JP2016171727A - Eddy current braking apparatus - Google Patents

Eddy current braking apparatus Download PDF

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JP2016171727A
JP2016171727A JP2015051578A JP2015051578A JP2016171727A JP 2016171727 A JP2016171727 A JP 2016171727A JP 2015051578 A JP2015051578 A JP 2015051578A JP 2015051578 A JP2015051578 A JP 2015051578A JP 2016171727 A JP2016171727 A JP 2016171727A
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eddy current
rotating body
disk
current brake
brake device
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JP6192176B2 (en
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雄真 鈴木
Yushin Suzuki
雄真 鈴木
欽吾 操谷
Kingo Sotani
欽吾 操谷
田中 寛之
Hiroyuki Tanaka
寛之 田中
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Kyosan Electric Manufacturing Co Ltd
Prospine Co Ltd
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Kyosan Electric Manufacturing Co Ltd
Prospine Co Ltd
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Abstract

PROBLEM TO BE SOLVED: To provide an electromagnetic braking apparatus capable of performing braking operation of a brake in a non-contact state and capable of downsizing the apparatus.SOLUTION: In an eddy current braking apparatus, a first rotor which is a mechanism requiring torques of winding or unwinding operation etc. in a treatment step of films, fibers, etc. and includes a permanent magnet group for generating eddy current braking and a second rotor including a conductor disk on the surface are arranged through a desired interspace. By arranging a plurality of projections of magnetic materials on the conductor disk at an equal pitch, an eddy current braking amount to be generated in accordance with a relative rotational speed difference between the two rotors can be increased and the apparatus can be also downsized.SELECTED DRAWING: Figure 1

Description

本発明は、フィルム類の加工処理工程における巻き取り又は巻出し操作等のトルクを必要とする機構において、電動機等の回転機械からの負荷を回転装置に所定のトルクを伝達する渦電流ブレーキに係り、特に渦電流による制動力を大幅に大きくできることを特徴とする渦電流ブレーキ装置に関するものである。
又、回転系を有する動力伝達装置に関し、伝達力が負荷によりスリップするブレーキ機能を有し、回転速度を減じる作用を内蔵する渦電流ブレーキ装置に関するものであり、特に相対回転速度に対する渦電流ブレーキ力が大きくでき且つ、ブレーキ力を調整可能にした渦電流ブレーキ装置に関するものである。
The present invention relates to an eddy current brake for transmitting a predetermined torque to a rotating device by applying a load from a rotating machine such as an electric motor in a mechanism that requires torque such as winding or unwinding operation in a film processing process. In particular, the present invention relates to an eddy current brake device characterized in that the braking force by eddy current can be greatly increased.
In addition, the present invention relates to a power transmission device having a rotating system, and relates to an eddy current braking device having a brake function in which the transmission force slips due to a load and has a built-in function of reducing the rotational speed. The present invention relates to an eddy current brake device in which the brake force can be adjusted and the brake force can be adjusted.

従来のこの種の渦電流ブレーキは多数の磁石がN.S交互に円盤上に配置された回転体(又は固定体)に、対向させて導体(例えばアルミ)を配置した固定盤(あるいは回転体)を有し、その回転体の回転数に応じた渦電流を導体に発生させることにより渦電流ブレーキを出現させている。(特許文献1参照。) A conventional eddy current brake of this type has a large number of magnets with N.P. S A rotating body (or stationary body) alternately arranged on a disk has a stationary board (or rotating body) in which a conductor (for example, aluminum) is disposed so as to face each other, and a vortex corresponding to the number of rotations of the rotating body An eddy current brake appears by generating a current in a conductor. (See Patent Document 1.)

