JPH0510833U - Non-excitation actuated electromagnetic brake - Google Patents

Non-excitation actuated electromagnetic brake

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Publication number
JPH0510833U
JPH0510833U JP6450491U JP6450491U JPH0510833U JP H0510833 U JPH0510833 U JP H0510833U JP 6450491 U JP6450491 U JP 6450491U JP 6450491 U JP6450491 U JP 6450491U JP H0510833 U JPH0510833 U JP H0510833U
Authority
JP
Japan
Prior art keywords
magnetic
pole
electromagnetic brake
brake
excitation actuated
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP6450491U
Other languages
Japanese (ja)
Inventor
孝久 藤原
Original Assignee
神鋼電機株式会社
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 神鋼電機株式会社 filed Critical 神鋼電機株式会社
Priority to JP6450491U priority Critical patent/JPH0510833U/en
Publication of JPH0510833U publication Critical patent/JPH0510833U/en
Pending legal-status Critical Current

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Abstract

(57)【要約】 【目的】 ブレ−キの安定解範囲を増大させ,ブレ−キ
制動(保持)時のトルクの安定化を計るようにした無励
磁作動形電磁ブレ−キを提供すること。 【構成】 永久磁石と並列に電磁石部を構成する磁極体
と励磁コイルを配置し,この電磁石部の磁極体と空隙を
隔ててア−マチュアと,このア−マチュアを軸方向に復
帰させる復帰用のばねとを備えてなる無励磁作動形電磁
ブレ−キにおいて,上記励磁コイルによる磁束の磁気回
路を構成するインナポ−ルとアウタポ−ルの内,磁気空
隙部を隔ててアウタポ−ルと対向する部分に配置される
インナポ−ルの磁極先端部に所定の切り欠き部を形成す
るように構成した。
(57) [Abstract] [Purpose] To provide a non-excitation actuated electromagnetic brake that increases the stable solution range of the brake and stabilizes the torque during brake braking (holding). . [Composition] A permanent magnet is arranged in parallel with a magnetic pole body and an exciting coil forming an electromagnet section, an armature is separated from the magnetic pole body of the electromagnet section by a gap, and a return for returning the armature in the axial direction. In the non-excitation actuated electromagnetic brake provided with a spring, the inner pole and the outer pole forming the magnetic circuit of the magnetic flux by the exciting coil face the outer pole with a magnetic gap therebetween. A predetermined notch is formed at the tip of the magnetic pole of the inner pole arranged in that part.

Description

【考案の詳細な説明】[Detailed description of the device]

【0001】[0001]

【産業上の利用分野】[Industrial applications]

本考案は無励磁作動形電磁ブレ−キの改良に関する。   The present invention relates to improvement of a non-excitation actuated electromagnetic brake.

【0002】[0002]

【従来の技術】[Prior art]

