As described above, the magnetic fluxes of the polar variable magnets 66A and 66B and the polar fixed magnet 64 do not pass (interlink) with the first rotating body 52 and the second rotating body 54. Therefore, the first rotating body 52 is separated from the second rotating body 54 in the axial direction (Y-axis direction) by the return spring 76 without attracting the two due to the magnetic force.
図11には極性反転時の様子が例示されている。コイル62に電流を供給して磁界を発生させることで、極性可変磁石66A,66Bの極性を反転させる。例えば図3のグラフより、動作点AとBの中間値を取る磁界をコイル62に発生させて、選択的に極性可変磁石66A,66Bの極性を反転させる。 FIG. 11 illustrates the state at the time of polarity reversal. By supplying a current to the coil 62 to generate a magnetic field, the polarities of the variable polarity magnets 66A and 66B are reversed. For example, from the graph of FIG. 3, a magnetic field having an intermediate value between the operating points A and B is generated in the coil 62 to selectively reverse the polarities of the polar variable magnets 66A and 66B.
図12には極性反転後の係合時の様子が例示されている。この図の破線で示されているように、極性可変磁石66A,66Bの磁束と極性固定磁石64の磁束とが逆極性となるために、概念上並列に2種類のループ経路L_ON1,L_ON2が発生する。 FIG. 12 illustrates the state of engagement after polarity reversal. As shown by the broken line in this figure, the magnetic fluxes of the variable polarity magnets 66A and 66B and the magnetic fluxes of the fixed polarity magnets 64 have opposite polarities, so that two types of loop paths L_ON1 and L_ON2 are conceptually generated in parallel. To do.
すなわち、極性固定磁石64→大径円環部70A→第1回転体52→第2回転体54→大径円環部70B→極性固定磁石64との経路を通過するループ経路L_ON1が形成される。また、極性可変磁石66A→大径円環部70A→第1回転体52→第2回転体54→大径円環部70B→極性可変磁石66B→小径円柱部68→極性可変磁石66Aとの経路を通過するループ経路L_ON2が形成される。 That is, a loop path L_ON1 that passes through the path of the polarity fixing magnet 64 → the large diameter ring portion 70A → the first rotating body 52 → the second rotating body 54 → the large diameter ring portion 70B → the polarity fixing magnet 64 is formed. .. Further, the path from the variable polarity magnet 66A → the large diameter annular portion 70A → the first rotating body 52 → the second rotating body 54 → the large diameter annular portion 70B → the variable polarity magnet 66B → the small diameter cylindrical portion 68 → the variable polarity magnet 66A. A loop path L_ON2 passing through is formed.
ループ経路L_ON1,L_ON2は第1回転体52及び第2回転体54を通過(鎖交)することから、両者は磁気的に結合され、互いに引き合う。このとき、リターンスプリング76の弾性力に抗して第1回転体52が軸方向(Y軸方向)に直動し、第2回転体54に近づく。さらに第1回転体52の突起列74Aと第2回転体54の突起列74Bとが噛み合い、両者が同期して回転移動する。 Since the loop paths L_ON1 and L_ON2 pass through (chain) the first rotating body 52 and the second rotating body 54, they are magnetically coupled and attract each other. At this time, the first rotating body 52 moves linearly in the axial direction (Y-axis direction) against the elastic force of the return spring 76 and approaches the second rotating body 54. Further, the protrusion row 74A of the first rotating body 52 and the protrusion row 74B of the second rotating body 54 mesh with each other, and both rotate and move in synchronization with each other.
このとき、ループ経路L_ON1,L_ON2によって、固定体56と第1回転体52及び第2回転体54とが磁気的に結合される。しかしながら上述したように、ボビン60の大径円環部70Aの外周面と第1回転体52の内周面は周方向に沿って極性が同一の磁束のみが通過し、同様にしてボビン60の大径円環部70Bの外周面と第2回転体54の内周面も周方向(回転方向)に沿って極性が同一の磁束のみが通過する。その上、ボビン60の大径円環部70Aの外周面と第1回転体52の内周面、及び、ボビン60の大径円環部70Bの外周面と第2回転体54の内周面とのギャップ幅W1は周方向(回転方向)に沿って一定となるように形成される。その結果、周方向に沿った磁束分布が発生しないため、回転の「引っ掛かり」となるような渦電流の発生が抑制され、第1回転体52及び第2回転体54の円滑な回転が可能となる。 At this time, the fixed body 56, the first rotating body 52, and the second rotating body 54 are magnetically coupled by the loop paths L_ON1 and L_ON2. However, as described above, only magnetic fluxes having the same polarity pass along the circumferential direction on the outer peripheral surface of the large-diameter annular portion 70A of the bobbin 60 and the inner peripheral surface of the first rotating body 52, and similarly, the bobbin 60 Only magnetic fluxes having the same polarity pass along the circumferential direction (rotational direction) of the outer peripheral surface of the large-diameter annular portion 70B and the inner peripheral surface of the second rotating body 54. Further, the outer peripheral surface of the large-diameter annular portion 70A of the bobbin 60 and the inner peripheral surface of the first rotating body 52, and the outer peripheral surface of the large-diameter annular portion 70B of the bobbin 60 and the inner peripheral surface of the second rotating body 54. The gap width W1 with and is formed to be constant along the circumferential direction (rotational direction). As a result, since the magnetic flux distribution along the circumferential direction is not generated, the generation of eddy currents that cause "catch" of rotation is suppressed, and the first rotating body 52 and the second rotating body 54 can be smoothly rotated. Become.