特開平6−014523JP-A-6-014523

しかしながら、上述した特許文献1に提案されている渦電流ブレーキでは前記回転体の回転数に応じて発生する渦電流がもたらすブレーキ力が小さく、そのため必要とするブレーキ力を確保するためには形状が大きくなる等の欠点がある。又、それを補うため対向部分を複数にしてブレーキ力を確保することが提案されているが、この場合は構造が複雑になり、又、ブレーキ力を調整するため前記回転体と前記固定体との空隙の調整が簡便に行うことが出来ないなどの欠陥を有している。 However, in the eddy current brake proposed in Patent Document 1 described above, the braking force caused by the eddy current generated according to the number of rotations of the rotating body is small, and therefore the shape is required to ensure the necessary braking force. There are drawbacks such as an increase in size. In order to compensate for this, it has been proposed to secure a braking force by using a plurality of opposing portions. In this case, however, the structure becomes complicated, and the rotating body and the fixed body are used to adjust the braking force. There is a defect that the adjustment of the voids cannot be performed easily.

本発明は、上記課題を解決するため、強いブレーキ力を得られる渦電流式ブレーキ方法を盛り込んだ渦電流ブレーキ装置を提供することを目的とする。 In order to solve the above-described problems, an object of the present invention is to provide an eddy current brake device incorporating an eddy current brake method capable of obtaining a strong braking force.

上記目的を達成するために、本発明の請求項1では、磁性体からなる円盤状回転体の側面に、回転方向にN極とS極を交互に配設した第1回転体と、該第1回転体の磁石表面に対向して所定の隙間を有して導体円板を配設した磁性円盤からなる第2回転体が非接触にて対向させ、該2つの回転体間の相対回転速度差に応じて生じる渦電流によって両回転体間に制動力を発生させてなる渦電流ブレーキ装置において、前記第2回転体の磁性円盤の側面に所定の高さを有する突起部を設け、且つこの突起部を覆う形態で前記導体円板を埋設したことを特徴とする渦電流ブレーキ装置である。 In order to achieve the above object, according to claim 1 of the present invention, a first rotating body in which N poles and S poles are alternately arranged in a rotating direction on a side surface of a disk-shaped rotating body made of a magnetic body, A second rotating body composed of a magnetic disk having a predetermined gap and facing a magnet surface of one rotating body is opposed to each other in a non-contact manner, and a relative rotational speed between the two rotating bodies is set. In an eddy current brake device in which a braking force is generated between both rotating bodies by an eddy current generated according to the difference, a protrusion having a predetermined height is provided on a side surface of the magnetic disk of the second rotating body, and The eddy current brake device is characterized in that the conductor disk is embedded in a form to cover the protrusion.

また、本発明の請求項2に係る渦電流装置では、上述した請求項1において前記第1回転体の磁石極数と前記第2回転体の突起部の突起数が異なる数としたことを特徴とする請求項1記載の渦電流ブレーキ装置により問題の解決を図ったものである。 In the eddy current device according to claim 2 of the present invention, the number of magnet poles of the first rotating body and the number of protrusions of the projecting portion of the second rotating body are different from each other in claim 1 described above. The problem is solved by the eddy current brake device according to claim 1.

さらに、請求項3では、前記第2回転体の前記導体円板を比抵抗値の大小に応じて簡便に取り換え可能とし、渦電流ブレーキ力を容易に調整可能としたことを特徴とする請求項1乃至請求項2に記載の渦電流ブレーキ装置により問題の解決を図ったものである。 Further, in claim 3, the conductive disk of the second rotating body can be easily replaced according to the magnitude of the specific resistance value, and the eddy current braking force can be easily adjusted. The problem is solved by the eddy current brake device according to claim 1 or 2.

又、請求項4では、前記第1回転体と前記第2回転体のいずれかを固定としたことを特徴とする請求項1乃至、請求項2乃至、請求項3に記載の渦電流ブレーキ装置。 Further, in claim 4, the eddy current brake device according to any one of claims 1 to 2, wherein either the first rotating body or the second rotating body is fixed. .