従来のものは図4に示すように構成されていた。 同図において,1はスプラインハブ,2は軸用止め輪,3はデテントリング, 4は復帰用ばねと成るばねプレ−ト,5はア−マチュアリング,6はア−マチュ ア,7はフェ−シングである。8はコイル,9はこのコイル8への給電用のリ− ド線,10はフランジ,11は取り付けボルト,12はインナポ−ル12a,ア ウタ−ポ−ル12bから成るマグネットアッセンブリ,13は永久磁石である。 通常の状態(無通電時)では,図4に破線で示すように,ア−マチュア6とイ ンナ−ポ−ル12a及びアウタポ−ル12bに永久磁石13による磁束が形成さ れ,ア−マチュア6がマグネットアッセンブリ12のフェ−シング7に吸着して ,回転部が制動または保持される。 この状態において,コイル8に通電すると,このコイル8の通電に伴い発生す る磁束が実線で示すように生じ,上記永久磁石13による磁束を打消す。 なお,この場合の磁気吸引力は図6に示すように変化し,相殺点が磁気中心軸 となるコイル電圧VA となるため,この一点でブレ−キの解放を行うのは困難の ため,ばねプレ−ト4のばね力FB で加勢しブレ−キの解放を行うようにしてい る。具体的には,コイル8の印加電圧がVA 以上に達し,この電圧による磁束が 所定値以上になると永久磁石13による磁束がコイルによる逆方向磁束により相 殺され,ア−マチュア6及びマグネットアッセンブリ12間の磁気吸引力が消滅 し,ばねプレ−ト4のばね力によりア−マチュア6が解放される。 なお,図5は,この場合のマグネットアッセンブリ12を構成しているインナ ポ−ル12aとアウタポ−ル12b間の磁気空隙部K近傍における磁束の通過状 態を示すもので,実線は有効磁束φを,また,破線は漏洩磁束φL を示す。 図6はこの関係を示す特性図で,横軸はコイル電圧(または電流),縦軸は磁 気吸引力である。なお,同図において,Aはコイル8による磁束と永久磁石13 による磁束が完全に相殺されるコイル電圧VA を通る磁気的中心軸を,また,B はばねプレ−ト4のばね力FB を示すレベル線であり,このレベル線Bと磁気吸 引力Fの特性の交点に対応するコイル電圧V1〜V2の範囲がこの無励磁作動形ブ レ−キの安定解放範囲ということになる。The conventional one is configured as shown in FIG. In the figure, 1 is a spline hub, 2 is a retaining ring for a shaft, 3 is a detent ring, 4 is a spring plate serving as a return spring, 5 is an armature ring, 6 is an armature, and 7 is a fader. Thing. Reference numeral 8 is a coil, 9 is a lead wire for feeding power to the coil 8, 10 is a flange, 11 is a mounting bolt, 12 is a magnet assembly consisting of an inner pole 12a and an outer pole 12b, and 13 is a permanent magnet. Is. In a normal state (when no current is applied), a magnetic flux is formed by the permanent magnet 13 in the armature 6, the inner pole 12a and the outer pole 12b as shown by the broken line in FIG. The magnet 7 is attracted to the facing 7 of the magnet assembly 12, and the rotating part is braked or held. When the coil 8 is energized in this state, the magnetic flux generated by energizing the coil 8 is generated as shown by the solid line, and the magnetic flux generated by the permanent magnet 13 is canceled. Since the magnetic attraction force in this case changes as shown in FIG. 6 and the offset point becomes the coil voltage V A having the magnetic center axis, it is difficult to release the brake at this one point. The spring force F B of the spring plate 4 is urged to release the brake. Specifically, when the voltage applied to the coil 8 reaches V A or higher and the magnetic flux due to this voltage exceeds a predetermined value, the magnetic flux generated by the permanent magnet 13 is canceled by the reverse magnetic flux generated by the coil, and the armature 6 and the magnet assembly 12 are cancelled. The magnetic attraction force between them disappears, and the armature 6 is released by the spring force of the spring plate 4. In addition, FIG. 5 shows a magnetic flux passing state in the vicinity of the magnetic gap K between the inner pole 12a and the outer pole 12b constituting the magnet assembly 12 in this case, and the solid line indicates the effective magnetic flux φ, The broken line shows the leakage flux φ L. FIG. 6 is a characteristic diagram showing this relationship, where the horizontal axis is the coil voltage (or current) and the vertical axis is the magnetic attraction force. In the figure, A is the magnetic center axis passing through the coil voltage V A at which the magnetic flux from the coil 8 and the magnetic flux from the permanent magnet 13 are completely canceled, and B is the spring force F B of the spring plate 4. The range of the coil voltages V 1 to V 2 corresponding to the intersection of the characteristic of the level line B and the magnetic attraction force F is the stable release range of this non-excitation type brake.