10,50 係合装置、12,56固定体、14,52 第1回転体、16,54 第2回転体、18,60 ボビン、20,62 コイル、22A,22B,66A,66B 極性可変磁石、24A,24B,70A,70B 大径円環部、26,68 小径円柱部、30A,30B 回転体ヨーク、32,64 極性固定磁石、74A,74B 突起列。 10,50 Engagement device, 12,56 fixed body, 14,52 first rotating body, 16,54 second rotating body, 18,60 bobbin, 20,62 coil, 22A, 22B, 66A, 66B polarity variable magnet, 24A, 24B, 70A, 70B Large diameter ring part, 26,68 small diameter column part, 30A, 30B rotating body yoke, 32,64 polar fixing magnet, 74A, 74B protrusion row.
Claims (8)
前記一対の大径円環部の一方の外周面とギャップを設けて内周面が対向する円環形状の第1回転体ヨークと、前記一対の大径円環部の他方とギャップを設けて内周面が対向する円環形状の第2回転体ヨークと、を備える第1回転体と、
前記第1及び第2回転体ヨークの外周面とのギャップ幅が周方向に沿って異なるように形成された内周面を備える第2回転体と、
を備え、
前記固定体及び前記第1回転体の少なくとも一方には、第1永久磁石と、前記第1永久磁石よりも着磁し易い第2永久磁石が設けられ、
前記コイルから生じる磁界によって前記第2永久磁石の磁極が反転し、前記第2永久磁石の磁極反転に応じて、前記第1及び第2永久磁石の磁束が前記第2回転体を通過する係合状態と、前記第1及び第2永久磁石の磁束が前記第2回転体を通過しない開放状態とに切り替え可能な、
係合装置であって、
前記一対の大径円環部の外周面と、前記第1及び第2回転体ヨークの内周面とのギャップ幅は、周方向に沿って等しくなるように形成され、
前記一対の大径円環部の一方の外周面と前記第1回転体ヨークの内周面との間、及び、前記一対の大径円環部の他方と前記第2回転体ヨークの内周面との間には、周方向に沿って極性が同一の磁束のみが通過する、
係合装置。 It was wound between a bobbin having a small-diameter cylindrical portion and a pair of large-diameter annular portions provided at both ends in the axial direction of the small-diameter cylindrical portion, and the pair of large-diameter annular portions of the small-diameter cylindrical portion. A fixed body with a coil,
A gap is provided between the outer peripheral surface of one of the pair of large-diameter annular portions and the ring-shaped first rotating body yoke whose inner peripheral surfaces face each other, and the other of the pair of large-diameter annular portions. A first rotating body including a ring-shaped second rotating body yoke whose inner peripheral surfaces face each other, and
A second rotating body having an inner peripheral surface formed so that the gap width between the first and second rotating body yokes and the outer peripheral surface is different along the circumferential direction.
With
At least one of the fixed body and the first rotating body is provided with a first permanent magnet and a second permanent magnet that is easier to magnetize than the first permanent magnet.
The magnetic field generated from the coil reverses the magnetic poles of the second permanent magnet, and the magnetic fluxes of the first and second permanent magnets pass through the second rotating body in response to the magnetic pole reversal of the second permanent magnet. It is possible to switch between the state and the open state in which the magnetic fields of the first and second permanent magnets do not pass through the second rotating body.
It ’s an engaging device,
The gap widths between the outer peripheral surfaces of the pair of large-diameter ring portions and the inner peripheral surfaces of the first and second rotating body yokes are formed to be equal along the circumferential direction.
Between one outer peripheral surface of the pair of large-diameter ring portions and the inner peripheral surface of the first rotating body yoke, and between the other of the pair of large-diameter ring portions and the inner circumference of the second rotating body yoke. Only magnetic fluxes of the same polarity pass along the circumferential direction between the surfaces.
Engagement device.
前記第1永久磁石は、前記第1回転体ヨークと前記第2回転体ヨークとを接続するようにして前記第1回転体に設けられる、係合装置。 The engaging device according to claim 1.
The first permanent magnet is an engaging device provided on the first rotating body so as to connect the first rotating body yoke and the second rotating body yoke.
前記第2永久磁石は、前記一対の大径円環部に設けられ、相対的に外周側であって周方向に沿って設けられた一方の磁極と、相対的に内周側であって周方向に沿って設けられた他方の磁極とを備える、係合装置。 The engaging device according to claim 1 or 2.