一方、請求項5では 前記第1回転体の永久磁石を電磁石としたことを特徴とする請求項1乃至、請求項2に記載の渦電流ブレーキ装置。 On the other hand, in Claim 5, the permanent magnet of the said 1st rotary body was made into the electromagnet, The eddy current brake apparatus of Claim 1 thru | or 2 characterized by the above-mentioned.

本発明の渦電流ブレーキ装置においては、限られた形状、スペースにおいて特別な機構を設けることなく回転体間に作用する渦電流ブレーキ力を大幅に向上させることが可能となり、渦電流ブレーキ製品のブレーキ性能向上に大きく貢献する。又、渦電流カップリングとして用いれば、スリップが発生する限界トルクが高くなることで渦電流カップリングの設定幅が広がり、製品の応用範囲、用途の拡大にもつがなる等の効果を奏する。更に、渦電流ブレーキ特性と密接な関係にある導体円板の比抵抗値の(例えば銅板、1000番タイプのアルミ板、5000番タイプのアルミ板)等の異なる導体円板を適宜選定し、製品の限界トルク、ブレーキ量の要求に応じてネジ等で簡便に交換が可能で、その結果回転体間のギャップを調整するという複雑な機械構造にすることなく、ブレーキ力、伝達トルク特性の設定が容易で安価な渦電流ブレーキ装置が提供できる。 In the eddy current brake device of the present invention, it becomes possible to greatly improve the eddy current brake force acting between rotating bodies without providing a special mechanism in a limited shape and space. Contributes greatly to improved performance. Further, when used as an eddy current coupling, the setting torque of the eddy current coupling is widened by increasing the limit torque at which slip occurs, resulting in the effect of expanding the application range and use of products. Furthermore, different conductor discs such as the specific resistance values of the conductor discs that are closely related to the eddy current brake characteristics (for example, copper plates, 1000 type aluminum plates, 5000 type aluminum plates) are selected as appropriate, and the product It is possible to easily replace with screws etc. according to the demands of the limit torque and brake amount, and as a result, setting of brake force and transmission torque characteristics can be done without making a complicated mechanical structure of adjusting the gap between rotating bodies. An easy and inexpensive eddy current brake device can be provided.

本発明の実施の形態である渦電流ブレーキ装置の全体図で、 Aはその側面図、Bは側面の断面図。BRIEF DESCRIPTION OF THE DRAWINGS It is a general view of the eddy current brake device which is embodiment of this invention, A is the side view, B is sectional drawing of a side. 図1に示した第1回転体の正面図。The front view of the 1st rotary body shown in FIG. 図1に示した第2回転体の正面図。The front view of the 2nd rotary body shown in FIG. 従来例に基づく第2の回転体の側面の断面図。Sectional drawing of the side surface of the 2nd rotary body based on a prior art example. 従来例に基づく第2の回転体の正面図。The front view of the 2nd rotary body based on a prior art example. 回転体1及び回転体2間に発生する磁束の流れを示す説明図で、Aは本発明の構成で、Bは従来の一般的な構成を示す。It is explanatory drawing which shows the flow of the magnetic flux which generate | occur | produces between the rotary body 1 and the rotary body 2, A is a structure of this invention, B shows the conventional general structure. 渦電流ブレーキの第1回転体と第2回転体との相対回転速度差に対するブレーキ作用によって発生するトルク特性を示すグラフである。It is a graph which shows the torque characteristic which generate | occur | produces by the brake effect | action with respect to the relative rotational speed difference of the 1st rotary body of a eddy current brake, and a 2nd rotary body. 本発明の他の実施例でAは第1の回転体の正面図、Bはその断面図である。In another embodiment of the present invention, A is a front view of the first rotating body, and B is a sectional view thereof.

以下、本発明の実施の形態について詳細に説明する。 Hereinafter, embodiments of the present invention will be described in detail.