【0003】[0003]

【考案が解決しようとする課題】[Problems to be solved by the device]

従来のものでは上記のような構成上,次のような問題点があった。 即ち,通常の場合,このブレ−キは電圧(電流)制御され,電圧をほぼ一定値 に設定して,電源スイッチをON−OFFさせることによってブレ−キの解放・ 制動(保持)をおこなっていた。 この場合,図6に示すように安定解放範囲は狭いため,電圧を解放電圧範囲内 に設定してもジュ−ル熱,雰囲気,温度等の変化によりコイル抵抗が微妙に変化 するので,設定電圧の調整が的確になされないとこの安定解放範囲を外れること が生じ,ブレ−キが正常に解放されなかったり,解放動作が不安定になったりす るという問題点があった。 このため安定解放範囲の増大とブレ−キ制動(保持)時のトルクの安定化を計 ることが要望されていた。 本考案は上記従来のものの問題点(課題)を解決するようにした無励磁作動形 ブレ−キを提供することを目的とする。   The conventional structure has the following problems due to the above structure.   That is, in the normal case, this break is voltage (current) controlled, and the voltage is kept at a substantially constant value. And release the brake by turning the power switch on and off. I was braking (holding).   In this case, as shown in Fig. 6, the stable release range is narrow, so the voltage must be within the release voltage range. Even if set to, coil resistance changes subtly due to changes in jule heat, atmosphere, temperature, etc. Therefore, if the setting voltage is not adjusted properly, the stable release range may be exceeded. Occurs, the brake may not be released normally, or the release operation may become unstable. There was a problem that   Therefore, it is necessary to increase the stable release range and stabilize the torque during brake braking (holding). Was requested.   The present invention is a non-excitation actuated type that solves the problems (problems) of the above-mentioned conventional ones. The purpose is to provide a break.

【0004】[0004]

【課題を解決するための手段】[Means for Solving the Problems]

本考案は永久磁石と並列に電磁石部を構成する磁極体と励磁コイルとを配置し ,この電磁石部の磁極体と空隙を隔ててア−マチュアと,このア−マチュアを軸 方向に復帰させる復帰用のばねとを備えてなる無励磁作動形電磁ブレ−キにおい て,上記励磁コイルによる磁束の磁気回路を構成するインナポ−ルとアウタポ− ルの内,磁気空隙部を隔ててアウタポ−ルと対向する部分に配置されるインナポ −ルの磁極先端部に所定の切り欠き部を形成するようにした無励磁作動形電磁ブ レ−キに関する。 この場合,上記切り欠き部はインナ−ポ−ルの半径方向に向かって,その先端 部が斜面を形成するように構成することが望ましい。   The present invention arranges a magnetic pole body and an exciting coil forming an electromagnet part in parallel with a permanent magnet. , The armature is separated from the magnetic pole body of the electromagnet by a gap, and the armature is A non-excitation actuated electromagnetic brake equipped with a spring for returning in the direction The inner pole and the outer pole which form the magnetic circuit of the magnetic flux by the exciting coil. Of the inner pole, which is arranged in a portion facing the outer pole across the magnetic gap. -A non-excitation actuated electromagnetic brake with a predetermined notch formed at the magnetic pole tip Regarding rake.   In this case, the above-mentioned cutout portion is directed toward the inner pole in the radial direction. It is desirable to configure the portion to form a slope.

【0005】[0005]

【作用】[Action]

本考案のものではコイルの磁束による磁気回路を構成するインナポ−ルとアウ タポ−ルの内,磁気空隙部を隔ててアウタポ−ルに対向する部分に配置される磁 極先端部に所定の切り欠き部を形成し,磁気空隙部が適正な体積となるように増 大させるようにしているから,コイル電圧が増大し,このコイルの磁束が所定量 以上に上昇しようとした場合には,磁極を早期に磁気飽和させるようにした。 この結果,ブレ−キの磁気吸引力の特性が磁気中心軸から右方は左方に比べて 勾配が小となり,復帰用のばねのばね力との右方側の交点の位置を右方に移動す る。したがって,ブレ−キの安定解放範囲は増大する。   In the present invention, the inner pole and the outer pole which form the magnetic circuit by the magnetic flux of the coil The magnets located in the part of the taper facing the outer pole across the magnetic gap. A predetermined notch is formed at the pole tip to increase the magnetic gap to an appropriate volume. Since the coil voltage is increased, the coil voltage increases and the magnetic flux of this coil is increased by a predetermined amount. When trying to rise above the above values, the magnetic poles were made to saturate magnetically at an early stage.   As a result, the characteristic of the magnetic attraction force of the brake is more rightward from the magnetic center axis than leftward. The slope becomes small, and the position of the intersection on the right side with the spring force of the return spring is moved to the right. It Therefore, the stable release range of the brake is increased.