The second permanent magnet is provided on the pair of large-diameter ring portions, and has one magnetic pole that is relatively on the outer peripheral side and is provided along the circumferential direction, and is relatively on the inner peripheral side and is circumferential. Engagement device with the other magnetic pole provided along the direction.
前記第2永久磁石は、前記第1及び前記第2回転体ヨークに設けられ、相対的に外周側であって周方向に沿って設けられた一方の磁極と、相対的に内周側であって周方向に沿って設けられた他方の磁極とを備える、係合装置。 The engaging device according to claim 1 or 2.
The second permanent magnet is provided on the first and second rotating body yokes, and is relatively on the outer peripheral side and relatively on the inner peripheral side with one magnetic pole provided along the circumferential direction. An engaging device including the other magnetic pole provided along the circumferential direction.
前記一対の大径円環部の一方の外周面とギャップを設けて内周面が対向する円環形状の第1回転体と、
前記一対の大径円環部の他方の外周面とギャップを設けて内周面が対向する円環形状の第2回転体と、
前記第1及び第2回転体の少なくとも一方を軸方向にガイドするガイド部材と、
を備え、
前記固定体には、第1永久磁石と、前記第1永久磁石よりも着磁し易い第2永久磁石が設けられ、
前記コイルから生じる磁界によって前記第2永久磁石の磁極が反転し、前記第2永久磁石の磁極反転に応じて、前記第1及び第2永久磁石の磁束が前記第1及び第2回転体を通過して両者を係合させる係合状態と、前記第1及び第2永久磁石の磁束が前記第1及び第2回転体を通過しない開放状態とに切り替え可能な、
係合装置であって、
前記一対の大径円環部の外周面と、前記第1及び第2回転体の内周面とのギャップ幅は、周方向に沿って等しくなるように形成され、
前記一対の大径円環部の一方の外周面と前記第1回転体の内周面との間、及び、前記一対の大径円環部の他方と前記第2回転体の内周面との間には、周方向に沿って極性が同一の磁束のみが通過する、
係合装置。 It was wound between a bobbin having a small-diameter cylindrical portion and a pair of large-diameter annular portions provided at both ends in the axial direction of the small-diameter cylindrical portion, and the pair of large-diameter annular portions of the small-diameter cylindrical portion. A fixed body with a coil,
A ring-shaped first rotating body having a gap with one outer peripheral surface of the pair of large-diameter annular portions and facing the inner peripheral surfaces.
A ring-shaped second rotating body having a gap with the other outer peripheral surface of the pair of large-diameter annular portions and facing the inner peripheral surfaces.
A guide member that guides at least one of the first and second rotating bodies in the axial direction, and
With
The fixed body is provided with a first permanent magnet and a second permanent magnet that is easier to magnetize than the first permanent magnet.
The magnetic field generated from the coil reverses the magnetic poles of the second permanent magnet, and the magnetic fluxes of the first and second permanent magnets pass through the first and second rotating bodies in response to the magnetic pole reversal of the second permanent magnet. It is possible to switch between an engaged state in which the two are engaged with each other and an open state in which the magnetic fluxes of the first and second permanent magnets do not pass through the first and second rotating bodies.
It ’s an engaging device,
The gap widths between the outer peripheral surfaces of the pair of large-diameter ring portions and the inner peripheral surfaces of the first and second rotating bodies are formed to be equal along the circumferential direction.
Between one outer peripheral surface of the pair of large-diameter ring portions and the inner peripheral surface of the first rotating body, and between the other of the pair of large-diameter ring portions and the inner peripheral surface of the second rotating body. Only magnetic fluxes of the same polarity pass along the circumferential direction between them.
Engagement device.
前記第1永久磁石は、前記コイルよりも外周側であって前記一対の大径円環部を接続するようにして前記固定体に設けられる、係合装置。 The engaging device according to claim 5.
The first permanent magnet is an engaging device provided on the fixed body on the outer peripheral side of the coil so as to connect the pair of large-diameter ring portions.
前記第2永久磁石は、前記一対の大径円環部に設けられ、相対的に外周側であって周方向に沿って設けられた一方の磁極と、相対的に内周側であって周方向に沿って設けられた他方の磁極とを備える、係合装置。 The engaging device according to claim 5 or 6.
The second permanent magnet is provided on the pair of large-diameter ring portions, and has one magnetic pole that is relatively on the outer peripheral side and is provided along the circumferential direction, and is relatively on the inner peripheral side and is circumferential. Engagement device with the other magnetic pole provided along the direction.
前記第1回転体及び前記第2回転体のそれぞれの対向面には、互いに噛み合う突起列が形成されている、係合装置。
The engaging device according to claim 5 or 6.
An engaging device in which a row of protrusions that mesh with each other is formed on the facing surfaces of the first rotating body and the second rotating body.
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