図1Aは、本発明に係る実施例の渦電流ブレーキ装置の側面図で、図1Bはその側面の断面図である。図において1は第1回転体で、磁性材の磁性円盤10、永久磁石群11及び、第1中心軸12で構成されている。又、該磁性円盤10は中心部に軸穴10aが開けられており、該軸穴10aを第1中心軸12が貫通して磁性盤10に平行キー13により連れまわり状態で固定されている。一方2は第2回転体2であって、中心部に軸穴20bを設けた磁性材からなる磁性円盤20、及び渦電流ブレーキを出現する導体円板21から構成され、該磁性円盤20の表面に図3に示す複数の突起部20aが設けてあり、該突起部20aの周囲を挟み込む態様で突起部20aと略同形状の穴を設けた前記導体円板21がネジ等(図示せず)で磁性円盤20に、磁性円盤の突起部20aと表面が略同一になるように固定されている。さらに該磁性円盤20の貫通穴20bに第2中心軸22が貫通し、平行キー23によって磁性円盤20に該軸22と連れまわり状態で固定している。 FIG. 1A is a side view of an eddy current brake device according to an embodiment of the present invention, and FIG. 1B is a side sectional view thereof. In the figure, reference numeral 1 denotes a first rotating body, which is composed of a magnetic disk 10 of magnetic material, a permanent magnet group 11 and a first central shaft 12. The magnetic disk 10 is provided with a shaft hole 10a in the center, and the first center shaft 12 passes through the shaft hole 10a and is fixed to the magnetic disk 10 by a parallel key 13 in a rotating state. On the other hand, reference numeral 2 denotes a second rotating body 2, which is composed of a magnetic disk 20 made of a magnetic material having a shaft hole 20 b in the center and a conductive disk 21 in which an eddy current brake appears, and the surface of the magnetic disk 20. Is provided with a plurality of protrusions 20a shown in FIG. 3, and the conductor disk 21 provided with holes having substantially the same shape as the protrusions 20a in a manner sandwiching the periphery of the protrusions 20a is a screw or the like (not shown). The magnetic disk 20 is fixed so that the surface thereof is substantially the same as the protrusion 20a of the magnetic disk. Further, the second central shaft 22 passes through the through hole 20 b of the magnetic disk 20, and is fixed to the magnetic disk 20 with the shaft 22 by a parallel key 23.

図2は上述した回転体1の正面図で、該磁性円盤10の表面には、永久磁石11a(表面がN極)と永久磁石11b(表面がS極)が磁性円盤10の中心に設けた軸穴10aに対して回転方向に等間隔で交互に接着剤等で配設している状態を示している。 FIG. 2 is a front view of the rotating body 1 described above. On the surface of the magnetic disk 10, a permanent magnet 11 a (surface is N pole) and a permanent magnet 11 b (surface is S pole) are provided at the center of the magnetic disk 10. A state is shown in which the shaft holes 10a are alternately disposed with an adhesive or the like at regular intervals in the rotation direction.

又、図3は前述した第2回転体の正面図で、磁性円盤20に設けた前記突起部20a・・・は前記中心軸22に対して回転方向に等間隔に設けてあり、前述したように該突起部20aとの周囲を挟み込む態様で突起部20aと略同形状の穴を設けた前記導体円板21が磁性円盤20に挿設されている状態を示している。 FIG. 3 is a front view of the second rotating body described above. The protrusions 20a... Provided on the magnetic disk 20 are provided at equal intervals in the rotational direction with respect to the central shaft 22, as described above. The conductor disk 21 provided with a hole having substantially the same shape as the protrusion 20a in a manner sandwiching the periphery of the protrusion 20a is inserted into the magnetic disk 20.