【0006】[0006]

【実施例】【Example】

以下図1〜図3に示す一実施例により本考案を説明する。 図1において,従来例と同等の構造については,図4と同一の符号を付して示 した。 本考案のものでは,同図に示すように,コイルの磁束による磁気回路となるマ グネットアッセンブリ12を構成するインナポ−ル12aのアウタポ−ル12b との対向部に存在する磁気空隙部Kの部分を適正な体積となるように増大させる ために,インナポ−ル12aの先端の磁極部に所定形状の切り欠き部14を形成 した点にその構成上の特徴がある。 この切り欠き部14は,本実施例では,工作上,最も簡単な形状といえる半径 方向に向かってインナ−ポ−ルの先端部を斜面を形成する構成としたが,これ以 外の形状,たとえば,先端部を平坦にした略円錐状など各種変形が考えられる。 即ち,本考案では,この切り欠き部14の存在により有効磁束φが通過する磁 気回路の断面積を縮小させて有効磁束の磁束密度を増大させ,その反作用として 漏洩磁束を減少させるようにした。このため,従来のものでは図5に示すように 生じていた漏洩磁束φL を図2に示すようにφL’へと減少させて,コイルによ る磁束が,所定量を超過した場合は磁気飽和させるようにしている。 この結果,本考案の無励磁作動形ブレ−キの磁気吸引力は図3に示すように, 磁気中心軸Aより右方側(コイル電圧の大の側)を勾配の小な特性となり,ブレ −キの安定解放範囲はV1〜V3と従来のものに比べて増大した。Hereinafter, the present invention will be described with reference to an embodiment shown in FIGS. In FIG. 1, structures similar to those of the conventional example are designated by the same reference numerals as those in FIG. According to the present invention, as shown in the figure, a portion of the magnetic gap K existing in the portion of the inner assembly 12a constituting the magnet assembly 12 which forms a magnetic circuit by the magnetic flux of the coil and the outer assembly 12b is disposed. In order to increase the volume so as to be an appropriate volume, there is a structural feature in that a notch portion 14 having a predetermined shape is formed in the magnetic pole portion at the tip of the inner pole 12a. In the present embodiment, the notch portion 14 has a structure in which the tip end portion of the inner pole forms a slope toward the radial direction, which is said to be the simplest shape in machining, but other shapes, for example, Various deformations are conceivable, such as a conical shape with a flat tip. That is, in the present invention, the presence of the notch portion 14 reduces the cross-sectional area of the magnetic circuit through which the effective magnetic flux φ passes, thereby increasing the magnetic flux density of the effective magnetic flux and, as a reaction thereof, reducing the leakage magnetic flux. For this reason, the leakage flux φ L generated in the conventional one as shown in FIG. 5 is reduced to φ L 'as shown in FIG. 2, and when the magnetic flux due to the coil exceeds a predetermined amount, magnetic saturation occurs. I am trying to let you. As a result, the magnetic attraction force of the non-excitation actuated brake of the present invention has a characteristic with a small gradient on the right side (the side where the coil voltage is large) from the magnetic center axis A as shown in FIG. - stable release range of key is increased as compared with the conventional and V 1 ~V 3.

【0007】[0007]

【考案の効果】[Effect of device]

本考案のものでは,上記のようにコイルによる磁気回路構成部においてインナ ポ−ル先端の磁極部に所定の切り欠き部を形成するという簡単な構成上の改良に よって,ブレ−キの安定解放電圧範囲を増大させることができるという優れた効 果を有する。 なお,この場合,上記切り欠き部をインナ−ポ−ルの半径方向に向かって,そ の先端部が斜面を形成するように構成すれば,工作上,極めて簡単で良いので実 用的である。   According to the present invention, as described above, the inner portion of the magnetic circuit configuration section using the coil is used. For simple structural improvement by forming a predetermined notch in the magnetic pole at the tip of the pole Therefore, it has an excellent effect that the stable release voltage range of the brake can be increased. Have fruit.   In addition, in this case, the notch is directed in the radial direction of the inner pole. If the tip of the tool is constructed so as to form a slope, it is extremely easy to work and It is purposeful.