このように第1回転体1の永久磁石群11に対して、第2回転体の導体円板21と突起部20aの表面が対向する態様で所定の隙間を有して配置することによって、この2つの回転体の回転速度差に応じて、前記永久磁石11の磁束が第2回転体の突起部20aに集中した磁束の流れとなり、この磁束を打ち消すように、前記導体円盤21に渦電流が発現することによって第1回転体と第2回転体間に渦電流ブレーキとして作用する。 In this manner, the permanent magnet group 11 of the first rotating body 1 is arranged with a predetermined gap in such a manner that the conductor disk 21 of the second rotating body and the surface of the protrusion 20a face each other. Depending on the rotational speed difference between the two rotating bodies, the magnetic flux of the permanent magnet 11 becomes a flow of magnetic flux concentrated on the protrusion 20a of the second rotating body, and an eddy current is generated in the conductor disk 21 so as to cancel the magnetic flux. By acting, it acts as an eddy current brake between the first rotating body and the second rotating body.

図4及び、図5は、第2回転体2を一般的な従来例に基づき構成した従来例の第2回転体3であって、図4はその側面の断面図、図5は正面図である。図において、3は従来の第2の回転体で、磁性円盤30と、該磁性円盤30の側面に例えば接着剤等で固着した導体円板31から構成されている。尚、第1回転体1は上述した本発明に係る渦電流ブレーキ装置で説明した回転体と同じである。図に示すように該第2回転体3は、前述した本発明の実施例に係る第2回転体2と同様に、第1回転体1の永久磁石群11に対向する形態で配置することで渦電流ブレーキを構成されているが、前記本発明による前記第2回転体と異なる点は、磁気円盤30には突起がなく、該導体円板31の表面が、前記第1回転体1の永久磁石群11と対向し、この永久磁石群11の磁束は導体円板31を経由して該永久磁石群11内の隣り合う異極性の永久磁石と磁気回路を形成する。しかし、導体円板は磁性材に比べ透磁率が大幅に低く、そのため、磁束の集中が弱く、2つの回転体間の隙間にも分流した磁束となり、その結果前述の本発明による第2回転体の導体円盤21に流れる渦電流に比べて導体円盤31に流れる渦電流も少なく、渦電流ブレーキ力が弱いものになっている。 4 and 5 show a second rotating body 3 of a conventional example in which the second rotating body 2 is configured based on a general conventional example. FIG. 4 is a sectional view of the side surface, and FIG. 5 is a front view. is there. In the figure, reference numeral 3 denotes a conventional second rotating body, which is composed of a magnetic disk 30 and a conductive disk 31 fixed to the side surface of the magnetic disk 30 with, for example, an adhesive. In addition, the 1st rotary body 1 is the same as the rotary body demonstrated with the eddy current brake apparatus which concerns on this invention mentioned above. As shown in the drawing, the second rotating body 3 is arranged in a form facing the permanent magnet group 11 of the first rotating body 1 in the same manner as the second rotating body 2 according to the embodiment of the present invention described above. Although an eddy current brake is configured, the magnetic disk 30 has no protrusions, and the surface of the conductive disk 31 is a permanent part of the first rotating body 1 except for the second rotating body according to the present invention. Opposing to the magnet group 11, the magnetic flux of the permanent magnet group 11 forms a magnetic circuit with the adjacent permanent magnets in the permanent magnet group 11 via the conductor disk 31. However, the magnetic permeability of the conductor disk is significantly lower than that of the magnetic material, so that the concentration of the magnetic flux is weak, and the magnetic flux is divided into the gap between the two rotating bodies. As a result, the second rotating body according to the present invention described above is obtained. The eddy current flowing in the conductor disk 31 is less than the eddy current flowing in the conductor disk 21, and the eddy current braking force is weak.

この状況を図6に図示した。図6Aは本発明の第1回転体1と第2回転体の磁束の流れを示しており、図6Bは一般的な従来例を模試したものである。図6Aでは前述したように、永久磁石群11の永久磁石11a(先端がN極)の表面から磁性円盤20の突起部20aに向う磁束の経路が支配的となり磁性円盤20の内部を経由して隣の突起部20aから、永久磁石群11の永久磁石11b(先端がS極)に戻るような磁気回路が形成され、この磁束密度の変化に応じて、これを打ち消す様に導体円板に渦電流が流れてこの渦電流による渦電流損がブレーキ力となり、この結果この2つの回転系には相対的な回転速度差に応じた強い渦電流ブレーキ力が発生する。図6Bは一般的な従来例の磁束の流れを示したもので、前述したような磁性円盤30に突起部(ツースヨーク)がないため、磁束の集中がおこらず、結果的に出現する渦電流も少なく、従って、渦電流ブレーキ力は小さい。尚、図6A、及び図6Bに示す、隙間gap1及び隙間gap2は同一距離とする。 This situation is illustrated in FIG. FIG. 6A shows the flow of magnetic flux of the first rotating body 1 and the second rotating body of the present invention, and FIG. 6B is a trial of a general conventional example. In FIG. 6A, as described above, the path of the magnetic flux from the surface of the permanent magnet 11 a (the tip is N pole) of the permanent magnet group 11 toward the protrusion 20 a of the magnetic disk 20 becomes dominant and passes through the inside of the magnetic disk 20. A magnetic circuit is formed from the adjacent protrusion 20a so as to return to the permanent magnet 11b (the tip is the S pole) of the permanent magnet group 11, and the conductor disk is vortexed so as to cancel it according to the change in the magnetic flux density. An electric current flows and the eddy current loss due to the eddy current becomes a braking force. As a result, a strong eddy current braking force corresponding to a relative rotational speed difference is generated in the two rotating systems. FIG. 6B shows the flow of magnetic flux in a general conventional example. Since there is no protrusion (tooth yoke) in the magnetic disk 30 as described above, the magnetic flux does not concentrate and the resulting eddy current also appears. Therefore, the eddy current braking force is small. Note that the gap gap1 and the gap gap2 shown in FIGS. 6A and 6B have the same distance.

図7はこの渦電流ブレーキ特性(又は伝達トルク)を本発明の実施例と従来例との特性比較をした図であって、横軸は2つの回転体間の相対回転速度差で、縦軸はトルク(渦電流ブレーキ力をトルクとして表す)である。図からわかるように相対回転速度差に対するブレーキ力(トルク)は本発明の突起部(ツースヨーク)ありの場合が、従来例の突起部無に比べて約2倍大きいことがわかる。 尚、特に図示しないが各種実験結果から、永久磁石の極数と突起部の数は突起部数が多い方がより望ましい。 FIG. 7 is a diagram comparing the eddy current brake characteristics (or transmission torque) between the embodiment of the present invention and the conventional example, where the horizontal axis is the relative rotational speed difference between the two rotating bodies, and the vertical axis. Is torque (the eddy current braking force is expressed as torque). As can be seen from the figure, the braking force (torque) with respect to the relative rotational speed difference is about twice as large in the case with the protrusion (tooth yoke) of the present invention as compared with the case without the protrusion in the conventional example. Although not particularly shown, from the results of various experiments, it is more desirable that the number of poles and the number of protrusions of the permanent magnet is larger.