【図面の簡単な説明】[Brief description of drawings]

【図1】本考案の一実施例を示す一部を省略して描いた
半部縦断正面図である。
FIG. 1 is a partially cutaway front view showing an embodiment of the present invention with a part omitted.

【図2】本考案の要部断面図である。FIG. 2 is a cross-sectional view of an essential part of the present invention.

【図3】本考案と従来例のブレ−キの磁気吸引力を比較
して示した特性図である。
FIG. 3 is a characteristic diagram showing a comparison between the magnetic attraction force of the brake of the present invention and the magnetic attraction force of the conventional brake.

【図4】従来例の構造を示す半部縦断正面図である。FIG. 4 is a front view of a half section showing a structure of a conventional example.

【図5】従来例の要部断面図である。FIG. 5 is a sectional view of a main part of a conventional example.

【図6】従来例のブレ−キの磁気吸引力の特性図であ
る。
FIG. 6 is a characteristic diagram of a magnetic attraction force of a brake of a conventional example.

【符号の説明】[Explanation of symbols]

12:マグネットアッセンブリ 12a:インナポ−ル 12b:アウタポ−ル 14:切り欠き部 12: Magnet assembly 12a: Inner pole 12b: Outer pole 14: Notch

Claims (2)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】 永久磁石と並列に電磁石部を構成する磁
極体と励磁コイルとを配置し,この電磁石部の磁極体と
空隙を隔ててア−マチュアと,このア−マチュアを軸方
向に復帰させる復帰用ばねとを備えてなる無励磁作動形
電磁ブレ−キにおいて,上記励磁コイルによる磁束の磁
気回路を構成するインナポ−ルとアウタポ−ルの内,磁
気空隙部を隔ててアウタポ−ルと対向する部分に配置さ
れるインナポ−ルの磁極先端部に所定の切り欠き部を形
成するようにしたことを特徴とする無励磁作動形電磁ブ
レ−キ。
1. A magnetic pole body constituting an electromagnet section and an exciting coil are arranged in parallel with a permanent magnet, an armature is separated from the magnetic pole body of the electromagnet section by a gap, and the armature is returned in the axial direction. In a non-excitation actuated electromagnetic brake equipped with a return spring, the inner pole and the outer pole forming the magnetic circuit of the magnetic flux by the exciting coil are separated from the outer pole by a magnetic gap. A non-excitation actuated electromagnetic brake, characterized in that a predetermined notch is formed at the tip of the magnetic pole of the inner pole arranged at the facing portion.
【請求項2】 上記切り欠き部はインナ−ポ−ルの半径
方向に向かって,その先端部が斜面を形成するように構
成した請求項1記載の無励磁作動形電磁ブレ−キ。
2. The non-excitation actuated electromagnetic brake according to claim 1, wherein said notch portion is configured such that the tip end portion thereof forms a slope in the radial direction of the inner pole.
JP6450491U 1991-07-22 1991-07-22 Non-excitation actuated electromagnetic brake Pending JPH0510833U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6450491U JPH0510833U (en) 1991-07-22 1991-07-22 Non-excitation actuated electromagnetic brake

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6450491U JPH0510833U (en) 1991-07-22 1991-07-22 Non-excitation actuated electromagnetic brake

Publications (1)

Publication Number Publication Date
JPH0510833U true JPH0510833U (en) 1993-02-12

Family

ID=13260104

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6450491U Pending JPH0510833U (en) 1991-07-22 1991-07-22 Non-excitation actuated electromagnetic brake

Country Status (1)

Country Link
JP (1) JPH0510833U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002317838A (en) * 2001-04-20 2002-10-31 Mitsubishi Electric Corp Electromagnet and braking device using the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002317838A (en) * 2001-04-20 2002-10-31 Mitsubishi Electric Corp Electromagnet and braking device using the same
JP4588246B2 (en) * 2001-04-20 2010-11-24 三菱電機株式会社 Electromagnetic magnet and braking device using the same

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