図8は本発明による他の実施例であって、図1に示した第1回転体の永久磁石群11を電磁石式にしたものであり、図8Aはその正面図、図8Bはその側面の断面図である。図において、4は磁性円盤で、その側面にはコイル42a、42bが該磁性円盤の中心に対して軸回転方向に互いに等間隔に42a、42b、42a、42b・・・と配列して、回路基盤41に固定してある。該コイルの端末の接続は、図示しないが例えばコイル42a群は9個が直列に接続され、その両端に直流電源の出力側に接続され直流電圧が印加される。又、同様にコイル42b群も9個が直列に接続され、その両端には直流電圧が印加される。この印加電圧の正負の極性によりコイルに流れる電流の方向を設定してコイル42a、42bのコイル表面の極性が決定され、コイル42a群とコイル42b群の表面の磁極が例えばコイル42a表面がN極又、コイル42bの表面がS極と異なる極性に励磁され、図1に示した永久磁石のN極、S極の役目を果すことで渦電流ブレーキの機能を発現する。尚、図では各コイルの中心に磁性体は設けていないが、必要に応じて、適当な磁性体を設けて磁極の磁力を増やすことも可能である。 FIG. 8 shows another embodiment of the present invention, in which the permanent magnet group 11 of the first rotating body shown in FIG. 1 is an electromagnet type, FIG. 8A is a front view thereof, and FIG. 8B is a side view thereof. It is sectional drawing. In the figure, reference numeral 4 denotes a magnetic disk, and coils 42a and 42b are arranged on the side thereof as 42a, 42b, 42a, 42b... At equal intervals in the axial rotation direction with respect to the center of the magnetic disk. It is fixed to the base 41. Although connection of the terminal of the coil is not shown, for example, nine coils 42a are connected in series, and both ends thereof are connected to the output side of the DC power source and a DC voltage is applied. Similarly, nine coils 42b are connected in series, and a DC voltage is applied to both ends thereof. The direction of the current flowing through the coil is set according to the polarity of the applied voltage to determine the polarity of the coil surfaces of the coils 42a and 42b. The magnetic poles on the surfaces of the coils 42a and 42b are, for example, N poles on the surface of the coil 42a. Further, the surface of the coil 42b is excited to have a polarity different from that of the south pole, and the function of the eddy current brake is exhibited by fulfilling the roles of the north pole and south pole of the permanent magnet shown in FIG. In the figure, no magnetic material is provided at the center of each coil, but if necessary, an appropriate magnetic material can be provided to increase the magnetic force of the magnetic poles.

以上、本発明の実施例では渦電流を発現する永久磁石盤と導体盤の各回転体を円盤型としたが、これを円筒型とした場合に比べて円盤型の利点は、対向する2つの回転体間の隙間を調整、設定することで簡便に2つの回転体間の相対回転速度差に応じた所望の渦電流ブレーキ力が得られる点にあるが、この隙間の調整距離に対する渦電流ブレーキ力の特性を磁気円盤上の永久磁石の極数の変更することによって急峻にしたり、なだらかにすることが、容易に設定できる等の利点がある。例えば永久磁石の極数を多くすること、2つの回転体間の回転速度差と渦電流ブレーキ力のブレーキ特性を急峻となる。これにより前記2つの回転体間の隙間を渦電流ブレーキが作用しない距離に離すことで渦電流クラッチとしても実用化も可能となる。 As described above, in the embodiment of the present invention, each rotating body of the permanent magnet board and the conductor board that generates the eddy current is a disk type, but the advantages of the disk type compared to the case where it is a cylindrical type are two opposing ones. By adjusting and setting the gap between the rotating bodies, the desired eddy current braking force can be easily obtained according to the relative rotational speed difference between the two rotating bodies. There is an advantage that the force characteristic can be easily set by making it steep or gentle by changing the number of poles of the permanent magnet on the magnetic disk. For example, increasing the number of poles of the permanent magnet makes the braking characteristics of the rotational speed difference between the two rotating bodies and the eddy current braking force steep. Accordingly, the gap between the two rotating bodies can be put to practical use as an eddy current clutch by separating the gap between the two rotators at a distance where the eddy current brake does not act.

以上説明したように、本発明に係る電磁ブレーキ装置は、2つの回転体間の互いの作用面が所望の隙間を有して非接触で対向する態様で設けられ、この作用面の相対回転速度差に応じたブレーキ力が限られたスペースの中でもより大きなブレーキ力が得られることから、例えばフィルムやガラス繊維、又炭素繊維等の巻取り、巻出し等の整列、たわみ取等の用途として広い利用価値がある。 As described above, the electromagnetic brake device according to the present invention is provided in such a manner that the working surfaces between the two rotating bodies face each other in a non-contact manner with a desired gap, and the relative rotational speed of the working surfaces. Since a larger braking force can be obtained even in a space where the braking force corresponding to the difference is limited, for example, film, glass fiber, carbon fiber winding, unwinding alignment, bending removal, etc. are wide There is utility value.

1 第1回転体
10 磁性円盤
11 永久磁石群
12 中心軸
13 キー
2 第2回転体
20 磁性円盤
20a 突起部(ツースヨーク)
21 導体円板
22 中心軸
23 キー
3 第2回転体
30 磁性円盤
31 導体円板
4 電磁石円盤
40 回路基盤ホルダー
41 回路基盤
42a 励磁コイル
42b 励磁コイル
DESCRIPTION OF SYMBOLS 1 1st rotary body 10 Magnetic disk 11 Permanent magnet group 12 Central axis 13 Key 2 2nd rotary body 20 Magnetic disk 20a Protrusion part (tooth yoke)
21 Conductor disk 22 Center axis 23 Key 3 Second rotating body 30 Magnetic disk 31 Conductor disk 4 Electromagnetic disk 40 Circuit board holder 41 Circuit board 42a Excitation coil 42b Excitation coil

Claims (5)

磁性体からなる円盤状回転体の側面に、回転方向にN極とS極を交互に配設した第1回転体と、該第1回転体の磁石表面に対向して所定の隙間を有して導体円板を配設した磁性円盤からなる第2回転体が非接触にて対向させ、該2つの回転体間の相対回転速度差に応じて生じる渦電流によって両回転体間に制動力を発生させてなる渦電流ブレーキ装置において、前記第2回転体の磁性円盤の側面に所定の高さを有する突起部を設け、且つこの突起部を覆う形態で前記導体円板を埋設したことを特徴とする渦電流ブレーキ装置。 On the side surface of the disk-shaped rotator made of a magnetic material, there is a first rotator in which N poles and S poles are alternately arranged in the rotation direction, and a predetermined gap facing the magnet surface of the first rotator. A second rotating body made of a magnetic disk provided with a conductive disk is opposed to each other in a non-contact manner, and a braking force is generated between the two rotating bodies by an eddy current generated according to a relative rotational speed difference between the two rotating bodies. In the generated eddy current brake device, a protrusion having a predetermined height is provided on a side surface of the magnetic disk of the second rotating body, and the conductor disk is embedded in a form covering the protrusion. Eddy current brake device. 前記第1回転体の磁石極数と前記第2回転体の突起部の突起数が異なる数としたことを特徴とする請求項1記載の渦電流ブレーキ装置。 2. The eddy current brake device according to claim 1, wherein the number of magnet poles of the first rotating body is different from the number of protrusions of the protrusions of the second rotating body. 前記第2回転体の前記導体円板を比抵抗値の大小に応じて簡便に取り換え可能とし、渦電流ブレーキ力を容易に調整可能としたことを特徴とする請求項1乃至請求項2に記載の渦電流ブレーキ装置。 3. The eddy current braking force can be easily adjusted by easily replacing the conductive disk of the second rotating body in accordance with the magnitude of the specific resistance value. 3. Eddy current brake device. 前記第1回転体と前記第2回転体のいずれかを固定としたことを特徴とする請求項1乃至、請求項2乃至、請求項3に記載の渦電流ブレーキ装置。 4. The eddy current brake device according to claim 1, wherein one of the first rotating body and the second rotating body is fixed. 5. 前記第1回転体の永久磁石を電磁石としたことを特徴とする請求項1乃至、請求項2乃至、請求項3乃至、請求項4に記載の渦電流装置。 5. The eddy current device according to claim 1, wherein the permanent magnet of the first rotating body is an electromagnet.
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JP7488397B1 (en) 2023-05-31 2024-05-21 株式会社京三製作所 Electric switch

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